**PERFORMANCE OF VARIOUS TYPES OF RESISTORS AT LOW TEMPERATURES**

Test Report

Richard Patterson

NASA Glenn Research Center

&

Ahmad Hammoud

QSS Group, Inc.

&

Scott Gerber

ZIN Technologies

NASA Glenn Research Center

Cleveland, Ohio

August 17, 2001

**Performance of Various Types of Resistors at Low Temperatures**

**Background**

Low temperature electronics find potential application in many of NASA
planetary exploration and deep space missions where extreme temperatures
are encountered. Electronics designed for cryogenic temperature
operation will improve reliability, increase energy density, and extend
the operational lifetimes of space-based electronic systems. Electronic
components needed in the development of NASA advanced power and control
systems for next-generation space missions include, but not limited to,
passive and active devices, power generation and conditioning modules,
and application-specific integrated circuits.

In an effort to address some of these technological challenges, several
types of standard and power resistors were investigated for potential
use in low temperature environments. This work has been performed within
the scope of the NASA Glenn Research Center Low Temperature Electronics
Program and in support of the NASA/JPL Electronic Parts and Packaging
Program (NEPP). The results of this and other research efforts will be
utilized to aid in the proper design and selection of components for the
development of electrical and electronic systems that are geared for low
temperature operation with good reliability and high efficiency.

**Test Setup**

Several types of low to medium power resistors were selected for
evaluation in terms of resistance stability as a function of
temperature. These passive devices included metal film, carbon and
ceramic composition, thin and thick film, wirewound, and power film
resistors. Manufacturer specifications of these resistors are listed in
Table I. Two values of each type of resistor were selected in this
evaluation. These values were 10 (or closest value if unavailable) and 1
k. For each type of resistor, two devices of the same value were
included in this work to confirm certainty and validity of the
performance of the resistor under test. The resistors, which totaled 32
devices, were characterized in terms of their resistance as a function
of temperature in the frequency range of 10 Hz to 500 kHz. Four-wire
measurements were performed on the resistors in the temperature range of
25 C to -190 C. The test temperatures were: 25 C, 0 C, ‑25 C, -50 C, -75
C, -100 C, -125 C, -150 C, -175 C, and -190 C. At a given test
temperature, the device under test was allowed to soak for 20 minutes so
that thermal equilibrium was reached before any measurement was made. A
temperature rate of change of 10 C/min was used throughout this work.
After the last measurement was taken at the lowest temperature, i.e.,
-190 C, data was then obtained at room temperature. Limited thermal
cycling testing was also performed on the resistors. These tests
consisted of subjecting the devices to a total of five thermal cycles
between +25 C and ‑190 C.

**Results and Discussion**

As was mentioned before, two devices of the same value for each type of
resistor were evaluated in this work. These paired devices have shown
exactly the same behavior in their characteristics with temperature.
Therefore, data pertaining to only one of each type of resistor of a
specific value will be presented. Although the characterization of the
resistors was performed as a function of temperature in the frequency
range of 10 Hz to 500 MHz, only the results obtained at a frequency of 1
kHz are presented graphically in this section. Measured values obtained
at all frequencies are, however, tabulated in Appendix A.

Table I. Manufacturer specifications of resistors \[1-5\].

