LTC2411/LTC2411-1 24-Bit No Latency TM ADC with Differential Input and Reference in MSOP DESCRIPTIO U FEATURES 24-Bit ADC in an MS10 Package Low Supply Current (200A in Conversion Mode and 4A in Autosleep Mode) Differential Input and Differential Reference with GND to VCC Common Mode Range 2ppm INL, No Missing Codes 4ppm Full-Scale Error and 1ppm Offset 0.29ppm Noise No Latency: Digital Filter Settles in a Single Cycle. Each Conversion Is Accurate, Even After an Input Step Single Supply 2.7V to 5.5V Operation Internal Oscillator--No External Components Required 110dB Min, Pin Selectable 50Hz/60Hz Notch Filter (LTC2411) Simultaneous 50Hz/60Hz Rejection (LTC2411-1) U APPLICATIO S Direct Sensor Digitizer Weight Scales Direct Temperature Measurement Gas Analyzers Strain Gauge Transducers Instrumentation Data Acquisition Industrial Process Control 6-Digit DVMs The LTC(R)2411/LTC2411-1 are 2.7V to 5.5V micropower 24-bit differential analog-to-digital converters with an integrated oscillator, 2ppm INL and 0.29ppm RMS noise. They use delta-sigma technology and provide single cycle settling time for multiplexed applications. Through a single pin, the LTC2411 can be configured for better than 110dB differential mode rejection at 50Hz or 60Hz 2%, and the LTC2411-1 can provide better than 87dB input differential mode rejection over the range of 49Hz to 61.2Hz, or they can be driven by an external oscillator for a user-defined rejection frequency. The LTC2411 and LTC2411-1 are identical when driven by an external oscillator. The internal oscillator requires no external frequency setting components. The converters accept any external differential reference voltage from 0.1V to VCC for flexible ratiometric and remote sensing measurement configurations. The fullscale differential input range is from - 0.5VREF to 0.5VREF. The reference common mode voltage, VREFCM, and the input common mode voltage, VINCM, may be independently set anywhere within the GND to VCC range of the LTC2411/LTC2411-1. The DC common mode input rejection is better than 140dB. The LTC2411/LTC2411-1 communicate through a flexible 3-wire digital interface that is compatible with SPI and MICROWIRETM protocols. , LTC and LT are registered trademarks of Linear Technology Corporation. No Latency is a trademark of Linear Technology Corporation. MICROWIRE is a trademark of National Semiconductor Corporation. U TYPICAL APPLICATIO VCC 2.7V TO 5.5V 1F VCC 1F 1 VCC FO 10 LTC2411/ LTC2411-1 REFERENCE VOLTAGE 0.1V TO VCC 2 REF + 3 REF - ANALOG INPUT RANGE -0.5VREF TO 0.5VREF 4 IN + SDO IN - CS 5 6 SCK = INTERNAL OSC/50Hz REJECTION (LTC2411) = EXTERNAL CLOCK SOURCE = INTERNAL OSC/60Hz REJECTION (LTC2411) = SIMULTANEOUS 50Hz/60Hz REJECTION (LTC2411-1) BRIDGE IMPEDANCE 100 TO 10k 9 8 7 GND 2 3-WIRE SPI INTERFACE 4 5 IN 1 REF + VCC + IN - 3 9 SCK 8 SDO LTC2411/ LTC2411-1 7 CS REF - GND 6 3-WIRE SPI INTERFACE FO 10 2411 TA02 2411 TA01 1 LTC2411/LTC2411-1 W W W AXI U U ABSOLUTE RATI GS U U W PACKAGE/ORDER I FOR ATIO (Notes 1, 2) Supply Voltage (VCC) to GND .......................- 0.3V to 7V Analog Input Pins Voltage to GND .................................... - 0.3V to (VCC + 0.3V) Reference Input Pins Voltage to GND .................................... - 0.3V to (VCC + 0.3V) Digital Input Voltage to GND ........ - 0.3V to (VCC + 0.3V) Digital Output Voltage to GND ..... - 0.3V to (VCC + 0.3V) Operating Temperature Range LTC2411C ............................................... 0C to 70C LTC2411I ............................................ - 40C to 85C Storage Temperature Range ................. - 65C to 150C Lead Temperature (Soldering, 10 sec).................. 300C ORDER PART NUMBER LTC2411CMS LTC2411IMS LTC2411-1CMS LTC2411-1IMS TOP VIEW VCC REF + REF - IN + IN - 1 2 3 4 5 10 9 8 7 6 FO SCK SDO CS GND MS10 PART MARKING MS10 PACKAGE 10-LEAD PLASTIC MSOP LTNS LTNT LTWV LTNN TJMAX = 125C, JA = 120C/W Consult LTC Marketing for parts specified with wider operating temperature ranges. ELECTRICAL CHARACTERISTICS The denotes specifications which apply over the full operating temperature range, otherwise specifications are at TA = 25C. (Notes 3, 4) PARAMETER CONDITIONS Resolution (No Missing Codes) 0.1V VREF VCC, - 0.5 * VREF VIN 0.5 * VREF (Note 5) Integral Nonlinearity 4.5V VCC 5.5V, REF + = 2.5V, REF- = GND, VINCM = 1.25V (Note 6) 5V VCC 5.5V, REF + = 5V, REF - = GND, VINCM = 2.5V (Note 6) REF + = 2.5V, REF - = GND, VINCM = 1.25V (Note 6) Offset Error 2.5V REF + VCC, REF - = GND, GND IN + = IN - VCC (Note 14) Offset Error Drift 2.5V REF + VCC, REF - = GND, GND IN + = IN - VCC Positive Full-Scale Error 2.5V REF + VCC, REF - = GND, IN + = 0.75REF +, IN - = 0.25 * REF + Positive Full-Scale Error Drift 2.5V REF + VCC, REF - = GND, IN + = 0.75REF +, IN - = 0.25 * REF + Negative Full-Scale Error 2.5V REF + VCC, REF - = GND, IN + = 0.25 * REF +, IN - = 0.75 * REF + Negative Full-Scale Error Drift 2.5V REF + VCC, REF - = GND, IN + = 0.25 * REF+, IN - = 0.75 * REF + Total Unadjusted Error 4.5V VCC 5.5V, REF + = 2.5V, REF - = GND, VINCM = 1.25V 5V VCC 5.5V, REF + = 5V, REF- = GND, VINCM = 2.5V REF + = 2.5V, REF - = GND, VINCM = 1.25V Output Noise 5V VCC 5.5V, REF + = 5V, VREF - = GND, GND IN - = IN + 5V, (Note 13) 2 MIN TYP MAX 24 UNITS Bits 1 2 6 14 ppm of VREF ppm of VREF ppm of VREF 5 20 V 20 4 nV/C 12 0.04 4 0.04 3 3 6 1.45 ppm of VREF ppm of VREF/C 12 ppm of VREF ppm of VREF/C ppm of VREF ppm of VREF ppm of VREF VRMS LTC2411/LTC2411-1 U CO VERTER CHARACTERISTICS The denotes specifications which apply over the full operating temperature range, otherwise specifications are at TA = 25C. (Notes 3, 4) PARAMETER CONDITIONS Input Common Mode Rejection DC 2.5V REF + V - CC, REF = GND, - + IN = IN 5V MIN TYP 130 140 Input Common Mode Rejection 60Hz 2% (LTC2411) 2.5V REF+ VCC, REF - = GND, GND IN - = IN + 5V, (Note 7) 140 dB Input Common Mode Rejection 50Hz 2% (LTC2411) 2.5V REF + VCC, REF - = GND, GND IN - = IN + 5V, (Note 8) 140 dB Input Common Mode Rejection 49Hz to 61.2Hz (LTC2411-1) 2.5V < REF + < VCC, REF - = GND, GND < IN- = IN+ < VCC (Note 15) 140 dB Input Normal Mode Rejection 60Hz 2% (LTC2411) (Note 7) 110 140 dB Input Normal Mode Rejection 50Hz 2% (LTC2411) (Note 8) 110 140 dB Input Normal Mode Rejection 49Hz to 61.2Hz (LTC2411-1) (Note 15) 87 Reference Common Mode Rejection DC 2.5V REF+ VCC, GND REF - 2.5V, VREF = 2.5V, IN - = IN + = GND 130 Power Supply Rejection, DC Power Supply Rejection, 60Hz 2% (LTC2411) GND MAX UNITS dB dB 140 dB REF + = 2.5V, REF - = GND, IN - = IN + = GND 110 dB REF + = 2.5V, REF - = IN + = GND, (Note 7) 120 dB Power Supply Rejection, 50Hz 2% REF + = 2.5V, REF - = GND, IN - = IN + = GND, (Note 8) (LTC2411) 120 dB 120 dB REF + = 2.5V, REF - = GND, IN - = IN + = GND, (Note 15) U U Power Supply Rejection, 49Hz to 61.2Hz (LTC2411-1) = GND, IN - U U A ALOG I PUT A D REFERE CE The denotes specifications which apply over the full operating temperature range, otherwise specifications are at TA = 25C. (Note 3) SYMBOL PARAMETER IN + Absolute/Common Mode IN + CONDITIONS MIN Voltage GND - 0.3V VCC + 0.3V IN - Absolute/Common Mode IN - Voltage GND - 0.3V VCC + 0.3V V VIN Input Differential Voltage Range (IN + - IN -) - VREF/2 VREF/2 V REF + Absolute/Common Mode REF + Voltage 0.1 VCC V REF - Absolute/Common Mode REF - Voltage GND VCC - 0.1V V VREF Reference Differential Voltage Range (REF + - REF -) 0.1 VCC V CS (IN +) IN + Sampling Capacitance 6 pF CS (IN -) IN - Sampling Capacitance 6 pF CS (REF +) REF + Sampling Capacitance 6 pF CS (REF -) REF - Sampling Capacitance 6 pF IDC_LEAK (IN +) IN + IDC_LEAK (IN -) IN - IDC_LEAK (REF +) REF + DC Leakage Current IDC_LEAK (REF -) REF - DC Leakage Current CS = VCC = 5.5V, REF - = GND DC Leakage Current DC Leakage Current TYP MAX UNITS V CS = VCC = 5.5V, IN + = GND -10 1 10 nA CS = VCC = 5.5V, IN - = GND -10 1 10 nA CS = VCC = 5.5V, REF + -10 1 10 nA -10 1 10 nA = 5V 3 LTC2411/LTC2411-1 U U DIGITAL I PUTS A D DIGITAL OUTPUTS The denotes specifications which apply over the full operating temperature range, otherwise specifications are at TA = 25C. (Note 3) SYMBOL PARAMETER CONDITIONS VIH High Level Input Voltage CS, FO 2.7V VCC 5.5V 2.7V VCC 3.3V MIN VIL Low Level Input Voltage CS, FO 4.5V VCC 5.5V 2.7V VCC 5.5V VIH High Level Input Voltage SCK 2.7V VCC 5.5V (Note 9) 2.7V VCC 3.3V (Note 9) VIL Low Level Input Voltage SCK 4.5V VCC 5.5V (Note 9) 2.7V VCC 5.5V (Note 9) IIN Digital Input Current CS, FO 0V VIN VCC IIN Digital Input Current SCK 0V VIN VCC (Note 9) CIN Digital Input Capacitance CS, FO CIN Digital Input Capacitance SCK (Note 9) VOH High Level Output Voltage SDO IO = - 800A VOL Low Level Output Voltage SDO IO = 1.6mA VOH High Level Output Voltage SCK IO = - 800A (Note 10) VOL Low Level Output Voltage SCK IO = 1.6mA (Note 10) IOZ Hi-Z Output Leakage SDO TYP MAX UNITS 2.5 2.0 V V 0.8 0.6 V V 2.5 2.0 V V 0.8 0.6 V V -10 10 A -10 10 A 10 pF 10 pF VCC - 0.5V V 0.4 V VCC - 0.5V V -10 0.4 V 10 A U W POWER REQUIRE E TS The denotes specifications which apply over the full operating temperature range, otherwise specifications are at TA = 25C. (Note 3) SYMBOL PARAMETER VCC Supply Voltage ICC Supply Current Conversion Mode Sleep Mode Sleep Mode 4 CONDITIONS MIN CS = 0V (Note 12) CS = VCC (Note 12) CS = VCC, 2.7V VCC 3.3V (Note 12) TYP 2.7 200 4 2 MAX UNITS 5.5 V 300 10 A A A LTC2411/LTC2411-1 WU TI I G CHARACTERISTICS The denotes specifications which apply over the full operating temperature range, otherwise specifications are at TA = 25C. (Note 3) SYMBOL PARAMETER CONDITIONS MIN fEOSC External Oscillator Frequency Range tHEO External Oscillator High Period tLEO External Oscillator Low Period tCONV Conversion Time FO = 0V (LTC2411) FO = VCC (LTC2411) FO = 0V (LTC2411-1) External Oscillator (Note 11) fISCK Internal SCK Frequency Internal Oscillator (LTC2411) (Note 10) Internal Oscillator (LTC2411-1) (Note 10) External Oscillator (Notes 10, 11) DISCK Internal SCK Duty Cycle (Note 10) fESCK External SCK Frequency Range (Note 9) tLESCK External SCK Low Period (Note 9) tHESCK External SCK High Period (Note 9) 250 tDOUT_ISCK Internal SCK 32-Bit Data Output Time Internal Oscillator (LTC2411) (Notes 10, 12) Internal Oscillator (LTC2411-1) (Notes 10, 12) External Oscillator (Notes 10, 11) 1.64 1.80 tDOUT_ESCK External SCK 32-Bit Data Output Time (Note 9) t1 CS to SDO Low Z 0 200 ns t2 CS to SDO High Z 0 200 ns t3 CS to SCK (Note 10) 0 200 ns t4 CS to SCK (Note 9) 50 tKQMAX SCK to SDO Valid tKQMIN SDO Hold After SCK 15 ns t5 SCK Set-Up Before CS 50 ns t6 SCK Hold After CS MAX UNITS 2.56 2000 kHz 0.25 390 s 0.25 390 s 130.86 133.53 136.20 157.03 160.23 163.44 143.78 146.71 149.64 20510/fEOSC (in kHz) 19.2 17.5 fEOSC/8 45 Note 1: Absolute Maximum Ratings are those values beyond which the life of the device may be impaired. Note 2: All voltage values are with respect to GND. Note 3: VCC = 2.7 to 5.5V unless otherwise specified. VREF = REF + - REF -, VREFCM = (REF + + REF -)/2; VIN = IN + - IN -, VINCM = (IN + + IN -)/2. Note 4: FO pin tied to GND or to VCC or to external conversion clock source with fEOSC = 153600Hz unless otherwise specified. Note 5: Guaranteed by design, not subject to test. Note 6: Integral nonlinearity is defined as the deviation of a code from a straight line passing through the actual endpoints of the transfer curve. The deviation is measured from the center of the quantization band. Note 7: FO = 0V (internal oscillator) or fEOSC = 153600Hz 2% (external oscillator). ms ms ms ms kHz kHz kHz 55 % 2000 kHz 250 ns ns 1.67 1.70 1.83 1.86 256/fEOSC (in kHz) ms ms ms 32/fESCK (in kHz) ms ns 220 (Note 5) TYP 50 ns ns Note 8: FO = VCC (internal oscillator) or fEOSC = 128000Hz 2% (external oscillator). Note 9: The converter is in external SCK mode of operation such that the SCK pin is used as digital input. The frequency of the clock signal driving SCK during the data output is fESCK and is expressed in kHz. Note 10: The converter is in internal SCK mode of operation such that the SCK pin is used as digital output. In this mode of operation the SCK pin has a total equivalent load capacitance CLOAD = 20pF. Note 11: The external oscillator is connected to the FO pin. The external oscillator frequency, fEOSC, is expressed in kHz. Note 12: The converter uses the internal oscillator. FO = 0V or FO = VCC. Note 13: The output noise includes the contribution of the internal calibration operations. Note 14: Guaranteed by design and test correlation. Note 15: FO = 0V (internal oscillator) or fEOSC = 139800Hz 2% (external oscillator). 