ICL7660, ICL7660A
FN3072 Rev.7.00 Page 9 of 11
Oct 5, 2010
In a typical application where fOSC = 10kHz and C = C1 = C2 =
10F:
RO 46 + 20 + 5 (ESRC)
Since the ESRs of the capacitors are reflected in the output
impedance multiplied by a factor of 5, a high value could
potentially swamp out a low 1/(fPUMP C1) term, rendering an
increase in switching frequency or filter capacitance ineffective.
Typical electrolytic capacitors may have ESRs as high as 10
RO/ 46 + 20 + 5 (ESRC)
Since the ESRs of the capacitors are reflected in the output
impedance multiplied by a factor of 5, a high value could
potentially swamp out a low 1/(fPUMP C1) term, rendering an
increase in switching frequency or filter capacitance ineffective.
Typical electrolytic capacitors may have ESRs as high as 10
Output Ripple
ESR also affects the ripple voltage seen at the output. The total
ripple is determined by 2 voltages, A and B, as shown in Figure
14. Segment A is the voltage drop across the ESR of C2 at the
instant it goes from being charged by C1 (current flow into C2)
to being discharged through the load (current flowing out of
C2). The magnitude of this current change is 2 IOUT, hence
the total drop is 2 IOUT eSRC2V. Segment B is the voltage
change across C2 during time t2, the half of the cycle when C2
supplies current to the load. The drop at B is lOUT t2/C2V.
The peak-to-peak ripple voltage is the sum of these voltage
drops:
Again, a low ESR capacitor will reset in a higher performance
output.
Parallelin g De vic e s
Any number of ICL7660 and ICL7660A voltage converters may
be paralleled to reduce output resistance. The reservoir
capacitor, C2, serves all devices while each device requires its
own pump capacitor, C1. The resultant output resistance would
be approximately:
Cascading Devices
The ICL7660 and ICL7660A may be cascaded as shown to
produced larger negative multiplication of the initial supply
voltage. However, due to the finite efficiency of each device,
the practical limit is 10 devices for light loads. The output
voltage is defined by:
VOUT = -n (VIN),
where n is an integer representing the number of devices
cascaded. The resulting output resistance would be
approximately the weighted sum of the individual ICL7660 and
ICL7660A ROUT values.
Changing the ICL7660/ICL7660A Oscillator
Frequency
It may be desirable in some applications, due to noise or other
considerations, to increase the oscillator frequency. This is
achieved by overdriving the oscillator from an external clock,
as shown in Figure 17. In order to prevent possible device
latchup, a 1k resistor must be used in series with the clock
output. In a situation where the designer has generated the
external clock frequency using TTL logic, the addition of a
10k pullup resistor to V+ supply is required. Note that the
pump frequency with external clocking, as with internal
clocking, will be 1/2 of the clock frequency. Output transitions
occur on the positive-going edge of the clock.
It is also possible to increase the conversion efficiency of the
ICL7660 and ICL7660A at low load levels by lowering the
oscillator frequency. This reduces the switching losses, and is
shown in Figure 18. However, lowering the oscillator frequency
will cause an undesirable increase in the impedance of the
pump (C1) and reservoir (C2) capacitors; this is overcome by
increasing the values of C1 and C2 by the same factor that the
frequency has been reduced. For example, the addition of a
100pF capacitor between pin 7 (OSC) and V+ will lower the
oscillator frequency to 1kHz from its nominal frequency of 10kHz
(a multiple of 10), and thereby necessitate a corresponding
increase in the value of C1 and C2 (from 10F to 100F).
RO 2 (23) + 1+ 4 (ESRC1) + ESRC2
(5 103) (10-5)
RO 2 (23) + 1+ 4 (ESRC1) + ESRC2
(5 103) (10-5)
VRIPPLE
[1
+ 2 (ESRC2)]
IOUT
2 (fPUMP) (C2)
ROUT = ROUT (of ICL7660/ICL7660A)
n (number of devices)
1
2
3
4
8
7
6
5
+
-
10F
ICL7660
VOUT
V+
+
-10F
V+
CMOS
GATE
1k
ICL7660A
FIGURE 17. EXTERNAL CLOCKING