<table>
<colgroup>
<col style="width: 12%" />
<col style="width: 7%" />
<col style="width: 6%" />
<col style="width: 7%" />
<col style="width: 7%" />
<col style="width: 9%" />
<col style="width: 10%" />
<col style="width: 9%" />
<col style="width: 13%" />
<col style="width: 15%" />
</colgroup>
<tbody>
<tr class="odd">
<td><strong>Type</strong></td>
<td><p><strong>Value</strong></p>
<p><strong>()</strong></p></td>
<td><p><strong>Tol.</strong></p>
<p><strong>(%)</strong></p></td>
<td><p><strong>Voltage</strong></p>
<p><strong>(V)</strong></p></td>
<td><p><strong>PWR</strong></p>
<p><strong>(W)</strong></p></td>
<td><p><strong>Temp</strong></p>
<p><strong>(C)</strong></p></td>
<td><p><strong>Temp Coeff</strong></p>
<p><strong>(ppm/C)</strong></p></td>
<td><strong>Package</strong></td>
<td><strong>Manufacturer</strong></td>
<td><strong>Part #</strong></td>
</tr>
<tr class="even">
<td rowspan="2">Metal Film</td>
<td>10</td>
<td>1</td>
<td>250</td>
<td>0.5</td>
<td>-55 to +175</td>
<td>25 to 200</td>
<td>Axial</td>
<td>Vishay/Dale</td>
<td>CMF55C10</td>
</tr>
<tr class="odd">
<td>1K</td>
<td>1</td>
<td>250</td>
<td>0.5</td>
<td>&lt; +170</td>
<td>50</td>
<td>Axial</td>
<td>Vishay</td>
<td>CT551K0FT2</td>
</tr>
<tr class="even">
<td rowspan="2">Wirewound</td>
<td>10</td>
<td>5</td>
<td>495</td>
<td>5</td>
<td>&lt; +350</td>
<td>30</td>
<td>Axial</td>
<td>Ohmite</td>
<td>95J10R</td>
</tr>
<tr class="odd">
<td>1K</td>
<td>5</td>
<td>495</td>
<td>5</td>
<td>&lt; +350</td>
<td>30</td>
<td>Axial</td>
<td>Ohmite</td>
<td>95J10K0</td>
</tr>
<tr class="even">
<td rowspan="2">Thin Film</td>
<td>33</td>
<td>(1 )</td>
<td>200</td>
<td>1.6</td>
<td>-55 to +125</td>
<td>250</td>
<td>Single-in-line</td>
<td>Bourns</td>
<td>4608X-102-330</td>
</tr>
<tr class="odd">
<td>1K</td>
<td>2</td>
<td>200</td>
<td>1.6</td>
<td>-55 to +125</td>
<td>100</td>
<td>Single-in-line</td>
<td>Bourns</td>
<td>4608X-102-102</td>
</tr>
<tr class="even">
<td rowspan="2">Thick Film</td>
<td>100</td>
<td>2</td>
<td>100</td>
<td>0.3</td>
<td>-55 to +125</td>
<td>100</td>
<td>Single-in-line</td>
<td>Dale</td>
<td>CSC08A-03-101G</td>
</tr>
<tr class="odd">
<td>1K</td>
<td>2</td>
<td>100</td>
<td>0.2</td>
<td>-55 to +125</td>
<td>100</td>
<td>Single-in-line</td>
<td>Dale</td>
<td>CSC08A-01-102G</td>
</tr>
<tr class="even">
<td rowspan="2">Carbon Film</td>
<td>10</td>
<td>5</td>
<td>250</td>
<td>0.25</td>
<td>&lt; +155</td>
<td>350</td>
<td>Axial</td>
<td>Ohmite</td>
<td>OK1005</td>
</tr>
<tr class="odd">
<td>1K</td>
<td>5</td>
<td>250</td>
<td>0.25</td>
<td>&lt; +155</td>
<td>-450</td>
<td>Axial</td>
<td>Ohmite</td>
<td>OK1025</td>
</tr>
<tr class="even">
<td rowspan="2"><p>Carbon</p>
<p>Composition</p></td>
<td>15</td>
<td>5</td>
<td>250</td>
<td>0.25</td>
<td>&lt; +130</td>
<td>--</td>
<td>Axial</td>
<td>Ohmite</td>
<td>OD150J</td>
</tr>
<tr class="odd">
<td>1K</td>
<td>5</td>
<td>250</td>
<td>0.25</td>
<td>&lt; +130</td>
<td>--</td>
<td>Axial</td>
<td>Ohmite</td>
<td>OD102J</td>
</tr>
<tr class="even">
<td rowspan="2"><p>Ceramic</p>
<p>Composition</p></td>
<td>10</td>
<td>10</td>
<td>500</td>
<td>1</td>
<td>&lt; +200</td>
<td>-1300300</td>
<td>Axial</td>
<td>Ohmite</td>
<td>OX100K</td>
</tr>
<tr class="odd">
<td>1K</td>
<td>10</td>
<td>500</td>
<td>1</td>
<td>&lt; +200</td>
<td>-1300300</td>
<td>Axial</td>
<td>Ohmite</td>
<td>OX102K</td>
</tr>
<tr class="even">
<td rowspan="2">Power Film</td>
<td>10</td>
<td>1</td>
<td>300</td>
<td>20</td>
<td>-55 to +175</td>
<td>-20 to +50</td>
<td>TO-220</td>
<td>Caddock</td>
<td>MP820-10.0-1</td>
</tr>
<tr class="odd">
<td>1K</td>
<td>1</td>
<td>300</td>
<td>20</td>
<td>-55 to +175</td>
<td>-20 to +50</td>
<td>TO-220</td>
<td>Caddock</td>
<td>MP820-1.0K-1</td>
</tr>
</tbody>
</table>

Figure 1 shows the resistance and the percentage change of the 10 metal
film resistor as a function of temperature. It can be clearly seen that
this resistor had shown excellent stability with temperature as its
value remained steady throughout the test temperature range. The 1 k
version of this type of resistor, however, exhibited a gradual, but very
slight, increase in resistance as temperature was decreased. This
increase in resistance amounted to only about 0.3% at -- 190 C, as shown
in Figure 2.