5 LTC2411/LTC2411-1 U W TYPICAL PERFOR A CE CHARACTERISTICS Total Unadjusted Error (VCC = 5V, VREF = 5V) Total Unadjusted Error (VCC = 5V, VREF = 2.5V) 3 1.5 2 1.0 Total Unadjusted Error (VCC = 2.7V, VREF = 2.5V) 10 1 TA = 25C 0 -2 TA = -45C TA = -45C 0 -0.5 VCC = 5V REF + = 5V REF - = GND VINCM = 2.5V FO = GND VCC = 5V REF + = 2.5V REF - = GND VINCM = 2.5V FO = GND -1.0 -3 -2.5 -2 -1.5 -1 -0.5 0 0.5 VIN (V) 1 1.5 2 2.5 -1.5 -1.25 -0.75 TA = 90C -0.25 0.25 VIN (V) 0.75 INL (ppm OF VREF) INL (ppm OF VREF) TA = 25C TA = 90C 0.5 TA = -45C 0 VCC = 5V REF + = 2.5V REF - = GND VINCM = 2.5V FO = GND -3 -2.5 -2 -1.5 -1 -0.5 0 0.5 VIN (V) -1.5 -1.25 1 1.5 2 2.5 -0.75 TA = 90C 1.25 4 2 -2 -4 -8 -0.25 0.25 VIN (V) 0.75 VCC = 2.7V REF + = 2.5V REF - = GND VINCM = 1.25V FO = GND -10 -1.25 1.25 - 0.75 TA = -45C TA = 25C 0.25 - 0.25 VIN (V) 0.75 RMS Noise vs Input Differential Voltage Long Term ADC Readings 1.0 ADC READING (ppm OF VREF) GAUSSIAN DISTRIBUTION m = -0.647ppm = 0.287ppm 0.5 0 -0.5 6 -1.0 4 -1.5 2 -2.0 1 2411 G07 0.5 VCC = 5V, VREF = 5V, VIN = 0V, VINCM = 2.5V, FO = GND, TA = 25C, RMS NOISE = 0.29ppm RMS NOISE (ppm OF VREF) 16 0 1.25 2411 G06 2411 G01 Noise Histogram 0 0.5 -0.5 OUTPUT CODE (ppm OF VREF) TA = 90C 0 -6 2411 G04 NUMBER OF READINGS (%) 0.75 6 -1.0 6 0.25 - 0.25 VIN (V) Integral Nonlinearity (VCC = 2.7V, VREF = 2.5V) TA = 25C -2 -1.0 TA = 25C 10 -0.5 -1.5 - 0.75 TA = -45C 8 -1 0 -2.0 VCC = 2.7V REF + = 2.5V REF - = GND VINCM = 1.25V FO = GND 2411 G03 1.0 TA = -45C 10,000 CONSECUTIVE READINGS 14 VCC = 5V = 5V V 12 REF VIN = 0V = 2.5V V 10 INCM FO = GND TA = 25C 8 -4 -10 -1.25 1.25 1.5 0 -2 Integral Nonlinearity (VCC = 5V, VREF = 2.5V) 3 1 TA = 90C 0 2411 G02 Integral Nonlinearity (VCC = 5V, VREF = 5V) 2 2 -8 2411 G01 VCC = 5V REF + = 5V REF - = GND VINCM = 2.5V FO = GND 4 -6 INL (ppm OF VREF) -1 TA = 25C 0.5 TUE (ppm OF VREF) 6 TA = 90C TUE (ppm OF VREF) TUE (ppm OF VREF) 8 5 10 15 20 25 30 35 40 45 50 55 60 TIME (HOURS) 2411 G08 0.4 0.3 0.2 0.1 TA = 25C VCC = 5V VREF = 5V VINCM = 2.5V FO = GND 0 -2.5 -2 -1.5 -1 -0.5 0 0.5 1 1.5 2 INPUT DIFFERENTIAL VOLTAGE (V) 2.5 2411 G09 LTC2411/LTC2411-1 U W TYPICAL PERFOR A CE CHARACTERISTICS RMS Noise vs Temperature 1.60 VCC = 5V VIN = 0V REF + = 5V FO = GND - REF = GND TA = 25C VCC = 5V VREF = 5V VIN = 0V VINCM = GND FO = GND 1.55 1.50 RMS NOISE (V) RMS NOISE (V) 1.55 1.45 1.40 1.50 1.55 1.45 1.40 1.35 1.35 1.30 -1 0 1 3 2 VINCM (V) 5 4 1.30 -45 -30 -15 6 0 15 30 45 60 TEMPERATURE (C) 75 1.35 1.30 VCC = 5V REF + = 5V REF - = GND VIN = 0V FO = GND TA = 25C -0.2 -0.3 -0.4 -0.1 -0.5 -0.6 -0.7 -0.8 3 VREF (V) -1 0 1 2 3 VINCM (V) 5 4 2411 G13 0.6 0.4 0.2 6 0 -0.4 -0.6 -0.8 -1.0 0.6 0.4 0.2 0 -0.2 -0.4 -0.6 -1.0 3.5 -0.6 -0.7 -0.8 -1.0 -45 -30 -15 3.9 4.3 VCC (V) 4.7 5.1 5.5 2411 G16 0 15 30 45 60 TEMPERATURE (C) 0 1 3 2 VREF (V) 90 75 2411 G15 + Full-Scale Error vs Temperature -0.8 3.1 -0.5 3 VCC = 5V REF- = GND VIN = 0V VINCM = GND FO = GND TA = 25C 0.8 -0.2 5.5 -0.4 Offset Error vs VREF REF + = 2.5V REF - = GND VIN = 0V VINCM = GND FO = GND TA = 25C 2.7 -0.3 0 OFFSET ERROR (ppm OF VREF) OFFSET ERROR (ppm OF VREF) 0.8 5.1 VCC = 5V VREF = 5V VIN = 0V VINCM = GND FO = GND 2411 G14 Offset Error vs VCC 0 4.7 -0.9 -1.0 5 4 -0.2 FULL-SCALE ERROR (ppm OF VREF) 2 3.9 4.3 VCC (V) Offset Error vs Temperature -0.9 1 3.5 2411 G12 OFFSET ERROR (ppm OF VREF) 1.40 3.1 0 -0.1 1.45 0 1.30 2.7 90 Offset Error vs VINCM OFFSET ERROR (ppm OF VREF) 1.50 1.40 0 VCC = 5V REF - = GND VIN = 0V FO = GND TA = 25C 1.55 1.45 2411 G11 RMS Noise vs VREF 1.60 1.50 REF + = 2.5V REF - = GND VIN = 0V FO = GND TA = 25C 1.35 2411 G10 RMS NOISE (V) RMS Noise vs VCC 1.60 RMS NOISE (V) RMS Noise vs VINCM 1.60 4 5 2411 G17 2 1 VCC = 5V REF + = 5V REF - = GND IN+ = 2.5V IN - = GND FO = GND 0 -1 -2 -3 -45 -30 -15 0 15 30 45 60 TEMPERATURE (C) 75 90 2411 G18 7 LTC2411/LTC2411-1 U W TYPICAL PERFOR A CE CHARACTERISTICS + Full-Scale Error vs Temperature -Full-Scale Error vs Temperature 2 1 0 -1 -2 -3 -4 -5 -45 -30 -15 0 15 30 45 60 TEMPERATURE (C) 75 90 2 1 0 VCC = 5V REF + = 5V REF - = GND + -2 IN - = GND IN = 2.5V FO = GND -3 -45 -30 -15 0 15 30 45 60 TEMPERATURE (C) -1 2411 G19 -40 -80 1 0 -1 -2 -3 -4 0 -60 -20 -40 -80 -60 -120 -120 -120 -140 10k 100k 1k 100 FREQUENCY AT VCC (Hz) 0 1M 30 0 0 REJECTION (dB) REJECTION (dB) VCC = 4.1V DC 1.4V REF + = 2.5V -20 REF - = GND IN + = GND -40 IN - = GND FO = GND -60 TA = 25C -80 VCC = 4.1V DC 0.7V REF + = 2.5V -20 REF - = GND IN + = GND -40 IN - = GND FO = GND -60 TA = 25C -80 -100 -100 -100 -120 -120 -120 -140 -140 1 10 10k 100k 1k 100 FREQUECY AT VCC (Hz) 1M 2411 G31 8 7800 PSRR vs Frequency at VCC (LTC2411-1) 0 -80 7700 7750 FREQUENCY AT VCC (Hz) 2411 G24 PSRR vs Frequency at VCC (LTC2411-1) VCC = 4.1V DC REF + = 2.5V -20 REF - = GND IN + = GND -40 IN - = GND FO = GND -60 TA = 25C 7650 2411 G23 PSRR vs Frequency at VCC (LTC2411-1) 90 VCC = 4.1V DC 0.7VP-P REF + = 2.5V REF - = GND IN + = GND IN - = GND FO = GND TA = 25C -140 7600 60 90 120 150 180 210 240 FREQUENCY AT VCC (Hz) 2411 G22 75 -80 -100 10 0 15 30 45 60 TEMPERATURE (C) PSRR vs Frequency at VCC (LTC2411) -100 1 VCC = 2.7V REF + = 2.5V REF - = GND IN + = GND IN - = 1.25V FO = GND 2411 G21 -100 -140 REJECTION (dB) 2 -5 -45 -30 -15 90 VCC = 4.1V DC 1.4V REF + = 2.5V REF - = GND IN + = GND IN - = GND FO = GND TA = 25C -20 REJECTION (dB) REJECTION (dB) 0 VCC = 4.1V DC REF + = 2.5V REF - = GND IN + = GND IN - = GND FO = GND TA = 25C -60 3 PSRR vs Frequency at VCC (LTC2411) 0 -40 4 2411 G20 PSRR vs Frequency at VCC (LTC2411) -20 75 REJECTION (dB) 3 -FULL-SCALE ERROR (ppm OF VREF) VCC = 2.7V REF + = 2.5V REF - = GND IN + = 1.25V IN - = GND FO = GND 4 -Full-Scale Error vs Temperature 5 3 -FULL-SCALE ERROR (ppm OF VREF) FULL-SCALE ERROR (ppm OF VREF) 5 0 20 40 60 80 100 120 140 160 180 200 220 FREQUENCY AT VCC (Hz) 2411 G32 -140 6880 6930 6980 7030 FREQUENCY AT VCC (Hz) 7080 2411 G33 LTC2411/LTC2411-1 U W TYPICAL PERFOR A CE CHARACTERISTICS Conversion Current vs Temperature 650 VCC = 5.5V SUPPLY CURRENT (A) 210 VCC = 5V 200 190 VCC = 3V 180 REF + = VCC 600 REF - = GND IN + = GND 550 IN - = GND 500 TA = 25C SCK = NC 450 SDO = NC CS = GND 400 FO = EXT OSC 350 300 75 150 90 0 10 20 30 40 50 60 70 80 90 100 OUTPUT DATA RATE (READINGS/SEC) VCC = 3V -20 VREF = 5V -40 VCC = 5V REF - = GND VINCM = 2.5V VIN = 0V FO = EXT OSC TA = 25C 10 20 30 40 50 60 70 80 90 100 OUTPUT DATA RATE (READINGS/SEC) 0 15 30 45 60 TEMPERATURE (C) 90 Resolution (INLMAX 1LSB) vs Output Data Rate 20 VREF = 2.5V 20 VCC = 5V REF - = GND VINCM = 2.5V 19 VIN = 0V FO = EXT OSC RES = LOG2(VREF/NOISERMS) TA = 25C 18 0 10 20 30 40 50 60 70 80 90 100 OUTPUT DATA RATE (READINGS/SEC) 2411 G28 75 22 21 RESOLUTION (BITS) OFFSET ERROR (ppm OF VREF) VREF = 2.5V 0 1 2411 G27 VREF = 5V 0 -120 VCC = 5V 0 -45 -30 -15 22 -100 2 Resolution (NOISERMS 1LSB) vs Output Data Rate 40 -80 VCC = 5.5V 3 2411 G26 Offset Error vs Output Data Rate -60 4 VCC = 2.7V 2411 G25 20 FO = GND CS = VCC SCK = NC SDO = NC 200 VCC = 2.7V 0 15 30 45 60 TEMPERATURE (C) VCC = 5V VCC = 3V 250 170 5 2411 G29 RESOLUTION (BITS) CONVERSION CURRENT (A) FO = GND 230 CS = GND SCK = NC 220 SDO = NC SLEEP MODE CURRENT (A) 240 160 -45 -30 -15 Sleep Mode Current vs Temperature Conversion Current vs Output Data Rate 18 VREF = 5V 16 VCC = 5V VREF = 2.5V REF - = GND VINCM = 2.5V VIN = 0V FO = EXT OSC RES = LOG2(VREF/INLMAX) TA = 25C 14 12 10 0 10 20 30 40 50 60 70 80 90 100 OUTPUT DATA RATE (READINGS/SEC) 2411 G30 U U U PI FU CTIO S VCC (Pin 1): Positive Supply Voltage. Bypass to GND (Pin 6) with a 10F tantalum capacitor in parallel with 0.1F ceramic capacitor as close to the part as possible. REF + (Pin 2), REF - (Pin 3): Differential Reference Input. The voltage on these pins can have any value between GND and VCC as long as the reference positive input, REF +, is more positive than the reference negative input, REF -, by at least 0.1V. IN + (Pin 4), IN- (Pin 5): Differential Analog Input. The voltage on these pins can have any value between GND - 0.3V and VCC + 0.3V. Within these limits, the converter bipolar input range (VIN = IN+ - IN-) extends from - 0.5 * (VREF ) to 0.5 * (VREF ). Outside this input range, the converter produces unique overrange and underrange output codes. GND (Pin 6): Ground. Connect this pin to a ground plane through a low impedance connection. CS (Pin 7): Active LOW Digital Input. A LOW on this pin enables the SDO digital output and wakes up the ADC. Following each conversion the ADC automatically enters 9 LTC2411/LTC2411-1 U U U PI FU CTIO S the Sleep mode and remains in this low power state as long as CS is HIGH. A LOW-to-HIGH transition on CS during the Data Output transfer aborts the data transfer and starts a new conversion. internal pull-up is automatically activated in Internal Serial Clock Operation mode. The Serial Clock Operation mode is determined by the logic level applied to the SCK pin at power up or during the most recent falling edge of CS. SDO (Pin 8): Three-State Digital Output. During the Data Output period, this pin is used as the serial data output. When the chip select CS is HIGH (CS = VCC), the SDO pin is in a high impedance state. During the Conversion and Sleep periods, this pin is used as the conversion status output. The conversion status can be observed by pulling CS LOW. FO (Pin 10): Frequency Control Pin. Digital input that controls the ADC's notch frequencies and conversion time. For the LTC2411, when the FO pin is connected to VCC (FO = VCC), the converter uses its internal oscillator and the digital filter first null is located at 50Hz. When the FO pin is connected to GND (FO = OV), the converter uses its internal oscillator and the digital filter first null is located at 60Hz. For the LTC2411-1, the converter provides simultaneous 50Hz/60Hz rejection with the FO pin connected to GND. When FO is driven by an external clock signal with a frequency fEOSC, the converters use this signal as their system clock and the digital filter first null is located at a frequency fEOSC/2560. SCK (Pin 9): Bidirectional Digital Clock Pin. In Internal Serial Clock Operation mode, SCK is used as the digital output for the internal serial interface clock during the Data Output period. In External Serial Clock Operation mode, SCK is used as the digital input for the external serial interface clock during the Data Output period. A weak W FU CTIO AL BLOCK DIAGRA U INTERNAL OSCILLATOR U VCC GND IN + IN - AUTOCALIBRATION AND CONTROL + - FO (INT/EXT) SDO SERIAL INTERFACE ADC SCK CS + REF REF - DECIMATING FIR - + DAC 2411 FD Figure 1 VCC TEST CIRCUITS 1.69k SDO SDO 1.69k CLOAD = 20pF 2411 TA03 Hi-Z TO VOH VOL TO VOH VOH TO Hi-Z 10 CLOAD = 20pF 2411 TA04 Hi-Z TO VOL VOH TO VOL VOL TO Hi-Z LTC2411/LTC2411-1 U W U U APPLICATIO S I FOR ATIO CONVERTER OPERATION Converter Operation Cycle The LTC2411/LTC2411-1 are low power, delta-sigma analog-to-digital converters with an easy-to-use 3-wire serial interface (see Figure 1). Their operation is made up of three states. The converter operating cycle begins with the conversion, followed by the low power sleep state and ends with the data output (see Figure 2). The 3-wire interface consists of serial data output (SDO), serial clock (SCK) and chip select (CS). Initially, the LTC2411/LTC2411-1 perform a conversion. Once the conversion is complete, the devices enter the sleep state. While in this sleep state, power consumption is reduced by an order of magnitude. The parts remain in the sleep state as long as CS is HIGH. The conversion result is held indefinitely in a static shift register while the converter is in the sleep state. Once CS is pulled LOW, the devices begin outputting the conversion result. There is no latency in the conversion result. The data output corresponds to the conversion just performed. This result is shifted out on the serial data out pin (SDO) under the control of the serial clock (SCK). Data is updated on the falling edge of SCK allowing the user to reliably latch data on the rising edge of SCK (see Figure 3). The data output state is concluded once 32 bits are read out of the ADC or when CS is brought HIGH. The devices automatically initiate a new conversion and the cycle repeats. Through timing control of the CS and SCK pins, the LTC2411/LTC2411-1 offer several flexible modes of operation (internal or external SCK and free-running conversion modes). These various modes do not require programming configuration registers; moreover, they do not disturb the cyclic operation described above. These modes of operation are described in detail in the Serial Interface Timing Modes section. Conversion Clock A major advantage the delta-sigma converter offers over conventional type converters is an on-chip digital filter (commonly implemented as a Sinc or Comb filter). For high resolution, low frequency applications, this filter is typically designed to reject line frequencies of 50 or 60Hz plus their harmonics. The filter rejection performance is directly related to the