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MAX1462 Datasheet, PDF (14/16 Pages) Maxim Integrated Products – Low-Voltage, Low-Power, 16-Bit Smart ADC
Low-Voltage, Low-Power,
16-Bit Smart ADC
Table 9. MAX1462 Conversion Timing
PARAMETER
Sensor Warmup Time
ADC Time
DSP Time
EOC Pulse Width
Conversion Time
SYMBOL
tWARM
tADC
tDSP
tEOC
tCONV
MIN
35
130,585
3220
8
133,805
MAX
—
130,585
3364
8
133,949
UNITS
ms
XIN clk cycles
XIN clk cycles
XIN clk cycles
XIN clk cycles
where
Equation (3)
x = DL − DOFF
DS − DOFF
Equations 2a, 2b, and 2c form a system of three linear
equations, with three unknowns, Of0, Of1, and Of2.
Solve for Of0, Of1, and Of2.
The small sensor excitation versions of equation 1 can
be ratioed to obtain:
Equation (4a)
(YCS − YAS ) + (G1 TAYCS − TCYAS ) +
G2


TA2YCS
−
TC2YAS


=
0
Equation (4b)
(YCS − YBS ) + (G1 TBYCS − TCYBS ) +
G2


TB2YCS
−
TC2YBS


=
0
Equations 4a and 4b form a system of two linear equa-
tions and two unknowns, G1 and G2. Solve for G1 and
G2. Equation 1 can now be readily solved for the last
unknown, Gain.
Arithmetic manipulation can magnify measurement
errors and noise. Quantization of the calibration coeffi-
cients is another reason to consider adjusting the Gain
and DOFF coefficients. To do this, load the MAX1462
registers with the calculated coefficients Gain, G1, G2,
Of0, Of1, Of2, and DOFF. Assuming the oven is still at
temperature C and the S sensor excitation is still
applied, measure the output DCS. Change to the L sen-
sor excitation, and measure DCL. Compute the new
Gain coefficient using equation 6. Remeasure DCL, and
compute the new DOFF coefficient, given by equation 7.
Equation (6)
GAINnew
=
Gain DL
DCL
− DS
− DCS
Equation (7)
DOFFnew = DOFF + DL − DCL
where:
Equation (5a)
YAS
=
SignalAS
DS − DOFF
+ Of0 + Of1TA
+ Of2 TA 2
Equation (5b)
YBS
=
SignalBS
DS − DOFF
+ Of0 + Of1TB
+ Of2 TB2
Equation (5c)
YCS
=
SignalCS
DS − DOFF
+ Of0 + Of1TC
+ Of2 TC2
The final calibration coefficients may now be written
into the MAX1462 EEPROM. The unit is now ready for
final test.
This algorithm minimizes the error directly at the six test
conditions, AS, AL, BS, BL, CS, and CL. Space the
temperatures A, B, and C widely to minimize the SNR
of the measurement. If there is a large error remaining
in the finished product, move the calibration tempera-
tures closer to the peak error temperatures. Similarly,
full-scale sensor excitation may not be the best calibra-
tion condition if the sensor has nonlinearities. Move S
and L away from full scale.
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