![](media/image1.wmf){width="6.442361111111111in"
height="2.401388888888889in"}

Figure 1. Resistance & percentage change of 10 metal film resistor
versus temperature @ 1 kHz.

![](media/image2.wmf){width="6.5680555555555555in"
height="2.401388888888889in"}

Figure 2. Resistance & percentage change of 1 k metal film resistor
versus temperature @ 1 kHz.

The resistance and the percentage change of both the 10 and the 1 k
wirewound resistors are shown as a function of temperature in Figures 3
and 4, respectively. Both resistors seemed to exhibit very slight
decrease in their resistance as temperature was decreased. The drop in
the resistance at --190 C for the 10 resistor was about 1%, while that
of the 1 k resistor reached only 0.6%.

![](media/image3.wmf){width="6.442361111111111in"
height="2.401388888888889in"}

Figure 3. Resistance & percentage change of 10 wirewound resistor versus
temperature @ 1 kHz.

![](media/image4.wmf){width="6.5680555555555555in"
height="2.401388888888889in"}

Figure 4. Resistance & percentage change of 1 k wirewound resistor
versus temperature @ 1 kHz.

Figures 5 and 6 show the resistance and the percentage change of the 33
and the 1 k thin film resistors, respectively. Unlike the wirewound
resistors, these types of resistors experienced an increase in their
resistance with decrease in temperature. While this increase approached
only 3.8% for the 33 resistor at the extreme low temperature, it did not
exceed 1.4% for the higher value resistor.

![](media/image5.wmf){width="6.442361111111111in"
height="2.401388888888889in"}

Figure 5. Resistance & percentage change of 33 thin film resistor versus
temperature @ 1 kHz.

![](media/image6.wmf){width="6.5680555555555555in"
height="2.401388888888889in"}

Figure 6. Resistance & percentage change of 1 k thin film resistor
versus temperature @ 1 kHz.

The resistance and the percentage change of the 100 thick film resistor
as a function of temperature are shown in Figure 7. It can be seen that
the resistance underwent an increase as the test temperature was
decreased. At --190 C, for example, this increase amounted to about
5.5%. Although the 1 k resistor displayed a trend similar to that of the
100 resistor with temperature, as shown in Figure 8, its increase in
resistance, however, did not exceed 0.5% at the lowest temperature.

![](media/image7.wmf){width="6.504861111111111in"
height="2.401388888888889in"}

Figure 7. Resistance & percentage change of 100 thick film resistor
versus temperature @ 1 kHz.

![](media/image8.wmf){width="6.668055555555555in"
height="2.401388888888889in"}

Figure 8. Resistance & percentage change of 1 k thick film resistor
versus temperature @ 1 kHz.

Figures 9 and 10 show the resistance and the percentage change of the 10
and the 1 k carbon film resistors, respectively. Both of these resistors
showed exact behavior with temperature as their resistance increased
gradually as the temperature was decreased. The increase in the
resistance, for either resistor, amounted to little over 5% at
temperature of --190 C.

![](media/image9.wmf){width="6.442361111111111in"
height="2.401388888888889in"}

Figure 9. Resistance & percentage change of 10 carbon film resistor
versus temperature @ 1 kHz.

![](media/image10.wmf){width="6.5680555555555555in"
height="2.401388888888889in"}

Figure 10. Resistance & percentage change of 1 k carbon film resistor
versus temperature @ 1 kHz.

Similar to their film counterpart, the carbon composition resistors also
exhibited an increase in resistance as the test temperature was reduced,
as shown in Figures 11 and 12. The increase in resistance, however, is
more significant as it approached 12% for the 15 resistor, while it fell
in the vicinity of 28% for the 1 k device. Both of these occurred at the
lowest test temperature of -- 190 C.

![](media/image11.wmf){width="6.442361111111111in"
height="2.401388888888889in"}

Figure 11. Resistance & percentage change of 15 carbon composition
resistor versus temperature @ 1 kHz.