accuracy of the converter system clock. The LTC2411/LTC2411-1 incorporate a highly accurate on-chip oscillator. This eliminates the need for external frequency setting components such as crystals or oscillators. Clocked by the on-chip oscillator, the LTC2411 achieves a minimum of 110dB rejection at the line frequency (50Hz or 60Hz 2%) and the LTC2411-1 achieves a minimum of 87dB rejection over 49Hz to 61.2Hz. Ease of Use The LTC2411/LTC2411-1 data output has no latency, filter settling delay or redundant data associated with the conversion cycle. There is a one-to-one correspondence between the conversion and the output data. Therefore, multiplexing multiple analog voltages is easy. CONVERT SLEEP FALSE CS = LOW AND SCK TRUE The LTC2411/LTC2411-1 perform offset and full-scale calibrations in every conversion cycle. This calibration is transparent to the user and has no effect on the cyclic operation described above. The advantage of continuous calibration is extreme stability of offset and full-scale readings with respect to time, supply voltage change and temperature drift. Power-Up Sequence DATA OUTPUT 2411 F02 Figure 2. LTC2411/LTC2411-1 State Transition Diagram The LTC2411/LTC2411-1 automatically enter an internal reset state when the power supply voltage VCC drops below approximately 1.9V. This feature guarantees the 11 LTC2411/LTC2411-1 U W U U APPLICATIO S I FOR ATIO integrity of the conversion result and of the serial interface mode selection. (See the 2-wire I/O sections in the Serial Interface Timing Modes section.) When the VCC voltage rises above this critical threshold, the converter creates an internal power-on-reset (POR) signal with a duration of approximately 1ms. The POR signal clears all internal registers. Following the POR signal, the LTC2411/LTC2411-1 start a normal conversion cycle and follow the succession of states described above. The first conversion result following POR is accurate within the specifications of the device if the power supply voltage is restored within the operating range (2.7V to 5.5V) before the end of the POR time interval. Reference Voltage Range The LTC2411/LTC2411-1 accept a truly differential external reference voltage. The absolute/common mode voltage specification for the REF + and REF - pins covers the entire range from GND to VCC. For correct converter operation, the REF + pin must always be more positive than the REF - pin. The LTC2411/LTC2411-1 can accept a differential reference voltage from 0.1V to VCC. The converter output noise is determined by the thermal noise of the front-end circuits, and, as such, its value in nanovolts is nearly constant with reference voltage. A decrease in reference voltage will not significantly improve the converter's effective resolution. On the other hand, a reduced reference voltage will improve the converter's overall INL performance. A reduced reference voltage will also improve the converter performance when operated with an external conversion clock (external FO signal) at substantially higher output data rates. Input Voltage Range The analog input is truly differential with an absolute/ common mode range for the IN+ and IN- input pins extending from GND - 0.3V to VCC + 0.3V. Outside these limits, the ESD protection devices begin to turn on and the errors due to input leakage current increase rapidly. Within these limits, the LTC2411/LTC2411-1 convert the bipolar differential input signal, VIN = IN + - IN -, from - FS = - 0.5 * VREF to +FS = 0.5 * VREF where VREF = REF+ - REF -. Outside this range the converter indicates 12 the overrange or the underrange condition using distinct output codes. Input signals applied to IN+ and IN- pins may extend by 300mV below ground and above VCC. In order to limit any fault current, resistors of up to 5k may be added in series with the IN+ and IN- pins without affecting the performance of the device. In the physical layout, it is important to maintain the parasitic capacitance of the connection between these series resistors and the corresponding pins as low as possible; therefore, the resistors should be located as close as practical to the pins. In addition, series resistors will introduce a temperature dependent offset error due to the input leakage current. A 1nA input leakage current will develop a 1ppm offset error on a 5k resistor if VREF = 5V. This error has a very strong temperature dependency. Output Data Format The LTC2411/LTC2411-1 serial output data stream is 32 bits long. The first 3 bits represent status information indicating the sign and conversion state. The next 24 bits are the conversion result, MSB first. The remaining 5 bits are sub LSBs beyond the 24-bit level that may be included in averaging or discarded without loss of resolution. The third and fourth bits together are also used to indicate an underrange condition (the differential input voltage is below - FS) or an overrange condition (the differential input voltage is above + FS). Bit 31 (first output bit) is the end of conversion (EOC) indicator. This bit is available at the SDO pin during the conversion and sleep states whenever the CS pin is LOW. This bit is HIGH during the conversion and goes LOW when the conversion is complete. Bit 30 (second output bit) is a dummy bit (DMY) and is always LOW. Bit 29 (third output bit) is the conversion result sign indicator (SIG). If VIN is >0, this bit is HIGH. If VIN is <0, this bit is LOW. Bit 28 (fourth output bit) is the most significant bit (MSB) of the result. This bit in conjunction with Bit 29 also provides the underrange or overrange indication. If both Bit 29 and Bit 28 are HIGH, the differential input voltage is LTC2411/LTC2411-1 U W U U APPLICATIO S I FOR ATIO above +FS. If both Bit 29 and Bit 28 are LOW, the differential input voltage is below -FS. The function of these bits is summarized in Table 1. Table 1. LTC2411/LTC2411-1 Status Bits Bit 31 Bit 30 Bit 29 Bit 28 EOC DMY SIG MSB Input Range VIN 0.5 * VREF 0 0 1 1 0V VIN < 0.5 * VREF 0 0 1 0 -0.5 * VREF VIN < 0V 0 0 0 1 VIN < - 0.5 * VREF 0 0 0 0 Bits 28-5 are the 24-bit conversion result MSB first. Bit 5 is the least significant bit (LSB). Bits 4-0 are sub LSBs below the 24-bit level. Bits 4-0 may be included in averaging or discarded without loss of resolution. Data is shifted out of the SDO pin under control of the serial clock (SCK), see Figure 3. Whenever CS is HIGH, SDO remains high impedance and any externally generated SCK clock pulses are ignored by the internal data out shift register. In order to shift the conversion result out of the device, CS must first be driven LOW. EOC is seen at the SDO pin of the device once CS is pulled LOW. EOC changes real time from HIGH to LOW at the completion of a conversion. This signal may be used as an interrupt for an external microcontroller. Bit 31 (EOC) can be captured on the first rising edge of SCK. Bit 30 is shifted out of the device on the first falling edge of SCK. The final data bit (Bit 0) is shifted out on the falling edge of the 31st SCK and may be latched on the rising edge of the 32nd SCK pulse. On the falling edge of the 32nd SCK pulse, SDO goes HIGH indicating the initiation of a new conversion cycle. This bit serves as EOC (Bit 31) for the next conversion cycle. Table 2 summarizes the output data format. CS SDO BIT 31 BIT 30 BIT 29 BIT 28 EOC "0" SIG MSB BIT 27 BIT 5 BIT 0 LSB24 Hi-Z SCK 1 2 3 4 SLEEP 5 26 27 32 DATA OUTPUT CONVERSION 2411 F03 Figure 3. Output Data Timing Table 2. LTC2411/LTC2411-1 Output Data Format Differential Input Voltage VIN * Bit 31 EOC Bit 30 DMY Bit 29 SIG Bit 28 MSB Bit 27 Bit 26 Bit 25 ... Bit 0 VIN* 0.5 * VREF** 0 0 1 1 0 0 0 ... 0 0.5 * VREF** - 1LSB 0 0 1 0 1 1 1 ... 1 0.25 * VREF** 0 0 1 0 1 0 0 ... 0 0.25 * VREF** - 1LSB 0 0 1 0 0 1 1 ... 1 0 0 0 1 0 0 0 0 ... 0 -1LSB 0 0 0 1 1 1 1 ... 1 - 0.25 * VREF** 0 0 0 1 1 0 0 ... 0 - 0.25 * VREF** - 1LSB 0 0 0 1 0 1 1 ... 1 - 0.5 * VREF** 0 0 0 1 0 0 0 ... 0 VIN* < -0.5 * VREF** 0 0 0 0 1 1 1 ... 1 *The differential input voltage VIN = IN+ - IN-. **The differential reference voltage VREF = REF+ - REF-. 13 LTC2411/LTC2411-1 U W U U APPLICATIO S I FOR ATIO Frequency Rejection Selection (FO) (LTC2411 Only) The LTC2411 internal oscillator provides better than 110dB normal mode rejection at the line frequency and all its harmonics for 50Hz 2% or 60Hz 2%. For 60Hz rejection, FO should be connected to GND while for 50Hz rejection the FO pin should be connected to VCC. The selection of 50Hz or 60Hz rejection can also be made by driving FO to an appropriate logic level. A selection change during the sleep or data output states will not disturb the converter operation. If the selection is made during the conversion state, the result of the conversion in progress may be outside specifications but the following conversions will not be affected. When a fundamental rejection frequency different from 50Hz or 60Hz is required or when the converter must be synchronized with an outside source, the LTC2411 can operate with an external conversion clock. The converter automatically detects the presence of an external clock signal at the FO pin and turns off the internal oscillator. The frequency fEOSC of the external signal must be at least 2560Hz (1Hz notch frequency) to be detected. The external clock signal duty cycle is not significant as long as the minimum and maximum specifications for the high and low periods tHEO and tLEO are observed. While operating with an external conversion clock of a frequency fEOSC, the LTC2411 provides better than 110dB normal mode rejection in a frequency range fEOSC/2560 4% and its harmonics. The normal mode rejection as a function of the input frequency deviation from fEOSC/2560 is shown in Figure 4. Whenever an external clock is not present at the FO pin, the converter automatically activates its internal oscillator and 14 -80 -85 NORMAL MODE REJECTION (dB) As long as the voltage on the IN+ and IN- pins is maintained within the - 0.3V to (VCC + 0.3V) absolute maximum operating range, a conversion result is generated for any differential input voltage VIN from -FS = -0.5 * VREF to +FS = 0.5 * VREF. For differential input voltages greater than +FS, the conversion result is clamped to the value corresponding to the +FS + 1LSB. For differential input voltages below -FS, the conversion result is clamped to the value corresponding to -FS - 1LSB. -90 -95 -100 -105 -110 -115 -120 -125 -130 -135 -140 -12 -8 -4 0 4 8 12 DIFFERENTIAL INPUT SIGNAL FREQUENCY DEVIATION FROM NOTCH FREQUENCY fEOSC/2560(%) 2411 F04 Figure 4. LTC2411 Normal Mode Rejection When Using an External Oscillator of Frequency fEOSC enters the Internal Conversion Clock mode. The LTC2411 operation will not be disturbed if the change of conversion clock source occurs during the sleep state or during the data output state while the converter uses an external serial clock. If the change occurs during the conversion state, the result of the conversion in progress may be outside specifications but the following conversions will not be affected. If the change occurs during the data output state and the converter is in the Internal SCK mode, the serial clock duty cycle may be affected but the serial data stream will remain valid. Table 3 summarizes the duration of each state and the achievable output data rate as a function of FO. Simultaneous Frequency Rejection (LTC2411-1 Only) The LTC2411-1 internal oscillator provides better than 87dB normal mode rejection over the range of 49Hz to 61.2Hz. For this simultaneous 50/60Hz rejection, FO should be connected to GND. The performance of the LTC2411-1 is the same as the LTC2411 when driven by an external conversion clock at FO pin. SERIAL INTERFACE PINS The LTC2411/LTC2411-1 transmit the conversion results and receive the start of conversion command through a synchronous 3-wire interface. During the conversion and sleep states, this interface can be used to assess the LTC2411/LTC2411-1 U W U U APPLICATIO S I FOR ATIO Table 3. LTC2411/LTC2411-1 State Duration State Operating Mode CONVERT Internal Oscillator Duration FO = LOW (LTC2411) (60Hz Rejection) 133ms, Output Data Rate 7.5 Readings/s FO = HIGH (LTC2411) (50Hz Rejection) 160ms, Output Data Rate 6.2 Readings/s FO = LOW (LTC2411-1) (Simultaneous 50Hz/60Hz Rejection) 147ms, Output Data Rate 6.8 Readings/s External Oscillator FO = External Oscillator with Frequency fEOSC kHz (fEOSC/2560 Rejection) 20510/fEOSCs, Output Data Rate fEOSC/20510 Readings/s Internal Serial Clock FO = LOW/HIGH (LTC2411) (Internal Oscillator) As Long As CS = LOW But Not Longer Than 1.67ms (32 SCK cycles) FO = LOW (LTC2411-1) (Internal Oscillator) As Long As CS = LOW But Not Longer Than 1.83ms (32 SCK cycles) FO = External Oscillator with Frequency