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LT1964 Datasheet PDF : 12 Pages
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LT1964
APPLICATIO S I FOR ATIO
GND
VIN
ADJ
LT1964
IN
OUT
R1 +
R2
VOUT
=
–1.22V(1
+
R2
R1
)
(IADJ)(R2)
VADJ = –1.22V
VOUT
1964 F01
IADJ = 30nA AT 25°C
OUTPUT RANGE = –1.22V TO –20V
Figure 1. Adjustable Operation
Bypass Capacitance and Low Noise Performance
The LT1964 may be used with the addition of a bypass
capacitor from VOUT to the BYP pin to lower output
voltage noise. A good quality low leakage capacitor is
recommended. This capacitor will bypass the reference of
the LT1964, providing a low frequency noise pole. The
noise pole provided by this bypass capacitor will lower the
output voltage noise to as low as 30µVRMS with the
addition of a 0.01µF bypass capacitor. Using a bypass
capacitor has the added benefit of improving transient
response. With no bypass capacitor and a 10µF output
capacitor, a –10mA to –200mA load step will settle to
within 1% of its final value in less than 100µs. With the
addition of a 0.01µF bypass capacitor, the output will stay
within 1% for the same –10mA to –200mA load step (see
LT1964-5 Transient Response in the Typical Characteris-
tics section). However, regulator start-up time is inversely
proportional to the size of the bypass capacitor.
Higher values of output voltage noise may be measured
if care is not exercised with regard to circuit layout
and testing. Crosstalk from nearby traces can induce
unwanted noise onto the output of the LT1964-X.
Output Capacitance and Transient Response
The LT1964 is designed to be stable with a wide range of
output capacitors. The ESR of the output capacitor affects
stability, most notably with small capacitors. A minimum
output capacitor of 1µF with an ESR of 3or less is
recommended to prevent oscillations. The LT1964 is a
micropower device and output transient response will be
a function of output capacitance. Larger values of output
capacitance decrease the peak deviations and provide
improved transient response for larger load current
changes. Bypass capacitors, used to decouple individual
components powered by the LT1964, will increase the
effective output capacitor value.
Extra consideration must be given to the use of ceramic
capacitors. Ceramic capacitors are manufactured with a
variety of dielectrics, each with different behavior across
temperature and applied voltage. The most common di-
electrics used are Z5U, Y5V, X5R, and X7R. The Z5U and
Y5V dielectrics are good for providing high capacitances
in a small package, but exhibit strong voltage and tem-
perature coefficients as shown in Figures 2 and 3. When
used with a –5V regulator, a 10µF Y5V capacitor can
exhibit an effective value as low as 1µF to 2µF over the
operating temperature range. The X5R and X7R dielectrics
result in more stable characteristics and are more suitable
for use as the output capacitor. The X7R type has better
stability across temperature, while the X5R is less expen-
sive and is available in higher values.
Voltage and temperature coefficients are not the only
sources of problems. Some ceramic capacitors have a
piezoelectric response. A piezoelectric device generates
voltage across its terminals due to mechanical stress,
similar to the way a piezoelectric accelerometer or micro-
phone works. For a ceramic capacitor the stress can be
induced by vibrations in the system or thermal transients.
The resulting voltages produced can cause appreciable
amounts of noise, especially when a ceramic capacitor is
used for noise bypassing. A ceramic capacitor produced
Figure 4’s trace in response to light tapping from a pencil.
Similar vibration induced behavior can masquerade as
increased output voltage noise.
1964f
9

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