The variation of LCD contrast with temperature can become a problem in some
applications. For instance, when working in a meat-packing plant, you might
go from scanning sides of beef in a refrigerated locker to downloading data
from your LCD bar-code reader in a heated office. That type of drastic temperature
change would definitely require an LCD-bias adjustment.
By combining automatic bias adjustment with manual-adjust capability, the
user can compensate for LCD viewing angles and manufacturing differences (Fig.
1). IC1 is a power-supply chip for portable systems, and it includes two
other switching-regulator controllers, plus circuitry for backup=battery switchover,
low-voltage warning, and power-fail reset. When using this setup, the circuit
provides a linear bias change with temperature, from -10 V at 50°C to -15
V at -20°C (Fig. 2).
The automatic compensation is supplied by a negative-temperature coefficient
resistor (R5) that affects the feedback for the LCD-bias-voltage
(V6) regulator in IC1. Decreasing temperature, for example, causes
an increase in R5's resistance and a consequent increase in the V6.
R4 linearizes the effect of R5, and R3 adjusts
the temperature coefficient of R5 to that of the LCD (other temperature
coefficients require different values for R2 and R3.
When calculating R2 and R3, first note that V6
is a function of VD/A and RT. VD/A is the output
of the internal 5-bit DAC, which enables the user to digitally adjust the LCD
bias voltage. Also, RT is the sum of R3 and the parallel
combination of R4 and R5. In equation form, it's as follows:
V6 = VD/A - (5V - VD/A) RT / R2
Therefore,
RT = R2(VD/A - V6)(5 V - VD/A)
Solve for RT at the extremes of V6 (-10V and -15V) using
the midrange value for VD/A (0.625 V): V6 = -10 V, RT
= 2.43R2; V6 = -15 V, RT = 3.57 R2.
Equivalent expressions for RT are based on its definition: V6
= -10 V, RT = R3 + (R5 @ 50°C) || R4;
V6 = -15 V, RT = R3 + (R5 @ -20°C)
|| R4.
From the R5 data sheet, R4 = 277 kΩ (choose 280
k, 1%), R5 @ 50°C = 52.7 kΩ, and R5 @ -20°C
= 250.1 kΩ. With that information, substitute those values in the previous
equations, equate corresponding expressions for RT, and solve for
R2 and R3. As a result, R2 = 172 kΩ (use
169 kΩ, 1%); R3 = 365 kΩ (use 365 kΩ, 1%).