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TMP04 数据表(PDF) 5 Page - Analog Devices

部件名 TMP04
功能描述  Serial Digital Output Thermometers
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制造商  AD [Analog Devices]
网页  http://www.analog.com
标志 AD - Analog Devices

TMP04 数据表(HTML) 5 Page - Analog Devices

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TMP03/TMP04
REV. 0
–5–
Table I. Counter Size and Clock Frequency Effects on Quantization Error
Maximum
Maximum
Maximum
Quantization
Quantization
Count Available
Temp Required
Frequency
Error (+25 C)
Error (+77 F)
4096
+125
°C
94 kHz
0.284
°C
0.512
°F
8192
+125
°C
188 kHz
0.142
°C
0.256
°F
16384
+125
°C
376 kHz
0.071
°C
0.128
°F
Optimizing Counter Characteristics
Counter resolution, clock rate, and the resultant temperature
decode error that occurs using a counter scheme may be
determined from the following calculations:
1. T1 is nominally 10 ms, and compared to T2 is relatively
insensitive to temperature changes. A useful worst-case
assumption is that T1 will never exceed 12 ms over the
specified temperature range.
T1 max = 12 ms
Substituting this value for T1 in the formula, temperature
(
°C) = 235 – ([T1/T2] × 400), yields a maximum value of
T2 of 44 ms at 125
°C. Rearranging the formula allows the
maximum value of T2 to be calculated at any maximum
operating temperature:
T2 (Temp) = (T1max
× 400)/(235 – Temp) in seconds
2. We now need to calculate the maximum clock frequency we
can apply to the gated counter so it will not overflow during
T2 time measurement. The maximum frequency is calculated
using:
Frequency (max) = Counter Size/ (T2 at maximum
temperature)
Substituting in the equation using a 12-bit counter gives,
Fmax = 4096/44 ms
94 kHz.
3. Now we can calculate the temperature resolution, or
quantization error, provided by the counter at the chosen
clock frequency and temperature of interest. Again, using a
12-bit counter being clocked at 90 kHz (to allow for ~5%
temperature over-range), the temperature resolution at
+25
°C is calculated from:
Quantization Error (
°C) = 400 × ([Count1/Count2] –
[Count1 – 1]/[Count2 + 1])
Quantization Error (
°F) = 720 × ([Count1/Count2] –
[Count1 – 1]/[Count2 + 1])
where, Count1 = T1max
× Frequency, and Count2 =
T2 (Temp)
× Frequency. At +25°C this gives a resolution of
better than 0.3
°C. Note that the temperature resolution
calculated from these equations improves as temperature
increases. Higher temperature resolution will be obtained by
employing larger counters as shown in Table I. The internal
quantization error of the TMP03/TMP04 sets a theoretical
minimum resolution of approximately 0.1
°C at +25°C.
Self-Heating Effects
The temperature measurement accuracy of the TMP03/TMP04
may be degraded in some applications due to self-heating.
Errors introduced are from the quiescent dissipation, and power
dissipated by the digital output. The magnitude of these
temperature errors is dependent on the thermal conductivity of
the TMP03/TMP04 package, the mounting technique, and
effects of airflow. Static dissipation in the TMP03/TMP04 is
typically 4.5 mW operating at 5 V with no load. In the TO-92
package mounted in free air, this accounts for a temperature
increase due to self-heating of
∆T = P
DISS × ΘJA = 4.5 mW × 162°C/W = 0.73°C (1.3°F)
For a free-standing surface-mount TSSOP package, the
temperature increase due to self-heating would be
∆T = P
DISS × ΘJA = 4.5 mW × 240°C/W = 1.08°C (1.9°F)
In addition, power is dissipated by the digital output which is
capable of sinking 800
µA continuous (TMP04). Under full
load, the output may dissipate
P
DISS = 0.6 V
() 0.8 mA
() T2
T1
+ T 2


For example with T2 = 20 ms and T1 = 10 ms, the power
dissipation due to the digital output is approximately 0.32 mW
with a 0.8 mA load. In a free-standing TSSOP package this
accounts for a temperature increase due to output self-heating
of
∆T = P
DISS × ΘJA = 0.32 mW × 240°C/W = 0.08°C (0.14°F)
This temperature increase adds directly to that from the
quiescent dissipation and affects the accuracy of the TMP03/
TMP04 relative to the true ambient temperature. Alternatively,
when the same package has been bonded to a large plate or
other thermal mass (effectively a large heatsink) to measure its
temperature, the total self-heating error would be reduced to
approximately
∆T = P
DISS × ΘJC = (4.5 mW + 0.32 mW) × 43°C/W = 0.21°C (0.37°F)
Calibration
The TMP03 and TMP04 are laser-trimmed for accuracy and
linearity during manufacture and, in most cases, no further
adjustments are required. However, some improvement in
performance can be gained by additional system calibration. To
perform a single-point calibration at room temperature, measure
the TMP03/TMP04 output, record the actual measurement
temperature, and modify the offset constant (normally 235; see
the Output Encoding section) as follows:
Offset Constant = 235 + (TOBSERVED – TTMP03OUTPUT)
A more complicated two-point calibration is also possible. This
involves measuring the TMP03/TMP04 output at two temp-
eratures, Temp1 and Temp2, and modifying the slope constant
(normally 400) as follows:
Slope Constant
=
Temp 2
− Temp1
T1@ Temp1
T 2@ Temp1


T1@ Temp 2
T 2@ Temp 2


where T1 and T2 are the output high and output low times,
respectively.


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