Applications Information
The LM2907 series of tachometer circuits is designed for
minimum external part count applications and maximum ver-
satility. In order to fully exploit its features and advantages
let’s examine its theory of operation. The first stage of oper-
ation is a differential amplifier driving a positive feedback
flip-flop circuit. The input threshold voltage is the amount of
differential input voltage at which the output of this stage
changes state. Two options (LM2907-8, LM2917-8) have
one input internally grounded so that an input signal must
swing above and below ground and exceed the input
thresholds to produce an output. This is offered specifically
for magnetic variable reluctance pickups which typically pro-
vide a single-ended ac output. This single input is also fully
protected against voltage swings to g28V, which are easily
attained with these types of pickups.
The differential input options (LM2907, LM2917) give the
user the option of setting his own input switching level and
still have the hysteresis around that level for excellent noise
rejection in any application. Of course in order to allow the
inputs to attain common-mode voltages above ground, input
protection is removed and neither input should be taken
outside the limits of the supply voltage being used. It is very
important that an input not go below ground without some
resistance in its lead to limit the current that will then flow in
the epi-substrate diode.
Following the input stage is the charge pump where the
input frequency is converted to a dc voltage. To do this
requires one timing capacitor, one output resistor, and an
integrating or filter capacitor. When the input stage changes
state (due to a suitable zero crossing or differential voltage
on the input) the timing capacitor is either charged or dis-
charged linearly between two voltages whose difference is
VCC/2. Then in one half cycle of the input frequency or a
time equal to 1/2 fIN the change in charge on the timing
capacitor is equal to VCC/2 cC1. The average amount of
current pumped into or out of the capacitor then is:
DQ
Teic(AVG) eC1 cVCC
2c(2fIN)eVCC cfIN cC1
The output circuit mirrors this current very accurately into
the load resistor R1, connected to ground, such that if the
pulses of current are integrated with a filter capacitor, then
VOeiccR1, and the total conversion equation becomes:
VOeVCC cfIN cC1 cR1 cK
Where K is the gain constantÐtypically 1.0.
The size of C2 is dependent only on the amount of ripple
voltage allowable and the required response time.
CHOOSING R1 AND C1
There are some limitations on the choice of R1 and C1
which should be considered for optimum performance. The
timing capacitor also provides internal compensation for the
charge pump and should be kept larger than 500 pF for very
accurate operation. Smaller values can cause an error cur-
rent on R1, especially at low temperatures. Several consid-
erations must be met when choosing R1. The output current
at pin 3 is internally fixed and therefore VO/R1 must be less
than or equal to this value. If R1 is too large, it can become
a significant fraction of the output impedance at pin 3 which
degrades linearity. Also output ripple voltage must be con-
sidered and the size of C2 is affected by R1. An expression
that describes the ripple content on pin 3 for a single R1C2
combination is:
VRIPPLE eVCC
2cC1
C2 c#1bVCC cfIN cC1
I2Jpk-pk
It appears R1 can be chosen independent of ripple, howev-
er response time, or the time it takes VOUT to stabilize at a
new voltage increases as the size of C2 increases, so a
compromise between ripple, response time, and linearity
must be chosen carefully.
As a final consideration, the maximum attainable input fre-
quency is determined by VCC, C1 and I2:
fMAX eI2
C1 cVCC
USING ZENER REGULATED OPTIONS (LM2917)
For those applications where an output voltage or current
must be obtained independent of supply voltage variations,
the LM2917 is offered. The most important consideration in
choosing a dropping resistor from the unregulated supply to
the device is that the tachometer and op amp circuitry alone
require about 3 mA at the voltage level provided by the
zener. At low supply voltages there must be some current
flowing in the resistor above the 3 mA circuit current to op-
erate the regulator. As an example, if the raw supply varies
from 9V to 16V, a resistance of 470Xwill minimize the ze-
ner voltage variation to 160 mV. If the resistance goes un-
der 400Xor over 600Xthe zener variation quickly rises
above 200 mV for the same input variation.
Typical Applications
Minimum Component Tachometer
TL/H/7942–8
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