![](media/image12.wmf){width="6.5680555555555555in"
height="2.401388888888889in"}

Figure 12. Resistance & percentage change of 1 k carbon composition
resistor versus temperature @ 1 kHz.

The behavior of the ceramic composition resistors with temperature
seemed to resemble that of the carbon composition resistors in terms of
change polarity and magnitude. The 10 as well as the 1 k ceramic
composition resistors experienced appreciable change in their resistance
values as temperature was decreased as shown in Figures 13 and 14,
respectively. The increase in the resistance, for either resistor, was
about 16% at the extreme low temperature.

![](media/image13.wmf){width="6.4222222222222225in"
height="2.401388888888889in"}

Figure 13. Resistance & percentage change of 10 ceramic composition
resistor versus temperature \@1kHz.

![](media/image14.wmf){width="6.5680555555555555in"
height="2.401388888888889in"}

Figure 14. Resistance & percentage change of 1 k ceramic composition
resistor versus temperature \@1kHz.

Both power film resistors exhibited an increase in their resistance with
decreasing temperature as shown in Figures 15 and 16. The magnitude of
this resistance increase occurring at -- 190 C, for either one of these
two resistors, was in the range between 4% and 5%.

![](media/image15.wmf){width="6.442361111111111in"
height="2.401388888888889in"}

Figure 15. Resistance & percentage change of 10 power film resistor
versus temperature @ 1 kHz.

![](media/image16.wmf){width="6.668055555555555in"
height="2.401388888888889in"}

Figure 16. Resistance & percentage change of 1 k power film resistor
versus temperature @ 1 kHz.

The resistance and percentage change occurring at --190 C for all
resistors are shown in Table II. Also listed are the resistors
manufacturer specified values as well as the values measured at room
temperature. It can be clearly seen that the metal film, wire wound, and
thin film resistors have displayed excellent stability in their
resistance with change in temperature. Both the carbon and the ceramic
composition resistors, on the other hand, have exhibited significant
increase in their resistance as the test temperature was decreased. The
low temperature-induced changes exhibited by the three remaining types
of resistors, which were film-based, i.e. power, thick, and carbon,
investigated in this work were not as severe and their performance was
in between the other two groups. Table III gives a graphical
illustration of the resistor type and the corresponding change in
resistance at the extreme low temperature of --190 C.

Table II. Resistance and percentage change at --190 C (@ 1 kHz).

+------------+------+-------------+-------------+--------------------+
| **Type**   | *    | *           | *           | **Change in        |
|            | *Val | *Resistance | *Resistance | Resistance (%)**   |
|            | ue** | ()**        | ()**        |                    |
|            |      |             |             | **at -190 C**      |
|            | **   | **at 25 C** | **at -190   |                    |
|            | ()** |             | C**         |                    |
+------------+------+-------------+-------------+--------------------+
| Metal Film | 10   | 10.00       | 9.99        | 0.0                |
+------------+------+-------------+-------------+--------------------+
|            | 1K   | 999.15      | 1001.86     | 0.3                |
+------------+------+-------------+-------------+--------------------+
| Wirewound  | 10   | 9.70        | 9.62        | -0.9               |
+------------+------+-------------+-------------+--------------------+
|            | 1K   | 984.80      | 979.31      | -0.6               |
+------------+------+-------------+-------------+--------------------+
| Thin Film  | 33   | 33.07       | 34.32       | 3.8                |
+------------+------+-------------+-------------+--------------------+
|            | 1K   | 995.41      | 1007.88     | 1.3                |
+------------+------+-------------+-------------+--------------------+
| Thick Film | 100  | 99.99       | 105.42      | 5.4                |
+------------+------+-------------+-------------+--------------------+
|            | 1K   | 998.70      | 1003.22     | 0.5                |
+------------+------+-------------+-------------+--------------------+
| Carbon     | 10   | 9.96        | 10.46       | 5.1                |
| Film       |      |             |             |                    |
+------------+------+-------------+-------------+--------------------+
|            | 1K   | 980.30      | 1035.83     | 5.7                |
+------------+------+-------------+-------------+--------------------+
| Carbon     | 15   | 14.65       | 16.34       | 11.6               |
|            |      |             |             |                    |
| C          |      |             |             |                    |
| omposition |      |             |             |                    |
+------------+------+-------------+-------------+--------------------+
|            | 1K   | 1013.29     | 1296.54     | 28.0               |
+------------+------+-------------+-------------+--------------------+
| Ceramic    | 10   | 9.49        | 10.99       | 15.8               |
|            |      |             |             |                    |
| C          |      |             |             |                    |
| omposition |      |             |             |                    |
+------------+------+-------------+-------------+--------------------+
|            | 1K   | 993.09      | 1167.51     | 17.6               |
+------------+------+-------------+-------------+--------------------+
| Power Film | 10   | 10.00       | 10.48       | 4.9                |
+------------+------+-------------+-------------+--------------------+
|            | 1K   | 996.20      | 1037.06     | 4.1                |
+------------+------+-------------+-------------+--------------------+

Table III. Percent change in resistance at --190 C versus resistor type.