fEOSC kHz As Long As CS = LOW But Not Longer Than 256/fEOSCms (32 SCK cycles) SLEEP DATA OUTPUT As Long As CS = HIGH Until CS = LOW and SCK External Serial Clock with Frequency fSCK kHz As Long As CS = LOW But Not Longer Than 32/fSCKms (32 SCK cycles) converter status and during the data output state it is used to read the conversion result. used as an end of conversion indicator during the conversion and sleep states. Serial Clock Input/Output (SCK) When CS (Pin 7) is HIGH, the SDO driver is switched to a high impedance state. This allows sharing the serial interface with other devices. If CS is LOW during the convert or sleep state, SDO will output EOC. If CS is LOW during the conversion phase, the EOC bit appears HIGH on the SDO pin. Once the conversion is complete, EOC goes LOW. The device remains in the sleep state until the first rising edge of SCK occurs while CS = LOW. The serial clock signal present on SCK (Pin 9) is used to synchronize the data transfer. Each bit of data is shifted out the SDO pin on the falling edge of the serial clock. In the Internal SCK mode of operation, the SCK pin is an output and the LTC2411/LTC2411-1 create their own serial clock by dividing the internal conversion clock by 8. In the External SCK mode of operation, the SCK pin is used as input. The internal or external SCK mode is selected on power-up and then reselected every time a HIGH-to-LOW transition is detected at the CS pin. If SCK is HIGH or floating at power-up or during this transition, the converter enters the internal SCK mode. If SCK is LOW at power-up or during this transition, the converter enters the external SCK mode. Serial Data Output (SDO) The serial data output pin, SDO (Pin 8), provides the result of the last conversion as a serial bit stream (MSB first) during the data output state. In addition, the SDO pin is Chip Select Input (CS) The active LOW chip select, CS (Pin 7), is used to test the conversion status and to enable the data output transfer as described in the previous sections. In addition, the CS signal can be used to trigger a new conversion cycle before the entire serial data transfer has been completed. The LTC2411/LTC2411-1 will abort any serial data transfer in progress and start a new conversion cycle anytime a LOW-to-HIGH transition is detected at the CS pin after the converter has entered the data output state (i.e., after the first rising edge of SCK occurs with CS = LOW). 15 LTC2411/LTC2411-1 U W U U APPLICATIO S I FOR ATIO Table 4. LTC2411/LTC2411-1 Interface Timing Modes SCK Source Conversion Cycle Control Data Output Control Connection and Waveforms External SCK, Single Cycle Conversion External CS and SCK CS and SCK Figures 5, 6 External SCK, 2-Wire I/O External SCK SCK Figure 7 Internal SCK, Single Cycle Conversion Internal CS CS Figures 8, 9 Internal SCK, 2-Wire I/O, Continuous Conversion Internal Continuous Internal Figure 10 Configuration 2.7V TO 5.5V VCC 1F 1 VCC FO = 50Hz REJECTION (LTC2411) = EXTERNAL OSCILLATOR = 60Hz REJECTION (LTC2411) = SIMULTANEOUS 50Hz/60Hz REJECTION (LTC2411-1) 10 LTC2411/ LTC2411-1 REFERENCE VOLTAGE 0.1V TO VCC 2 REF + 3 REF - ANALOG INPUT RANGE -0.5VREF TO 0.5VREF 4 IN + SDO 5 IN - CS 6 SCK 9 3-WIRE SPI INTERFACE 8 7 GND CS TEST EOC TEST EOC SDO BIT 31 EOC Hi-Z BIT 30 BIT 29 BIT 28 SIG MSB BIT 27 BIT 26 BIT 5 BIT 0 LSB SUB LSB TEST EOC Hi-Z Hi-Z SCK (EXTERNAL) CONVERSION SLEEP DATA OUTPUT CONVERSION 2411 F05 Figure 5. External Serial Clock, Single Cycle Operation Finally, CS can be used to control the free-running modes of operation, see Serial Interface Timing Modes section. Grounding CS will force the ADC to continuously convert at the maximum output rate selected by FO. SERIAL INTERFACE TIMING MODES The LTC2411/LTC2411-1's 3-wire interface is SPI and MICROWIRE compatible. This interface offers several flexible modes of operation. These include internal/external serial clock, 2- or 3-wire I/O, single cycle conversion. The following sections describe each of these serial interface timing modes in detail. In all these cases, the converter can use the internal oscillator (FO = LOW or FO = HIGH) or an external oscillator connected to the FO pin. Refer to Table 4 for a summary. 16 External Serial Clock, Single Cycle Operation (SPI/MICROWIRE Compatible) This timing mode uses an external serial clock to shift out the conversion result and a CS signal to monitor and control the state of the conversion cycle, see Figure 5. The serial clock mode is selected on the falling edge of CS. To select the external serial clock mode, the serial clock pin (SCK) must be LOW during each CS falling edge. The serial data output pin (SDO) is Hi-Z as long as CS is HIGH. At any time during the conversion cycle, CS may be pulled LOW in order to monitor the state of the converter. While CS is pulled LOW, EOC is output to the SDO pin. EOC = 1 while a conversion is in progress and EOC = 0 if the device is in the sleep state. Independent of CS, the LTC2411/LTC2411-1 U W U U APPLICATIO S I FOR ATIO device automatically enters the low power sleep state once the conversion is complete. requiring all 32 bits of output data, aborting an invalid conversion cycle or synchronizing the start of a conversion. When the device is in the sleep state (EOC = 0), its conversion result is held in an internal static shift register. The device remains in the sleep state until the first rising edge of SCK is seen while CS is LOW. Data is shifted out the SDO pin on each falling edge of SCK. This enables external circuitry to latch the output on the rising edge of SCK. EOC can be latched on the first rising edge of SCK and the last bit of the conversion result can be latched on the 32nd rising edge of SCK. On the 32nd falling edge of SCK, the device begins a new conversion. SDO goes HIGH (EOC = 1) indicating a conversion is in progress. External Serial Clock, 2-Wire I/O At the conclusion of the data cycle, CS may remain LOW and EOC monitored as an end-of-conversion interrupt. Alternatively, CS may be driven HIGH setting SDO to Hi-Z. As described above, CS may be pulled LOW at any time in order to monitor the conversion status. Typically, CS remains LOW during the data output state. However, the data output state may be aborted by pulling CS HIGH anytime between the first rising edge and the 32nd falling edge of SCK, see Figure 6. On the rising edge of CS, the device aborts the data output state and immediately initiates a new conversion. This is useful for systems not This timing mode utilizes a 2-wire serial I/O interface. The conversion result is shifted out of the device by an externally generated serial clock (SCK) signal, see Figure 7. CS may be permanently tied to ground, simplifying the user interface or isolation barrier. The external serial clock mode is selected at the end of the power-on reset (POR) cycle. The POR cycle is concluded approximately 1ms after VCC exceeds 1.9V. The level applied to SCK at this time determines if SCK is internal or external. SCK must be driven LOW prior to the end of POR in order to enter the external serial clock timing mode. Since CS is tied LOW, the end-of-conversion (EOC) can be continuously monitored at the SDO pin during the convert and sleep states. EOC may be used as an interrupt to an external controller indicating the conversion result is ready. EOC = 1 while the conversion is in progress and EOC = 0 once the conversion enters the low power sleep state. On the falling edge of EOC, the conversion result is loaded into an internal static shift register. The device remains in the sleep state until the first rising edge of SCK. 2.7V TO 5.5V VCC 1F 1 VCC FO = 50Hz REJECTION (LTC2411) = EXTERNAL OSCILLATOR = 60Hz REJECTION (LTC2411) = SIMULTANEOUS 50Hz/60Hz REJECTION (LTC2411-1) 10 LTC2411/ LTC2411-1 REFERENCE VOLTAGE 0.1V TO VCC 2 REF + 3 REF - ANALOG INPUT RANGE -0.5VREF TO 0.5VREF 4 IN + SDO 5 IN - CS 6 SCK 9 3-WIRE SPI INTERFACE 8 7 GND CS BIT 0 SDO TEST EOC TEST EOC BIT 31 EOC EOC Hi-Z Hi-Z BIT 30 BIT 29 BIT 28 SIG MSB BIT 27 BIT 9 Hi-Z TEST EOC BIT 8 Hi-Z SCK (EXTERNAL) SLEEP CONVERSION SLEEP DATA OUTPUT DATA OUTPUT CONVERSION 2411 F06 Figure 6. External Serial Clock, Reduced Data Output Length 17 LTC2411/LTC2411-1 U W U U APPLICATIO S I FOR ATIO Internal Serial Clock, Single Cycle Operation Data is shifted out the SDO pin on each falling edge of SCK enabling external circuitry to latch data on the rising edge of SCK. EOC can be latched on the first rising edge of SCK. On the 32nd falling edge of SCK, SDO goes HIGH (EOC = 1) indicating a new conversion has begun. This timing mode uses an internal serial clock to shift out the conversion result and a CS signal to monitor and control the state of the conversion cycle, see Figure 8. 2.7V TO 5.5V VCC 1F 1 VCC FO = 50Hz REJECTION (LTC2411) = EXTERNAL OSCILLATOR = 60Hz REJECTION (LTC2411) = SIMULTANEOUS 50Hz/60Hz REJECTION (LTC2411-1) 10 LTC2411/ LTC2411-1 REFERENCE VOLTAGE 0.1V TO VCC 2 REF + 3 REF - ANALOG INPUT RANGE -0.5VREF TO 0.5VREF 4 IN + SDO 5 IN - CS 6 SCK 9 2-WIRE I/O 8 7 GND CS BIT 31 SDO BIT 30 EOC BIT 29 BIT 28 SIG MSB BIT 27 BIT 26 BIT 5 BIT 0 LSB24 SCK (EXTERNAL) CONVERSION SLEEP DATA OUTPUT CONVERSION 2411 F07 Figure 7. External Serial Clock, CS = 0 Operation VCC 2.7V TO 5.5V VCC 1F 1 VCC FO 10 LTC2411/ LTC2411-1 REFERENCE VOLTAGE 0.1V TO VCC 2 REF + 3 REF - ANALOG INPUT RANGE -0.5VREF TO 0.5VREF 4 IN + SDO 5 IN - CS 6 SCK = 50Hz REJECTION (LTC2411) = EXTERNAL OSCILLATOR = 60Hz REJECTION (LTC2411) = SIMULTANEOUS 50Hz/60Hz REJECTION (LTC2411-1) 10k 9 3-WIRE SPI INTERFACE 8 7 GND tEOCtest SCK 10k 9 3-WIRE SPI INTERFACE 8 7 GND (VCC - 0.4V)]. During the conversion period, the undershoot and/or overshoot of a fast digital signal connected to the LTC2411/ LTC2411-1 pins may severely disturb the analog to digital conversion process. Undershoot and overshoot can occur because of the impedance mismatch at the converter pin when the transition time of an external control signal is less than twice the propagation delay from the driver to LTC2411/LTC2411-1. For reference, on a regular FR-4 board, signal propagation velocity is approximately 183ps/inch for internal traces and 170ps/inch for surface traces. Thus, a driver generating a control signal with a minimum transition time of 1ns must be connected to the converter pin through a trace shorter than 2.5 inches. This problem becomes particularly difficult when shared control lines are used and multiple reflections may occur. The solution is to carefully terminate all transmission lines close to their characteristic impedance. Parallel termination near the LTC2411/LTC2411-1 pin will eliminate this problem but will increase the driver power dissipation. A series resistor between 27 and 56 placed near the driver or near the LTC2411/LTC2411-1 pin will also eliminate this problem without additional power dissipation. The actual resistor value depends upon the trace impedance and connection topology. An alternate solution is to reduce the edge rate of the control signals. It should be noted that using very slow edges will increase the converter power supply current during the transition time. The differential input and reference architecture reduce substantially the converter's sensitivity to ground currents. 21 LTC2411/LTC2411-1 U W U U APPLICATIO S I FOR ATIO Particular attention must be given to the connection of the FO signal when the LTC2411/LTC2411-1 are used with an external conversion clock. This clock is active during the conversion time and the normal mode rejection provided by the internal digital filter is not very high at this frequency. A normal mode signal of this frequency at the converter reference terminals may result into DC gain and INL errors. A normal mode signal of this frequency at the converter input terminals may result into a DC offset error. Such perturbations may occur due to asymmetric capacitive coupling between the FO signal trace and the converter input and/or reference connection traces. An immediate solution is to maintain maximum possible separation between the FO signal trace and the input/reference signals. When the FO signal is parallel terminated near the converter, substantial AC current is flowing in the loop formed by the FO connection trace, the termination and the ground return path. Thus, perturbation signals may be inductively coupled into the converter input and/or reference. In this situation, the user must reduce to a minimum the loop area for the FO signal as well as the loop area for the differential input and reference connections. IREF+ VCC ILEAK VCC ILEAK RSW (TYP) 20k VIN+ CEQ 6pF (TYP) ILEAK IIN - VCC V2 I REF + ( + VREFCM IN - )AVG = 1.5 * VREF0-.5V*INCM REQ VREF * REQ ( + VREFCM IN + )AVG = -1.5 * VREF0.