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TC7129(2002) View Datasheet(PDF) - Microchip Technology

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Description
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TC7129 Datasheet PDF : 24 Pages
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TC7129
FIGURE 4-6:
TEMPERATURE COMPENSATING CIRCUITS
V+
V+
1N4148
5k
75k
39k
200k
+
24
TC7129
19 VDISP
36 DGND
23
39k
24
20k
2N2222 TC7129
18k
19
VDISP
36
DGND
23
V-
4.8 RC Oscillator
For applications in which 3-1/2 digit (100µV) resolution
is sufficient, an RC oscillator is adequate. A recom-
mended value for the capacitor is 51pF. Other values
can be used as long as they are sufficiently larger than
the circuit parasitic capacitance. The resistor value is
calculated as:
EQUATION 4-1:
R = 0.45
Freq * C
For 120kHz frequency and C = 51pF, the calculated
value of R is 75k. The RC oscillator and the crystal
oscillator circuits are shown in Figure 4-7.
FIGURE 4-7:
OSCILLATOR CIRCUITS
1
5pF
V+
120kHz
40
270k
10pF
TC7129
2
V+
V-
4.9 Measuring Techniques
Two important techniques are used in the TC7129: suc-
cessive integration and digital auto-zeroing. Succes-
sive integration is a refinement to the traditional dual
slope conversion technique.
4.10 Dual Slope Conversion
A dual slope conversion has two basic phases: inte-
grate and de-integrate. During the integrate phase, the
input signal is integrated for a fixed period of time; the
integrated voltage level is thus proportional to the input
voltage. During the de-integrate phase, the integrated
voltage is ramped down at a fixed slope, and a counter
counts the clock cycles until the integrator voltage
crosses zero. The count is a measurement of the time
to ramp the integrated voltage to zero, and is, there-
fore, proportional to the input voltage being measured.
This count can then be scaled and displayed as a mea-
surement of the input voltage. Figure 4-8 shows the
phases of the dual slope conversion.
FIGURE 4-8:
Integrate
DUAL SLOPE
CONVERSION
De-integrate
TC7129
1
40
2
75k
51pF
© 2002 Microchip Technology Inc.
Zero
Crossing
Time
The dual slope method has a fundamental limitation.
The count can only stop on a clock cycle, so that mea-
surement accuracy is limited to the clock frequency. In
addition, a delay in the zero crossing comparator can
add to the inaccuracy. Figure 4-9 shows these errors in
an actual measurement.
DS21459B-page 11

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