![](media/image17.wmf){width="5.413194444444445in"
height="3.3229166666666665in"}

To determine the effect of extended low temperature exposure, the
resistors were subjected to limited thermal cycling. The devices were
thermally cycled for a total of five cycles in the temperature range of
25 C to ‑190 C. As with the previous tests, a temperature rate of 10
C/min was used with a soak time of 20 minutes at both the room and the
‑190 C temperatures. The values of the resistance of all resistors at
room temperature, for both the pre-cycling and post-cycling conditions,
are listed in Table IV. It can be clearly seen that all resistors
exhibited no change due to this limited thermal cycling as they retained
their resistance values.

Table IV. Resistance before and after five thermal cycles (@ 1 kHz).

+-----------------+------------+-----------------+--------------------+
|                 |            | **Resistance () |                    |
|                 |            | at 25 C**       |                    |
+-----------------+------------+-----------------+--------------------+
| **Type**        | **Value    | **Pre-cycling** | **Post-cycling**   |
|                 | ()**       |                 |                    |
+-----------------+------------+-----------------+--------------------+
| Metal Film      | 10         | 10.00           | 10.00              |
+-----------------+------------+-----------------+--------------------+
|                 | 1K         | 999.15          | 999.30             |
+-----------------+------------+-----------------+--------------------+
| Wirewound       | 10         | 9.70            | 9.70               |
+-----------------+------------+-----------------+--------------------+
|                 | 1K         | 984.80          | 984.79             |
+-----------------+------------+-----------------+--------------------+
| Thin Film       | 33         | 33.07           | 33.06              |
+-----------------+------------+-----------------+--------------------+
|                 | 1K         | 995.41          | 995.01             |
+-----------------+------------+-----------------+--------------------+
| Thick Film      | 100        | 99.99           | 99.98              |
+-----------------+------------+-----------------+--------------------+
|                 | 1K         | 998.70          | 998.68             |
+-----------------+------------+-----------------+--------------------+
| Carbon Film     | 10         | 9.96            | 9.96               |
+-----------------+------------+-----------------+--------------------+
|                 | 1K         | 980.30          | 980.13             |
+-----------------+------------+-----------------+--------------------+
| Carbon          | 15         | 14.65           | 14.78              |
|                 |            |                 |                    |
| Composition     |            |                 |                    |
+-----------------+------------+-----------------+--------------------+
|                 | 1K         | 1013.29         | 1015.93            |
+-----------------+------------+-----------------+--------------------+
| Ceramic         | 10         | 9.96            | 9.95               |
|                 |            |                 |                    |
| Composition     |            |                 |                    |
+-----------------+------------+-----------------+--------------------+
|                 | 1K         | 993.09          | 992.31             |
+-----------------+------------+-----------------+--------------------+
| Power Film      | 10         | 10.00           | 9.99               |
+-----------------+------------+-----------------+--------------------+
|                 | 1K         | 996.20          | 996.01             |
+-----------------+------------+-----------------+--------------------+

**Conclusion**

Passive as well as active electronic components capable of low
temperature operation constitute a key requirement for the development
of advanced and reliable power and communication systems for space
applications. Eight types of resistors were investigated in this work
for their potential use in extreme temperature environments. T he
resistors were characterized in terms of their resistance stability
between 25 C and --190 C in the frequency range of 20 Hz to 500 kHz.
Limited thermal cycling was also performed on the resistors in the same
temperature range. While some of these resistors showed excellent
stability with temperature, others did not fare as well. More
comprehensive testing, however, is required to fully characterize the
behavior of these and other devices to determine their suitability and
limitation in low temperature environments. Issues such as thermal
cycling under long-term exposure and multi-stress conditions will need
to be carried out for a complete assessment of the performance and
reliability of these devices.

**References**

1\. Vishay resistor data sheet.

2\. Dale resistor data sheet.

3\. Ohmite resistor data sheet.