-5 *VINCM REQ VREF * REQ I REF - V2 where: REF + + REF - VREFCM = 2 VIN - ILEAK IREF - When using the internal oscillator (FO = LOW or HIGH), the LTC2411 (LTC2411-1)'s front-end switched-capacitor network is clocked at 76800Hz (69900Hz) corresponding to VREF = REF + - REF - RSW (TYP) 20k ILEAK For a simple approximation, the source impedance RS driving an analog input pin (IN+, IN-, REF+ or REF-) can be considered to form, together with RSW and CEQ (see Figure 11), a first order passive network with a time constant = (RS + RSW) * CEQ. The converter is able to sample the input signal with better than 1ppm accuracy if the sampling period is at least 14 times greater than the input circuit time constant . The sampling process on the four input analog pins is quasi-independent so each time constant should be considered by itself and, under worstcase circumstances, the errors may add. - VREFCM ( )AVG = VIN + V0INCM .5 * REQ -V + V -V = IN INCM REFCM I(IN- ) AVG 0.5 * REQ VREF+ IIN+ The input and reference pins of the LTC2411/LTC2411-1 converter are directly connected to a network of sampling capacitors. Depending upon the relation between the differential input voltage and the differential reference voltage, these capacitors are switching between these four pins transfering small amounts of charge in the process. A simplified equivalent circuit is shown in Figure 11. I IN+ RSW (TYP) 20k ILEAK Driving the Input and Reference VIN = IN+ - IN- VCC ILEAK IN+ - IN- VINCM = 2 RSW (TYP) 20k 2411 F11 VREF - REQ = 10.8M INTERNAL OSCILLATOR 60Hz Notch (FO = LOW)(LTC 2411) REQ = 13.0M INTERNAL OSCILLATOR 50Hz Notch (FO = HIGH)(LTC 2411) ILEAK REQ = 11.9M INTERNAL OSCILLATOR (FO = LOW)(LTC 2411 - 1) SWITCHING FREQUENCY fSW = 76800Hz INTERNAL OSCILLATOR (FO = LOW OR HIGH) fSW = 0.5 * fEOSC EXTERNAL OSCILLATOR ( ) REQ = 1.67 * 1012 / fEOSC EXTERNAL OSCILLATOR Figure 11. LTC2411/LTC2411-1 Equivalent Analog Input Circuit 22 LTC2411/LTC2411-1 U W U U APPLICATIO S I FOR ATIO a 13s (14.2s) sampling period. Thus, for settling errors of less than 1ppm, the driving source impedance should be chosen such that 13s/14 = 920ns (1.02s). When an external oscillator of frequency fEOSC is used, the sampling period is 2/fEOSC and, for a settling error of less than 1ppm, 0.14/fEOSC. they include the effect of the actual second order input network together with the nonlinear settling process of the input amplifiers. For small CIN values, the settling on IN+ and IN - occurs almost independently and there is little benefit in trying to match the source impedance for the two pins. RSOURCE Input Current For relatively small values of input capacitance (C IN < 0.01F), the voltage on the sampling capacitor settles almost completely and relatively large values for the source impedance result in only small errors. Such values for CIN will deteriorate the converter offset and gain performance without significant benefits of signal filtering and the user is advised to avoid them. Nevertheless, when small values of CIN are unavoidably present as parasitics of input multiplexers, wires, connectors or sensors, the LTC2411/LTC2411-1 can maintain their exceptional accuracy while operating with relative large values of source resistance as shown in Figures 13 and 14. These measured results may be slightly different from the first order approximation suggested earlier because CPAR 20pF CIN RSOURCE VINCM - 0.5VIN LTC2411/ LTC2411-1 IN - CPAR 20pF CIN 2411 F12 Figure 12. An RC Network at IN + and IN - 50 +FS ERROR (ppm OF VREF) The effect of this input dynamic current can be analyzed using the test circuit of Figure 12. The CPAR capacitor includes the LTC2411/LTC2411-1 pin capacitance (5pF typical) plus the capacitance of the test fixture used to obtain the results shown in Figures 13 and 14. A careful implementation can bring the total input capacitance (CIN + CPAR) closer to 5pF thus achieving better performance than the one predicted by Figures 13 and 14. The effect of the input dynamic current is almost the same for the LTC2411 and the LTC2411-1 and measurements of the LTC2411 with FO = GND are plotted out as a typical case. For simplicity, two distinct situations can be considered. VINCM + 0.5VIN VCC = 5V REF + = 5V REF - = GND IN + = 5V IN - = 2.5V CIN = 0.01F FO = GND TA = 25C 40 30 CIN = 0.001F 20 CIN = 100pF CIN = 0pF 10 0 1 10 100 1k RSOURCE () 10k 100k 2411 F13 Figure 13. +FS Error vs RSOURCE 0 -FS ERROR (ppm OF VREF) If complete settling occurs on the input, conversion results will be unaffected by the dynamic input current. An incomplete settling of the input signal sampling process may result in gain and offset errors, but it will not degrade the INL performance of the converter. Figure 11 shows the mathematical expressions for the average bias currents flowing through the IN + and IN - pins as a result of the sampling charge transfers when integrated over a substantial time period (longer than 64 internal clock cycles). IN + at IN + or IN - (Small CIN) VCC = 5V REF + = 5V REF - = GND IN + = GND IN - = 2.5V CIN = 0pF FO = GND TA = 25C CIN = 100pF -10 -20 CIN = 0.001F -30 CIN = 0.01F -40 -50 1 10 100 1k RSOURCE () 10k 100k 2411 F14 Figure 14. -FS Error vs RSOURCE at IN + or IN - (Small CIN) 23 LTC2411/LTC2411-1 U W U U APPLICATIO S I FOR ATIO Larger values of input capacitors (CIN > 0.01F) may be required in certain configurations for antialiasing or general input signal filtering. Such capacitors will average the input sampling charge and the external source resistance will see a quasi constant input differential impedance. For the LTC2411, when FO = LOW (internal oscillator and 60Hz notch), the typical differential input resistance is 5.4M which will generate a gain error of approximately 0.093ppm for each ohm of source resistance driving IN+ or IN -. When FO = HIGH (internal oscillator and 50Hz notch), the typical differential input resistance is 6.5M which will generate a gain error of approximately 0.077ppm for each ohm of source resistance driving IN+ or IN -. For the LTC2411-1, the typical differential input resistance is 6M which will generate a gain error of approximately 0.084ppm for each ohm of source resistance driving IN+ or IN- (FO = LOW). When FO is driven by an external oscillator with a frequency fEOSC (external conversion clock operation), the typical differential input resistance is 0.83 * 1012/fEOSC and each ohm of source resistance driving IN+ or IN - will result in 0.59 * 10-6 * fEOSCppm gain error. The effect of the source resistance on the two input pins is additive with respect to this gain error. The typical +FS and -FS errors as a function of the sum of the source resistance seen by IN+ and IN- for large values of CIN are shown in Figure 15. reference common mode voltages. While the input drive circuit nonzero source impedance combined with the converter average input current will not degrade the INL performance, indirect distortion may result from the modulation of the offset error by the common mode component of the input signal. Thus, when using large CIN capacitor values, it is advisable to carefully match the source impedance seen by the IN+ and IN- pins. For the LTC2411, when FO = LOW (internal oscillator and 60Hz notch), every 1 mismatch in source impedance transforms a full-scale common mode input signal into a differential mode input signal of 0.093ppm. When FO = HIGH (internal oscillator and 50Hz notch), every 1 mismatch in source impedance transforms a full-scale common mode input signal into a differential mode input signal of 0.077ppm. For the LTC2411-1, when internal oscillator is used (FO = LOW), every 1 mismatch in source impedance transforms a full-scale common mode input signal into a differential mode input signal of 0.084ppm. When FO is driven by an external oscillator with a frequency fEOSC, every 1 mismatch in source impedance transforms a full-scale common mode input signal into a differential mode input signal of 0.59 * 10-6 * fEOSCppm. Figure 16 shows the typical offset error due to input common mode voltage for various values of source resistance imbalance between the IN+ and IN- pins when large CIN values are used. In addition to this gain error, an offset error term may also appear. The offset error is proportional with the mismatch between the source impedance driving the two input pins IN+ and IN- and with the difference between the input and If possible, it is desirable to operate with the input signal common mode voltage very close to the reference signal common mode voltage as is the case in the ratiometric measurement of a symmetric bridge. This configuration +FS ERROR (ppm OF VREF) 100 80 0 VCC = 5V REF + = 5V REF - = GND IN + = 3.75V IN - = 1.25V FO = GND TA = 25C CIN = 0.01F -20 CIN = 10F CIN = 1F 60 40 20 CIN = 0.1F CIN = 0.01F -40 CIN = 0.1F -60 -80 -100 -120 0 0 100 200 300 400 500 600 700 800 900 1000 RSOURCE () 2411 F15a Figure 15a. + FS Error vs RSOURCE at IN + or IN - (Large CIN) 24 -FS ERROR (ppm OF VREF) 120 VCC = 5V REF + = 5V REF - = GND IN + = 1.25V IN - = 3.75V FO = GND TA = 25C CIN = 10F CIN = 1F 0 100 200 300 400 500 600 700 800 900 1000 RSOURCE () 2411 F15b Figure 15b. - FS Error vs RSOURCE at IN + or IN - (Large CIN) LTC2411/LTC2411-1 U W U U APPLICATIO S I FOR ATIO 50 OFFSET ERROR (ppm OF VREF) 30 B 20 does not change the converter offset, but it may degrade the gain and INL performance. The effect of this current can be analyzed in the same two distinct situations. VCC = 5V REF + = 5V REF - = GND IN + = IN - = VINCM A 40 C 10 D 0 E -10 F -20 -30 FO = GND TA = 25C RSOURCEIN - = 500 CIN = 10F G -40 -50 0 0.5 1 1.5 2 2.5 3 VINCM (V) A: RIN = +400 B: RIN = +200 C: RIN = +100 D: RIN = 0 3.5 4 4.5 5 E: RIN = -100 F: RIN = -200 G: RIN = -400 2411 F16 Figure 16. Offset Error vs Common Mode Voltage (VINCM = IN+ = IN-) and Input Source Resistance Imbalance (RIN = RSOURCEIN+ - RSOURCEIN-) for Large CIN Values (CIN 1F) eliminates the offset error caused by mismatched source impedances. The magnitude of the dynamic input current depends upon the size of the very stable internal sampling capacitors and upon the accuracy of the converter sampling clock. The accuracy of the internal clock over the entire temperature and power supply range is typically better than 1%. Such a specification can also be easily achieved by an external clock. When relatively stable resistors (50ppm/C) are used for the external source impedance seen by IN+ and IN-, the expected drift of the dynamic current, offset and gain errors will be insignificant (about 1% of their respective values over the entire temperature and voltage range). Even for the most stringent applications, a one-time calibration operation may be sufficient. In addition to the input sampling charge, the input ESD protection diodes have a temperature dependent leakage current. This current, nominally 1nA (10nA max), results in a small offset shift. A 100 source resistance will create a 0.1V typical and 1V maximum offset voltage. Reference Current In a similar fashion, the LTC2411/LTC2411-1 sample the differential reference pins REF+ and REF- transfering small amount of charge to and from the external driving circuits thus producing a dynamic reference current. This current For relatively small values of the external reference capacitors (CREF < 0.01F), the voltage on the sampling capacitor settles almost completely and relatively large values for the source impedance result in only small errors. Such values for CREF will deteriorate the converter offset and gain performance without significant benefits of reference filtering and the user is advised to avoid them. Larger values of reference capacitors (CREF > 0.01F) may be required as reference filters in certain configurations. Such capacitors will average the reference sampling charge and the external source resistance will see a quasi constant reference differential impedance. For the LTC2411, when FO = LOW (internal oscillator and 60Hz notch), the typical differential reference resistance is 3.9M which will generate a gain error of approximately 0.13ppm for each ohm of source resistance driving REF+ or REF-. When FO = HIGH (internal oscillator and 50Hz notch), the typical differential reference resistance is 4.68M which will generate a gain error of approximately 0.11ppm for each ohm of source resistance driving REF+ or REF -. For the LTC2411-1, when internal oscillator is used (FO = LOW), the typical differential reference resistance is 4.29M which will generate a gain error of approximately 0.12ppm for each ohm of source resistance driving REF + or REF -. When FO is driven by an external oscillator with a frequency fEOSC (external conversion clock operation), the typical differential reference resistance is 0.60 * 