4\. Bourns resistor data sheet.

5\. Caddock resistor data sheet.

**Acknowledgments**

This work has been performed at the NASA Glenn Research Center under
GESS Contract \# NAS3-00142. Support was also provided by the Jet
Propulsion Laboratory through the NASA Electronic Parts and Packaging
(NEPP) Program.

**Appendix A**

Detailed experimental results obtained on all resistor types
investigated in this work are listed in this appendix. The data
represents the measured resistance of a specific resistor in the
frequency range of 10 Hz to 500 kHz at a given test temperature. Room
temperature measurement of the resistance obtained after the five
thermal cycles (post) is also listed in the tables.

Table A-I. Resistance measurements for 10 metal film resistor as a
function of frequency and temperature.

<table>
<colgroup>
<col style="width: 8%" />
<col style="width: 8%" />
<col style="width: 8%" />
<col style="width: 8%" />
<col style="width: 8%" />
<col style="width: 8%" />
<col style="width: 8%" />
<col style="width: 8%" />
<col style="width: 8%" />
<col style="width: 8%" />
<col style="width: 8%" />
<col style="width: 8%" />
</colgroup>
<tbody>
<tr class="odd">
<td></td>
<td colspan="11"><strong>Temperature</strong></td>
</tr>
<tr class="even">
<td><strong>Freq. (Hz)</strong></td>
<td><strong>25C</strong></td>
<td><strong>0C</strong></td>
<td><strong>-25C</strong></td>
<td><strong>-50C</strong></td>
<td><strong>-75C</strong></td>
<td><strong>-100C</strong></td>
<td><strong>-125C</strong></td>
<td><strong>-150C</strong></td>
<td><strong>-175C</strong></td>
<td><strong>-190C</strong></td>
<td><p><strong>25C</strong></p>
<p><strong>post</strong></p></td>
</tr>
<tr class="odd">
<td><strong>10</strong></td>
<td>9.997</td>
<td>9.998</td>
<td>9.998</td>
<td>9.997</td>
<td>9.997</td>
<td>9.996</td>
<td>9.995</td>
<td>9.994</td>
<td>9.994</td>
<td>9.993</td>
<td>9.997</td>
</tr>
<tr class="even">
<td><strong>50</strong></td>
<td>9.997</td>
<td>9.997</td>
<td>9.997</td>
<td>9.997</td>
<td>9.997</td>
<td>9.996</td>
<td>9.995</td>
<td>9.994</td>
<td>9.993</td>
<td>9.993</td>
<td>9.997</td>
</tr>
<tr class="odd">
<td><strong>100</strong></td>
<td>9.997</td>
<td>9.997</td>
<td>9.997</td>
<td>9.997</td>
<td>9.997</td>
<td>9.996</td>
<td>9.995</td>
<td>9.994</td>
<td>9.993</td>
<td>9.993</td>
<td>9.997</td>
</tr>
<tr class="even">
<td><strong>200</strong></td>
<td>9.996</td>
<td>9.997</td>
<td>9.997</td>
<td>9.997</td>
<td>9.996</td>
<td>9.995</td>
<td>9.994</td>
<td>9.994</td>
<td>9.993</td>
<td>9.993</td>
<td>9.996</td>
</tr>
<tr class="odd">
<td><strong>500</strong></td>
<td>9.996</td>
<td>9.997</td>
<td>9.997</td>
<td>9.996</td>
<td>9.996</td>
<td>9.995</td>
<td>9.994</td>
<td>9.993</td>
<td>9.993</td>
<td>9.993</td>
<td>9.996</td>
</tr>
<tr class="even">
<td><strong>1K</strong></td>
<td>9.996</td>
<td>9.997</td>
<td>9.997</td>
<td>9.997</td>
<td>9.996</td>
<td>9.996</td>
<td>9.995</td>
<td>9.994</td>
<td>9.993</td>
<td>9.993</td>
<td>9.997</td>
</tr>
<tr class="odd">
<td><strong>2K</strong></td>
<td>9.996</td>
<td>9.997</td>
<td>9.997</td>
<td>9.997</td>
<td>9.996</td>
<td>9.995</td>
<td>9.994</td>
<td>9.994</td>
<td>9.993</td>
<td>9.993</td>
<td>9.996</td>
</tr>
<tr class="even">
<td><strong>5K</strong></td>
<td>9.996</td>
<td>9.997</td>
<td>9.997</td>
<td>9.996</td>
<td>9.996</td>
<td>9.995</td>
<td>9.994</td>
<td>9.993</td>
<td>9.993</td>
<td>9.992</td>
<td>9.996</td>
</tr>
<tr class="odd">
<td><strong>10K</strong></td>
<td>9.997</td>
<td>9.998</td>
<td>9.998</td>
<td>9.997</td>
<td>9.997</td>
<td>9.996</td>
<td>9.995</td>
<td>9.994</td>
<td>9.993</td>
<td>9.993</td>
<td>9.997</td>
</tr>
<tr class="even">
<td><strong>20K</strong></td>
<td>9.997</td>
<td>9.997</td>
<td>9.997</td>
<td>9.997</td>
<td>9.996</td>
<td>9.996</td>
<td>9.995</td>
<td>9.994</td>
<td>9.993</td>
<td>9.993</td>
<td>9.997</td>
</tr>
<tr class="odd">
<td><strong>50K</strong></td>
<td>9.997</td>
<td>9.997</td>
<td>9.997</td>
<td>9.997</td>
<td>9.996</td>
<td>9.996</td>
<td>9.995</td>
<td>9.994</td>
<td>9.993</td>
<td>9.993</td>
<td>9.997</td>
</tr>
<tr class="even">
<td><strong>100K</strong></td>
<td>9.996</td>
<td>9.996</td>
<td>9.996</td>
<td>9.996</td>
<td>9.996</td>
<td>9.995</td>
<td>9.994</td>
<td>9.993</td>
<td>9.993</td>
<td>9.992</td>
<td>9.996</td>
</tr>
<tr class="odd">
<td><strong>200K</strong></td>
<td>9.996</td>
<td>9.997</td>
<td>9.997</td>
<td>9.997</td>
<td>9.996</td>
<td>9.995</td>
<td>9.995</td>
<td>9.993</td>
<td>9.993</td>
<td>9.992</td>
<td>9.995</td>
</tr>
<tr class="even">
<td><strong>500K</strong></td>
<td>9.993</td>
<td>9.997</td>
<td>9.996</td>
<td>9.996</td>
<td>9.995</td>
<td>9.994</td>
<td>9.994</td>
<td>9.992</td>
<td>9.992</td>
<td>9.990</td>
<td>9.992</td>
</tr>
</tbody>
</table>