1012/fEOSC and each ohm of source resistance drving REF+ or REF- will result in 0.823 * 10-6 * fEOSCppm gain error. The effect of the source resistance on the two reference pins is additive with respect to this gain error. The typical FS errors for various combinations of source resistance seen by the REF+ and REF- pins and external capacitance CREF connected to these pins are shown in Figures 17 and 18. Typical - FS errors are similar to + FS errors with opposite polarity. In addition to this gain error, the converter INL performance is degraded by the reference source impedance. For LTC2411, when FO = LOW (internal oscillator and 60Hz notch), every 100 of source resistance driving REF+ or 25 LTC2411/LTC2411-1 U W U U APPLICATIO S I FOR ATIO 50 VCC = 5V REF + = 5V REF - = GND IN + = 3.75V IN - = 1.25V FO = GND TA = 25C -10 -20 -FS ERROR (ppm OF VREF) +FS ERROR (ppm OF VREF) 0 CREF = 0pF -30 CREF = 100pF CREF = 0.001F -40 VCC = 5V REF + = 5V REF - = GND 40 IN + = 1.25V IN - = 3.75V FO = GND 30 TA = 25C CREF = 0pF 20 CREF = 100pF CREF = 0.001F 10 CREF = 0.01F CREF = 0.01F -50 0 1 10 100 1k RSOURCE () 10k 100k 1 10 100 1k RSOURCE () 10k 100k 2411 F17a Figure 17a. +FS Error vs RSOURCE at REF+ or REF- (Small CIN) 2411 F17b Figure 17b. - FS Error vs RSOURCE at REF+ or REF- (Small CIN) 160 0 CREF = 0.01F CREF = 0.1F - FS ERROR (ppm OF VREF) +FS ERROR (ppm OF VREF) -20 -40 -60 CREF = 10F CREF = 1F -80 -100 -120 -140 -160 VCC = 5V REF + = 5V REF - = GND IN + = 3.75V IN - = 1.25V FO = GND TA = 25C VCC = 5V + 140 REF - = 5V REF = GND + 120 IN - = 1.25V IN = 3.75V 100 FO = GND TA = 25C CREF = 10F CREF = 1F 80 CREF = 0.1F 60 40 CREF = 0.01F 20 0 0 100 200 300 400 500 600 700 800 900 1000 RSOURCE () 0 100 200 300 400 500 600 700 800 900 1000 RSOURCE () 2411 F18b 2411 F18a Figure 18a. +FS Error vs RSOURCE at REF+ or REF- (Large CIN) Figure 18b. - FS Error vs RSOURCE at REF+ or REF- (Large CIN) 10 REF- translates into about 0.45ppm additional INL error. 26 6 INL (ppm OF VREF) When FO = HIGH (internal oscillator and 50Hz notch), every 100 of source resistance driving REF+ or REF- translates into about 0.37ppm additional INL error. For the LTC2411-1, when FO = LOW, every 100 of source resistance driving REF+ or REF- translates into about 0.41ppm additional INL error. When FO is driven by an external oscillator with a frequency fEOSC, every 100 of source resistance driving REF+ or REF- translates into about 2.91 * 10-6 * fEOSCppm additional INL error. Figure 19 shows the typical INL error due to the source resistance driving the REF+ or REF- pins when large CREF values are used. The effect of the source resistance on the two reference pins is additive with respect to this INL error. In general, matching of source impedance for the REF+ and REF- pins does not help the gain or the INL error. The 9 RSOURCE = 2k RSOURCE = 1k 4 2 0 -2 RSOURCE = 500 -4 -6 -8 -10 -0.5-0.4- 0.3- 0.2- 0.1 0 0.1 0.2 0.3 0.4 0.5 VINDIF/VREFDIF VCC = 5V FO = GND REF + = 5V CREF = 10F REF - = GND TA = 25C 2411 F19 VINCM = 0.5 * (IN + + IN -) = 2.5V Figure 19. INL vs Differential Input Voltage (VIN = IN+ = IN-) and Reference Source Resistance (RSOURCE at REF + and REF -) for Large CREF Values (CREF 1F) LTC2411/LTC2411-1 U W U U APPLICATIO S I FOR ATIO user is thus advised to minimize the combined source impedance driving the REF+ and REF- pins rather than to try to match it. The magnitude of the dynamic reference current depends upon the size of the very stable internal sampling capacitors and upon the accuracy of the converter sampling clock. The accuracy of the internal clock over the entire temperature and power supply range is typical better than 1%. Such a specification can also be easily achieved by an external clock. When relatively stable resistors (50ppm/C) are used for the external source impedance seen by REF+ and REF-, the expected drift of the dynamic current gain error will be insignificant (about 1% of its value over the entire temperature and voltage range). Even for the most stringent applications, a one-time calibration operation may be sufficient. In addition to the reference sampling charge, the reference pins ESD protection diodes have a temperature dependent leakage current. This leakage current, nominally 1nA (10nA max), results in a small gain error. A 100 source resistance will create a 0.05V typical and 0.5V maximum full-scale error. Output Data Rate When using its internal oscillator, the LTC2411 can produce up to 7.5 readings per second with a notch frequency of 60Hz (FO = LOW) and 6.25 readings per second with a notch frequency of 50Hz (FO = HIGH) and the LTC2411-1 can produce up to 6.8 readings per second with FO = LOW. The actual output data rate will depend upon the length of the sleep and data output phases which are controlled by the user and which can be made insignificantly short. When operated with an external conversion clock (FO connected to an external oscillator), the LTC2411/LTC24111 output data rate can be increased as desired. The duration of the conversion phase is 20510/fEOSC. If fEOSC = 153600Hz, the converter behaves as if the internal oscillator is used and the notch is set at 60Hz. There is no significant difference in the LTC2411/LTC2411-1 performance between these two operation modes. An increase in fEOSC over the nominal 153600Hz will translate into a proportional increase in the maximum output data rate. This substantial advantage is nevertheless accompanied by three potential effects, which must be carefully considered. First, a change in fEOSC will result in a proportional change in the internal notch position and in a reduction of the converter differential mode rejection at the power line frequency. In many applications, the subsequent performance degradation can be substantially reduced by relying upon the LTC2411/LTC2411-1's exceptional common mode rejection and by carefully eliminating common mode to differential mode conversion sources in the input circuit. The user should avoid single-ended input filters and should maintain a very high degree of matching and symmetry in the circuits driving the IN+ and IN- pins. Second, the increase in clock frequency will increase proportionally the amount of sampling charge transferred through the input and the reference pins. If large external input and/or reference capacitors (CIN, CREF) are used, the previous section provides formulae for evaluating the effect of the source resistance upon the converter performance for any value of fEOSC. If small external input and/ or reference capacitors (CIN, CREF) are used, the effect of the external source resistance upon the LTC2411/ LTC2411-1 typical performance can be inferred from Figures 13, 14 and 17 in which the horizontal axis is scaled by 153600/fEOSC. Third, an increase in the frequency of the external oscillator above 460800Hz (a more than 3x increase in the output data rate) will start to decrease the effectiveness of the internal autocalibration circuits. This will result in a progressive degradation in the converter accuracy and linearity. Typical measured performance curves for output data rates up to 100 readings per second are shown in Figures 20 to 27. In order to obtain the highest possible level of accuracy from this converter at output data rates above 20 readings per second, the user is advised to maximize the power supply voltage used and to limit the maximum ambient operating temperature. In certain circumstances, a reduction of the differential reference voltage may be beneficial. Input Bandwidth The combined effect of the internal sinc4 digital filter and of the analog and digital autocalibration circuits determines the LTC2411/LTC2411-1 input bandwidth. When 27 LTC2411/LTC2411-1 U W U U APPLICATIO S I FOR ATIO 250 VCC = 5V VREF = 5V VINCM = 2.5V VIN = 0V FO = EXT OSC 80 40 VCC = 5V VREF = 5V IN + = 3.75V IN - = 1.25V FO = EXT OSC 200 +FS ERROR (ppm OF VREF) OFFSET ERROR (ppm OF VREF) 120 TA = 85C 0 -40 TA = 25C 150 100 TA = 85C 50 TA = 25C 0 -80 -50 -120 0 0 10 20 30 40 50 60 70 80 90 100 OUTPUT DATA RATE (READINGS/SEC) 10 20 30 40 50 60 70 80 90 100 OUTPUT DATA RATE (READINGS/SEC) 2411 F21 2411 F20 Figure 20. Offset Error vs Output Data Rate and Temperature Figure 21. + FS Error vs Output Data Rate and Temperature 22 100 TA = 25C 21 50 0 TA = 85C -50 VCC = 5V VREF = 5V -100 IN + = 1.25V IN - = 3.75V FO = EXT OSC -150 0 10 20 30 40 50 60 70 80 90 100 OUTPUT DATA RATE (READINGS/SEC) RESOLUTION (BITS) -FS ERROR (ppm OF VREF) TA = 25C TA = 85C 20 19 VCC = 5V VREF = 5V VINCM = 2.5V VIN = 0V FO = EXT OSC RES = LOG2(VREF/NOISERMS) 18 17 16 0 10 20 30 40 50 60 70 80 90 100 OUTPUT DATA RATE (READINGS/SEC) 2411 F22 2411 F23 Figure 23. Resolution (NoiseRMS 1LSB) vs Output Data Rate and Temperature Figure 22. - FS Error vs Output Data Rate and Temperature 40 22 RESOLUTION (BITS) 18 TA = 85C TA = 25C 16 VCC = 5V VREF = 5V VINCM = 2.5V VIN = 0V FO = EXT OSC RES = LOG2(VREF/INLMAX) 14 12 10 0 VREF = 2.5V 0 -20 VREF = 5V -40 -60 VCC = 5V REF - = GND VINCM = 2.5V VIN = 0V FO = EXT OSC TA = 25C -80 -100 -120 10 20 30 40 50 60 70 80 90 100 OUTPUT DATA RATE (READINGS/SEC) 2411 F24 Figure 24. Resolution (INLRMS 1LSB) vs Output Data Rate and Temperature 28 OFFSET ERROR (ppm OF VREF) 20 20 0 10 20 30 40 50 60 70 80 90 100 OUTPUT DATA RATE (READINGS/SEC) 2411 F25 Figure 25. Offset Error vs Output Data Rate and Reference Voltage LTC2411/LTC2411-1 U W U U APPLICATIO S I FOR ATIO 22 22 VREF = 5V 20 VREF = 2.5V 20 VCC = 5V REF - = GND VINCM = 2.5V 19 VIN = 0V FO = EXT OSC RES = LOG2(VREF/NOISERMS) TA = 25C 18 0 10 20 30 40 50 60 70 80 90 100 OUTPUT DATA RATE (READINGS/SEC) RESOLUTION (BITS) RESOLUTION (BITS) 21 18 VREF = 2.5V VCC = 5V REF - = GND VINCM = 2.5V VIN = 0V FO = EXT OSC RES = LOG2(VREF/INLMAX) TA = 25C 14 12 10 0 10 20 30 40 50 60 70 80 90 100 OUTPUT DATA RATE (READINGS/SEC) 2411 F27 2411 F26 Figure 27. Resolution (INLMAX 1LSB) vs Output Data Rate and Reference Voltage Figure 26. Resolution (NoiseRMS 1LSB) vs Output Data Rate and Reference Voltage 0.0 -0.5 INPUT SIGNAL ATTENUATION (dB) the internal oscillator is used, the 3dB input bandwidth of the LTC2411 is 3.63Hz for 60Hz notch frequency (FO = LOW) and 3.02Hz for 50Hz notch frequency (FO = HIGH). The 3dB input bandwidth for the LTC2411-1 is 3.30Hz (FO = LOW). If an external conversion clock generator of frequency fEOSC is connected to the FO pin, the 3dB input bandwidth is 0.236 * 10-6 * fEOSC. VREF = 5V 16 -1.0 -1.5 -2.0 -2.5 -3.0 -3.5 -4.0 FO = HIGH (LTC2411) FO = LOW (LTC2411) FO = LOW (LTC2411-1) -4.5 Due to the complex filtering and calibration algorithms utilized, the converter input bandwidth is not modeled very accurately by a first order filter with the pole located at the 3dB frequency. When the internal oscillator is used, the shape of the LTC2411/LTC2411-1 input bandwidth is shown in Figure 28. When an external oscillator of frequency fEOSC is used, the shape of the LTC2411/LTC2411-1 input bandwidth can be derived from Figure 28, FO = LOW curve of the LTC2411 in which the horizontal axis is scaled by fEOSC/153600. solution is a high gain, low bandwidth amplifier stage followed by a high bandwidth unity-gain buffer. The conversion noise (1.45VRMS typical for VREF = 5V) can be modeled as a white noise source connected to a noise free converter. The noise spectral density is 70nV/Hz for an infinite bandwidth source and 126nV/Hz for a single 0.5MHz pole source. From these numbers, it is clear that particular attention must be given to the design of external amplification circuits. Such circuits face the simultaneous requirements of very low bandwidth (just a few Hz) in order to reduce the output referred noise and relatively high bandwidth (at least 500kHz) necessary to drive the input switched-capacitor network. A possible When external amplifiers are driving the LTC2411/ LTC2411-1, the ADC input referred system noise calculation can be simplified by Figure 29. The noise of an amplifier driving the LTC2411/LTC2411-1 input pin can be modeled as a band-limited white noise source. Its bandwidth can be approximated by the bandwidth of a single pole lowpass filter with a corner frequency fi. The amplifier noise spectral density is ni. From Figure 29, using fi as the x-axis selector, we can find on the y-axis the noise equivalent bandwidth freqi of the input driving amplifier. This bandwidth includes the band limiting effects of the ADC -5.0 -5.5 -6.0 0 0.5 1 1.5 2 2.5 3 3.5 4 4.5 5 DIFFERENTIAL INPUT SIGNAL FREQUENCY (Hz) 2411 F28 Figure 28. Input Signal Bandwidth Using the Internal Oscillator 29 LTC2411/LTC2411-1 U W U U APPLICATIO S I FOR ATIO internal calibration and filtering. The noise of the driving amplifier referred to the converter input and including all these effects can be calculated as N = ni * freqi. The total system noise (referred to the LTC2411/LTC2411-1 input) can now be obtained by summing as square root of sum of squares the three ADC input referred noise sources: the LTC2411/LTC2411-1 internal noise (1.45V), the noise of the IN + driving amplifier and the noise of the IN - driving amplifier. If the FO pin is driven by an external oscillator of frequency fEOSC, Figure 29 can still be used for noise calculation if the x-axis is scaled by fEOSC/153600. For large values of the ratio fEOSC/153600, the Figure 29 plot accuracy begins to decrease, but in the same time the LTC2411/LTC2411-1 INPUT REFERRED NOISE EQUIVALENT BANDWIDTH (Hz) 1000 100 FO = LOW 10 FO = HIGH 1 0.1 0.1 1 10 100 1k 10k 100k INPUT NOISE SOURCE SINGLE POLE EQUIVALENT BANDWIDTH (Hz) 1M 2411 G29 Figure 29. Input Referred Noise Equivalent Bandwidth of an Input Connected White Noise Source -30 -40 -50 -60 -70 -80 -90 -100 -110 0 fS 2fS 3fS 4fS 5fS 6fS 7fS 8fS 9fS 10fS11fS12fS DIFFERENTIAL INPUT SIGNAL FREQUENCY (Hz) 2411 F30 Figure 30. Input Normal Mode Rejection, Internal Oscillator and 50Hz Notch (LTC2411) 30 One of the advantages delta-sigma ADCs offer over conventional ADCs is on-chip digital filtering. Combined with a large oversampling ratio, the LTC2411/LTC2411-1 significantly simplifies antialiasing filter requirements. The sinc4 digital filter provides greater than 120dB normal mode rejection at all frequencies except DC and integer multiples of the modulator sampling frequency (fS). The LTC2411/LTC2411-1's autocalibration circuits further simplify the antialiasing requirements by additional normal mode signal filtering both in the analog and digital domain. Independent of the operating mode, fS = 256 * fN = 2048 * fOUTMAX where fN is the notch frequency and fOUTMAX is the maximum output data rate. In the internal oscillator mode, for the LTC2411, FS = 12800Hz with a 50Hz notch setting and fS = 15360Hz with a 60Hz notch setting. For the LTC2411-1, fS = 13980Hz (FO = LOW). In the external oscillator mode, fS = fEOSC/10. The combined normal mode rejection performance is shown in Figure 30 for the internal oscillator with 50Hz notch setting (FO = HIGH) and in Figure 31 for the internal oscillator with FO = LOW and for the external oscillator mode. The regions of low rejection occurring at integer multiples of fS have a very narrow bandwidth. Magnified details of the normal mode rejection curves are shown in 0 FO = HIGH -20 -120 Normal Mode Rejection and Antialiasing INPUT NORMAL MODE REJECTION (dB) INPUT NORMAL MODE REJECTION (dB) 0 -10 noise floor rises and the noise contribution of the driving amplifiers lose significance. FO = LOW OR FO = EXTERNAL OSCILLATOR, fEOSC = 10 * fS -10 -20 -30 -40 -50 -60 -70 -80 -90 -100 -110 -120 0 fS 2fS 3fS 4fS 5fS 6fS 7fS 8fS 9fS 10fS DIFFERENTIAL INPUT SIGNAL FREQUENCY (Hz) 2411 F31 Figure 31. Input Normal Mode Rejection, Internal Oscillator and FO = LOW or External Oscillator LTC2411/LTC2411-1 U W U U 0 0 -10 -10 INPUT NORMAL MODE REJECTION (dB) INPUT NORMAL MODE REJECTION (dB) APPLICATIO S I FOR ATIO -20 -30 -40 -50 -60 -70 -80 -90 -100 -110 -120 0 fN 2fN 3fN 4fN 5fN 6fN 7fN INPUT SIGNAL FREQUENCY (Hz) -20 -30 -40 -50 -60 -70 -80 -90 -100 -110 -120 250fN 252fN 254fN 256fN 258fN 260fN 262fN INPUT SIGNAL FREQUENCY (Hz) 8fN 2411 F33 2411 F32 Figure 32. Input Normal Mode Rejection As a result of these remarkable normal mode specifications, minimal (if any) antialias filtering is required in front of the LTC2411/LTC2411-1. If passive RC components are placed in front of the LTC2411/LTC2411-1, the input dynamic current should be considered (see Input Current section). In cases where large effective RC time constants are used, an external buffer amplifier may be required to minimize the effects of dynamic input current. Traditional high order delta-sigma modulators, while providing very good linearity and resolution, suffer from potential instabilities at large input signal levels. The proprietary architecture used for the LTC2411/LTC2411-1 third order modulator resolves this problem and guarantees a predictable stable behavior at input signal levels of NORMAL MODE REJECTION (dB) The user can expect to achieve in practice this level of performance using the internal oscillator as it is demonstrated by Figures 34 to 36. Typical measured values of the normal mode rejection of the LTC2411 operating with an internal oscillator and a 60Hz notch setting are shown in Figure 34 superimposed over the theoretical calculated curve. Similarly, typical measured values of the normal mode rejection of the LTC2411 operating with an internal oscillator and a 50Hz notch setting are shown in Figure 35 superimposed over the theoretical calculated curve. 0 MEASURED DATA CALCULATED DATA -20 -40 VCC = 5V VREF = 5V VINCM = 2.5V VIN(P-P) = 5V FO = GND TA = 25C - 60 -80 -100 -120 0 15 30 45 60 75 90 105 120 135 150 165 180 195 210 225 240 INPUT FREQUENCY (Hz) 2411 F34 Figure 34. Input Normal Mode Rejection vs Input Frequency (LTC2411) 0 NORMAL MODE REJECTION (dB) Figure 32 (rejection near DC) and Figure 33 (rejection at fS = 256fN) where fN represents the notch frequency. These curves have been derived for the external oscillator mode but they can be used in all operating modes by appropriately selecting the fN value. Figure 33. Input Normal Mode Rejection MEASURED DATA CALCULATED DATA VCC = 5V VREF = 5V VINCM = 2.5V VIN(P-P) = 5V FO = 5V TA = 25C -20 -40 - 60 -80 -100 -120 0 25 50 75 100 125 INPUT FREQUENCY (Hz) 150 175 200 2411 F35 Figure 35. Input Normal Mode Rejection vs Input Frequency (LTC2411) 31 LTC2411/LTC2411-1 U W U U APPLICATIO S I FOR ATIO NORMAL MODE REJECTION (dB) MEASURED DATA CALCULATED DATA -20 -40 - 60 VCC = 5V VREF = 5V REF - = GND VINCM = 2.5V VIN(P-P) = 5V FO = GND TA = 25C -80 -100 -120 NORMAL MODE REJECTION (dB) 0 0 VIN(P-P) = 5V VIN(P-P) = 7.5V (150% OF FULL SCALE) -20 -40 VCC = 5V VREF = 5V VINCM = 2.5V FO = GND TA = 25C - 60 -80 -100 -120 0 20 40 60 80 100 120 140 160 INPUT FREQUENCY (Hz) 180 200 0 220 15 30 45 60 75 90 105 120 135 150 165 180 195 210 225 240 INPUT FREQUENCY (Hz) 2411 F37 2411 F36 Figure 36. Input Normal Mode Rejection vs Input Frequency (LTC2411-1) BRIDGE APPLICATIONS Typical strain gauge based bridges deliver only 2mV/Volt of excitation. As the maximum reference voltage of the LTC2411/LTC2411-1 is 5V, remote sensing of applied excitation without additional circuitry requires that excitation be limited to 5V. This gives only 10mV full scale, which can be resolved to 1 part in 5000 without averaging. For many solid state sensors, this is comparable to the sensor. 32 NORMAL MODE REJECTION (dB) 0 VIN(P-P) = 5V VIN(P-P) = 7.5V (150% OF FULL SCALE) -20 -40 VCC = 5V VREF = 5V VINCM = 2.5V FO = 5V TA = 25C - 60 -80 -100 -120 0 25 50 75 100 125 INPUT FREQUENCY (Hz) 150 175 200 2411 F38 Figure 38. Measured Input Normal Mode Rejection vs Input Frequency (LTC2411) 0 NORMAL MODE REJECTION (dB) up to 150% of full scale. In many industrial applications, it is not uncommon to have to measure microvolt level signals superimposed over volt level perturbations and LTC2411/LTC2411-1 are eminently suited for such tasks. When the perturbation is differential, the specification of interest is the normal mode rejection for large input signal levels. With a reference voltage VREF = 5V, the LTC2411/ LTC2411-1 have a full-scale differential input range of 5V peak-to-peak. Figures 37 and 38 show measurement results for the LTC2411 normal mode rejection ratio with a 7.5V peak-to-peak (150% of full scale) input signal superimposed over the more traditional normal mode rejection ratio results obtained with a 5V peak-to-peak (full scale) input signal and Figure 39 shows the corresponding measurement result for the LTC2411-1. It is clear that the LTC2411/LTC2411-1 rejection performance is maintained with no compromises in this extreme situation. When operating with large input signal levels, the user must observe that such signals do not violate the device absolute maximum ratings. Figure 37. Measured Input Normal Mode Rejection vs Input Frequency (LTC2411) VIN(P-P) = 5V VIN(P-P) = 7.5V (150% OF FULL SCALE) -20 -40 VCC = 5V VREF = 5V REF - = GND VINCM = 2.5V FO = GND TA = 25C - 60 -80 -100 -120 0 20 40 60 80 100 120 140 160 INPUT FREQUENCY (Hz) 180 200 220 2411 F39 Figure 39. Measured Input Normal Mode Rejection vs Input Frequency (LTC2411-1) LTC2411/LTC2411-1 U W U U APPLICATIO S I FOR ATIO Another option is the use of a reference within the 5V input range of the LTC2411/LTC2411-1 and developing excitation via fixed gain, or LTC1043 based voltage multiplication, along with remote feedback in the excitation amplifiers, as shown in Figures 45 and 46. Averaging 64 samples however reduces the noise level by a factor of eight, bringing the resolving power to 1 part in 40000, comparable to better weighing systems. Hysteresis and creep effects in the load cells are typically much greater than this. Most applications that require strain measurements to this level of accuracy are measuring slowly changing phenomena, hence the time required to average a large number of readings is usually not an issue. For those systems that require accurate measurement of a small incremental change on a significant tare weight, the lack of history effects in the LTC2400 family is of great benefit. Figure 40 shows an example of a simple bridge connection. Note that it is suitable for any bridge application where measurement speed is not of the utmost importance. For many applications where large vessels are weighed, the average weight over an extended period of time is of concern and short term weight is not readily determined due to movement of contents, or mechanical resonance. Often, large weighing applications involve load cells located at each load bearing point, the output of which can be summed passively prior to the signal processing circuitry, actively with amplification prior to the ADC, or can be digitized via multiple ADC channels and summed mathematically. The mathematical summation of the output of multiple LTC2411/LTC2411-1's provide the benefit of a root square reduction in noise. The low power consumption of the LTC2411/LTC2411-1 make it attractive for multidrop communication schemes where the ADC is located within the load-cell housing. For those applications that cannot be fulfilled by the LTC2411/LTC2411-1 alone, compensating for error in external amplification can be done effectively due to the "no latency" feature of the LTC2411/LTC2411-1. No latency operation allows samples of the amplifier offset and gain to be interleaved with weighing measurements. The use of correlated double sampling allows suppression of 1/f noise, offset and thermocouple effects within the bridge. Correlated double sampling involves alternating the polarity of excitation and dealing with the reversal of input polarity mathematically. Alternatively, bridge excitation can be increased to as much as 10V, if one of several precision attenuation techniques is used to produce a precision divide operation on the reference signal. A direct connection to a load cell is perhaps best incorporated into the load-cell body, as minimizing the distance to + R1 350 BRIDGE LT1019 1 2 REF + 3 REF - 4 IN + VCC SDO SCK CS 8 9 7 LTC2411/ LTC2411-1 5 IN - GND R2 FO 10 6 2411 F40 R1 AND R2 CAN BE USED TO INCREASE TOLERABLE AC COMPONENT ON REF SIGNALS Figure 40. Simple Bridge Connection 33 LTC2411/LTC2411-1 U U W U APPLICATIO S I FOR ATIO the sensor largely eliminates the need for protection devices, RFI suppression and wiring. The LTC2411/ LTC2411-1 exhibit extremely low temperature dependent drift. As a result, exposure to external ambient temperature ranges does not compromise performance. The incorporation of any amplification considerably complicates thermal stability, as input offset voltages and currents, temperature coefficient of gain settling resistors all become factors. input stage from the transient load steps produced during conversion. The gain stability and accuracy of this approach is very good, due to a statistical improvement in resistor matching due to individual error contribution being reduced. A gain of 34 may seem low, when compared to common practice in earlier generations of load-cell interfaces, however the accuracy of the LTC2411/LTC2411-1 changes the rationale. Achieving high gain accuracy and linearity at higher gains may prove difficult, while providing little benefit in terms of noise reduction. The circuit in Figure 41 shows an example of a simple amplification scheme. This example produces a differential output with a common mode voltage of 2.5V, as determined by the bridge. The use of a true three amplifier instrumentation amplifier is not necessary, as the LTC2411/ LTC2411-1 have common mode rejection far beyond that of most amplifiers. The LTC1051 is a dual autozero amplifier that can be used to produce a gain of 30 before its input referred noise dominates the LTC2411/LTC2411-1 noise. This example shows a gain of 34, that is determined by a feedback network built using a resistor array containing eight individual resistors. The resistors are organized to optimize temperature tracking in the presence of thermal gradients. The second LTC1051 buffers the low noise At a gain of 100, the gain error that could result from typical open-loop gain of 160dB is -1ppm, however, worst-case is at the minimum gain of 116dB, giving a gain error of -158ppm. Worst-case gain error at a gain of 34, is -54ppm. The use of the LTC1051A reduces the worstcase gain error to -33ppm. The advantage of gain higher than 34, then becomes dubious, as the input referred noise sees little improvement1 and gain accuracy is potentially compromised. 1Input referred noise for A V = 34 is approximately 0.05VRMS, whereas at a gain of 50, it would be 0.048VRMS. 5VREF 0.1F 5V 3 8 + 2 5V - 2 4 350 BRIDGE - 14 4 5 12 3 1 RN1 16 6 11 7 2 6 8 3 - 2 REF + 3 REF - 4 IN + 4 13 U2B 5 7 5 + RN1 = 5k x 8 RESISTOR ARRAY U1A, U1B, U2A, U2B = 1/2 LTC1051 Figure 41. Using Autozero Amplifiers to Reduce Input Referred Noise 34 VCC SDO SCK CS 8 9 7 LTC2411/ LTC2411-1 - 7 + 1 9 6 U1B 5 10 + 1 8 U2A 15 0.1F 0.1F 1 U1A IN - GND FO 10 6 2411 F41 LTC2411/LTC2411-1 U W U U APPLICATIO S I FOR ATIO Note that this 4-amplifier topology has advantages over the typical integrated 3-amplifier instrumentation amplifier in that it does not have the high noise level common in the output stage that usually dominates when an instrumentation amplifier is used at low gain. If this amplifier is used at a gain of 10, the gain error is only 10ppm and input referred noise is reduced to 0.15VRMS. The buffer stages can also be configured to provide gain of up to 50 with high gain stability and linearity. Common mode gain is half the differential gain. The maximum differential signal that can be used is 1/4 VREF, as opposed to 1/2 VREF in the 2-amplifier topology above. Remote Half Bridge Interface As opposed to full bridge applications, typical half bridge applications must contend with nonlinearity in the bridge output, as signal swing is often much greater. Applications include RTD's, thermistors and other resistive elements that undergo significant changes over their span. For single variable element bridges, the nonlinearity of the half Figure 42 shows an example of a single amplifier used to produce single-ended gain. This topology is best used in applications where the gain setting resistor can be made to match the temperature coefficient of the strain gauges. If the bridge is composed of precision resistors, with only one or two variable elements, the reference arm of the bridge can be made to act in conjunction with the feedback resistor to determine the gain. If the feedback resistor is incorporated into the design of the load cell, using resistors which match the temperature coefficient of the loadcell elements, good results can be achieved without the need for resistors with a high degree of absolute accuracy. The common mode voltage in this case, is again a function of the bridge output. Differential gain as used with a 350 bridge is: VS 2.7V TO 5.5V 1 2 R1 25.5k 0.1% REF + VCC 3 REF - LTC2411/ LTC2411-1 4 + IN 2 4 PLATINUM 100 RTD 1 3 5 IN - GND 6 R1 + R2 A V = 9.95 = R1 + 175 2411 F43 Figure 43. Remote Half Bridge Interface 5V + 10F 0.1F 5V 350 BRIDGE 3 + LTC1050S8 2 + - 1 0.1V 7 6 175 REF + 3 REF - 4 IN + + 1F 4 2 20k 1F R1 4.99k R2 46.4k VCC LTC2411/ LTC2411-1 20k 5 IN - GND 6 AV = 9.95 = R1 + R2 R1 + 175 2411 F42 Figure 42. Bridge Amplification Using a Single Amplifier 35 LTC2411/LTC2411-1 U W U U APPLICATIO S I FOR ATIO bridge output can be eliminated completely; if the reference arm of the bridge is used as the reference to the ADC, as shown in Figure 43. The LTC2411/LTC2411-1 can accept inputs up to 1/2 VREF. Hence, the reference resistor R1 must be at least 2x the highest value of the variable resistor. result as the two resistor version, but has a few benefits. If, for example, a 25k reference resistor is used to set the excitation current with a 100 RTD, the negative reference input is sampling the same external node as the positive input, but may result in errors if used with a long cable. For short cable applications, the errors may be acceptably low. If instead the single 25k resistor is replaced with a 10k 5% and a 10k 0.1% reference resistor, the noise level introduced at the reference, at least at higher frequencies, will be reduced. A filter can be introduced into the network, in the form of one or more capacitors, or ferrite beads, as long as the sampling pulses are not translated into an error. The reference voltage is also reduced, but this is not undesirable, as it will decrease the value of the LSB, although, not the input referred noise level. In the case of 100 platinum RTD's, this would suggest a value of 800 for R1. Such a low value for R1 is not advisable due to self-heating effects. A value of 25.5k is shown for R1, reducing self-heating effects to acceptable levels for most sensors. The basic circuit shown in Figure 43 shows connections for a full 4-wire connection to the sensor, which may be located remotely. The differential input connections will reject induced or coupled 60Hz interference, however, the reference inputs do not have the same rejection. If 60Hz or other noise is present on the RTD, a low pass filter is recommended as shown in Figure 44. Note that you cannot place a large capacitor directly at the junction of R1 and R2, as it will store charge from the sampling process. A better approach is to produce a low pass filter decoupled from the input lines with a high value resistor (R3). The circuit shown in Figure 44 shows a more rigorous example of Figure 43, with increased noise suppression and more protection for remote applications. Figure 45 shows an example of gain in the excitation circuit and remote feedback from the bridge. The LTC1043s provide voltage multiplication, providing 10V from a 5V reference with only 1ppm error. The amplifiers are used at unity-gain and, hence, introduce a very little error due to The use of a third resistor in the half bridge, between the variable and fixed elements gives essentially the same 5V R2 10k 0.1% R1 10k, 5% 2 4 PLATINUM 100 RTD 1 3 5V R3 10k 5% + 1F 1 560 LTC1050 2 REF + 3 REF - - VCC LTC2411/ LTC2411-1 10k 4 IN + 10k 5 IN - GND 6 2411 F44 Figure 44. Remote Half Bridge Sensing with Noise Suppression on Reference 36 LTC2411/LTC2411-1 U W U U APPLICATIO S I FOR ATIO 15V 7 20 Q1 2N3904 15V U1 4 LTC1043 15V 6 + 4 200 2 LT1236-5 + 47F 11 10V + 0.1F 12 14 13 + 10F 0.1F 1k 5V 7 1F -15V 33 8 * LTC1150 - 10V 3 17 350 10V BRIDGE 5V 0.1F 1 VCC LTC2411/ LTC2411-1 2 REF + 3 REF - -10V 33 Q2 2N3906 6 + 3 4 -15V - 6 6 * 2 2 3 -15V 1k IN - GND 5 LTC1150 20 IN + 5 U2 LTC1043 15V 7 4 15 18 0.1F *FLYING CAPACITORS ARE 1F FILM (MKP OR EQUIVALENT) 5V U2 4 LTC1043 8 7 SEE LTC1043 DATA SHEET FOR DETAILS ON UNUSED HALF OF U1 * 11 1F FILM 12 200 14 13 2411 F45 -10V 17 -10V Figure 45. LTC1043 Provides Precise 4 x Reference for Excitation Voltages 37 LTC2411/LTC2411-1 U W U U APPLICATIO S I FOR ATIO gain error or due to offset voltages. A 1V/C offset voltage drift translates into 0.05ppm/C gain error. Simpler alternatives, with the amplifiers providing gain using resistor arrays for feedback, can produce results that are similar to bridge sensing schemes via attenuators. Note that the amplifiers must have high open-loop gain or gain error will be a source of error. The fact that input offset voltage has relatively little effect on overall error may lead one to use low performance amplifiers for this application. Note that the gain of a device such as an LF156, (25V/mV over temperature) will produce a worst-case error of -180ppm at a noise gain of 3, such as would be encountered in an inverting gain of 2, to produce -10V from a 5V reference. the LTC2411/LTC2411-1 of 2.5V, maximizing the AC input range for applications where induced 60Hz could reach amplitudes up to 2VRMS. The circuits in Figures 45 and 47 could be used where multiple bridge circuits are involved and bridge output can be multiplexed onto a single LTC2411/LTC2411-1, via an inexpensive multiplexer such as the 74HC4052. Figure 46 shows the use of an LTC2411/LTC2411-1 with a differential multiplexer. This is an inexpensive multiplexer that will contribute some error due to leakage if used directly with the output from the bridge, or if resistors are inserted as a protection mechanism from overvoltage. Although the bridge output may be within the input range of the A/D and multiplexer in normal operation, some thought should be given to fault conditions that could result in full excitation voltage at the inputs to the multiplexer or ADC. The use of amplification prior to the multiplexer will largely eliminate errors associated with channel leakage developing error voltages in the source impedance. The error associated with the 10V excitation would be -80ppm. Hence, overall reference error could be as high as 130ppm, the average of the two. Figure 47 shows a similar scheme to provide excitation using resistor arrays to produce precise gain. The circuit is configured to provide 10V and -5V excitation to the bridge, producing a common mode voltage at the input to 5V 5V + 16 47F 12 14 15 11 REF + 3 REF - LTC2411/ LTC2411-1 74HC4052 1 5 TO OTHER DEVICES 2 1 VCC 13 4 IN + 3 5 IN - 2 6 4 GND 6 8 9 10 A0 A1 2411 F46 Figure 46. Use a Differential Multiplexer to Expand Channel Capability 38 LTC2411/LTC2411-1 U PACKAGE DESCRIPTIO MS10 Package 10-Lead Plastic MSOP (Reference LTC DWG # 05-08-1661) 0.118 0.004* (3.00 0.102) 10 9 8 7 6 0.118 0.004** (3.00 0.102) 0.193 0.006 (4.90 0.15) 1 2 3 4 5 0.034 (0.86) REF 0.043 (1.10) MAX 0.007 (0.18) 0 - 6 TYP 0.021 0.006 (0.53 0.015) SEATING PLANE 0.007 - 0.011 (0.17 - 0.27) 0.0197 (0.50) BSC 0.005 0.002 (0.13 0.05) MSOP (MS10) 1100 * DIMENSION DOES NOT INCLUDE MOLD FLASH, PROTRUSIONS OR GATE BURRS. MOLD FLASH, PROTRUSIONS OR GATE BURRS SHALL NOT EXCEED 0.006" (0.152mm) PER SIDE ** DIMENSION DOES NOT INCLUDE INTERLEAD FLASH OR PROTRUSIONS. INTERLEAD FLASH OR PROTRUSIONS SHALL NOT EXCEED 0.006" (0.152mm) PER SIDE Information furnished by Linear Technology Corporation is believed to be accurate and reliable. However, no responsibility is assumed for its use. Linear Technology Corporation makes no representation that the interconnection of its circuits as described herein will not infringe on existing patent rights. 39 LTC2411/LTC2411-1 U TYPICAL APPLICATIO 15V + 20 Q1 2N3904 1/2 LT1112 1 - C1 0.1F 22 5V 3 LT1236-5 + C3 47F 2 C1 0.1F RN1 10k 10V 1 5V 2 RN1 10k 350 BRIDGE TWO ELEMENTS VARYING 3 1 VCC LTC2411/ LTC2411-1 2 REF + 3 REF - 4 -5V 8 RN1 10k 5 7 IN + 5 IN - GND 6 6 C2 0.1F 33 x2 Q2, Q3 2N3906 x2 RN1 10k 4 20 7 15V RN1 IS CADDOCK T914 10K-010-02 8 4 -15V - 1/2 LT1112 -15V + 6 5 2411 F47 Figure 47. Use Resistor Arrays to Provide Precise Matching in Excitation Amplifier RELATED PARTS PART NUMBER DESCRIPTION COMMENTS LT1019 Precision Bandgap Reference, 2.5V, 5V 3ppm/C Drift, 0.05% Max Initial Accuracy LT1025 Micropower Thermocouple Cold Junction Compensator 80A Supply Current, 0.5C Initial Accuracy LTC1050 Precision Chopper Stabilized Op Amp No External Components 5V Offset, 1.6VP-P Noise LT1236A-5 Precision Bandgap Reference, 5V 0.05% Max Initial Accuracy, 5ppm/C Drift LT1460 Micropower Series Reference 0.075% Max Initial Accuracy, 10ppm/C Max Drift LTC2400 24-Bit, No Latency ADC in SO-8 0.3ppm Noise, 4ppm INL, 10ppm Total Unadjusted Error, 200A LTC2401/LTC2402 1-/2-Channel, 24-Bit, No Latency ADC in MSOP 0.6ppm Noise, 4ppm INL, 10ppm Total Unadjusted Error, 200A LTC2404/LTC2408 4-/8-Channel, 24-Bit, No Latency ADC 0.3ppm Noise, 4ppm INL, 10ppm Total Unadjusted Error, 200A LTC2410 24-Bit, Fully Differential, No Latency ADC 0.16ppm Noise, 2ppm INL, 10ppm Total Unadjusted Error, 200A LTC2413 24-Bit, Fully Differential, No Latency ADC Simultaneous 50Hz and 60Hz Rejection, 800nVRMS Noise LTC2415 24-Bit, No Latency ADC with 15Hz Output Rate Pin Compatible with the LTC2410 LTC2420 20-Bit, No Latency ADC in SO-8 1.2ppm Noise, 8ppm INL, Pin Compatible with LTC2400 LTC2424/LTC2428 4-/8-Channel, 20-Bit, No Latency ADC 1.2ppm Noise, Pin Compatible with LTC2404/LTC2408 40 Linear Technology Corporation 24111f LT/TP 0601 2K * PRINTED IN USA 1630 McCarthy Blvd., Milpitas, CA 95035-7417 (408) 432-1900 FAX: (408) 434-0507 www.linear.com LINEAR TECHNOLOGY CORPORATION 2000