Table A-II. Resistance measurements for 1 k metal film resistor as a
function of frequency and temperature.

<table>
<colgroup>
<col style="width: 8%" />
<col style="width: 8%" />
<col style="width: 8%" />
<col style="width: 8%" />
<col style="width: 8%" />
<col style="width: 8%" />
<col style="width: 8%" />
<col style="width: 8%" />
<col style="width: 8%" />
<col style="width: 8%" />
<col style="width: 8%" />
<col style="width: 8%" />
</colgroup>
<tbody>
<tr class="odd">
<td></td>
<td colspan="11"><strong>Temperature</strong></td>
</tr>
<tr class="even">
<td><strong>Freq. (Hz)</strong></td>
<td><strong>25C</strong></td>
<td><strong>0C</strong></td>
<td><strong>-25C</strong></td>
<td><strong>-50C</strong></td>
<td><strong>-75C</strong></td>
<td><strong>-100C</strong></td>
<td><strong>-125C</strong></td>
<td><strong>-150C</strong></td>
<td><strong>-175C</strong></td>
<td><strong>-190C</strong></td>
<td><p><strong>25C</strong></p>
<p><strong>post</strong></p></td>
</tr>
<tr class="odd">
<td><strong>10</strong></td>
<td>999.17</td>
<td>999.29</td>
<td>999.45</td>
<td>999.66</td>
<td>999.91</td>
<td>1000.21</td>
<td>1000.58</td>
<td>1001.03</td>
<td>1001.57</td>
<td>1001.85</td>
<td>999.27</td>
</tr>
<tr class="even">
<td><strong>50</strong></td>
<td>999.14</td>
<td>999.26</td>
<td>999.43</td>
<td>999.63</td>
<td>999.87</td>
<td>1000.18</td>
<td>1000.54</td>
<td>1001.01</td>
<td>1001.53</td>
<td>1001.80</td>
<td>999.24</td>
</tr>
<tr class="odd">
<td><strong>100</strong></td>
<td>999.12</td>
<td>999.23</td>
<td>999.41</td>
<td>999.61</td>
<td>999.86</td>
<td>1000.17</td>
<td>1000.53</td>
<td>1000.99</td>
<td>1001.51</td>
<td>1001.80</td>
<td>999.23</td>
</tr>
<tr class="even">
<td><strong>200</strong></td>
<td>999.12</td>
<td>999.25</td>
<td>999.42</td>
<td>999.61</td>
<td>999.86</td>
<td>1000.16</td>
<td>1000.56</td>
<td>1000.98</td>
<td>1001.51</td>
<td>1001.80</td>
<td>999.22</td>
</tr>
<tr class="odd">
<td><strong>500</strong></td>
<td>999.13</td>
<td>999.25</td>
<td>999.41</td>
<td>999.61</td>
<td>999.86</td>
<td>1000.17</td>
<td>1000.56</td>
<td>1000.99</td>
<td>1001.52</td>
<td>1001.81</td>
<td>999.24</td>
</tr>
<tr class="even">
<td><strong>1K</strong></td>
<td>999.15</td>
<td>999.26</td>
<td>999.42</td>
<td>999.64</td>
<td>999.90</td>
<td>1000.18</td>
<td>1000.55</td>
<td>1001.02</td>
<td>1001.57</td>
<td>1001.86</td>
<td>999.30</td>
</tr>
<tr class="odd">
<td><strong>2K</strong></td>
<td>999.15</td>
<td>999.28</td>
<td>999.46</td>
<td>999.65</td>
<td>999.89</td>
<td>1000.20</td>
<td>1000.58</td>
<td>1001.00</td>
<td>1001.55</td>
<td>1001.81</td>
<td>999.27</td>
</tr>
<tr class="even">
<td><strong>5K</strong></td>
<td>999.16</td>
<td>999.30</td>
<td>999.47</td>
<td>999.66</td>
<td>999.91</td>
<td>1000.22</td>
<td>1000.58</td>
<td>1001.01</td>
<td>1001.55</td>
<td>1001.81</td>
<td>999.28</td>
</tr>
<tr class="odd">
<td><strong>10K</strong></td>
<td>999.14</td>
<td>999.28</td>
<td>999.45</td>
<td>999.64</td>
<td>999.87</td>
<td>1000.18</td>
<td>1000.54</td>
<td>1001.01</td>
<td>1001.51</td>
<td>1001.77</td>
<td>999.28</td>
</tr>
<tr class="even">
<td><strong>20K</strong></td>
<td>999.08</td>
<td>999.20</td>
<td>999.38</td>
<td>999.56</td>
<td>999.80</td>
<td>1000.10</td>
<td>1000.47</td>
<td>1000.92</td>
<td>1001.45</td>
<td>1001.73</td>
<td>999.20</td>
</tr>
<tr class="odd">
<td><strong>50K</strong></td>
<td>998.95</td>
<td>999.08</td>
<td>999.22</td>
<td>999.43</td>
<td>999.63</td>
<td>999.93</td>
<td>1000.24</td>
<td>1000.67</td>
<td>1001.17</td>
<td>1001.42</td>
<td>999.09</td>
</tr>
<tr class="even">
<td><strong>100K</strong></td>
<td>998.61</td>
<td>998.75</td>
<td>998.70</td>
<td>998.90</td>
<td>999.09</td>
<td>999.25</td>
<td>999.64</td>
<td>999.88</td>
<td>1000.43</td>
<td>1000.36</td>
<td>998.84</td>
</tr>
<tr class="odd">
<td><strong>200K</strong></td>
<td>1001.19</td>
<td>1000.95</td>
<td>1000.78</td>
<td>1000.71</td>
<td>1000.48</td>
<td>1000.40</td>
<td>1000.27</td>
<td>1000.09</td>
<td>1000.24</td>
<td>1000.06</td>
<td>998.56</td>
</tr>
<tr class="even">
<td><strong>500K</strong></td>
<td>1009.80</td>
<td>1008.03</td>
<td>1006.29</td>
<td>1004.25</td>
<td>1002.51</td>
<td>1000.81</td>
<td>997.86</td>
<td>995.82</td>
<td>993.32</td>
<td>990.36</td>
<td>989.46</td>
</tr>
</tbody>
</table>

Table A-III. Resistance measurements for 10 wirewound resistor as a
function of frequency and temperature.

<table>
<colgroup>
<col style="width: 8%" />
<col style="width: 8%" />
<col style="width: 8%" />
<col style="width: 8%" />
<col style="width: 8%" />
<col style="width: 8%" />
<col style="width: 8%" />
<col style="width: 8%" />
<col style="width: 8%" />
<col style="width: 8%" />
<col style="width: 8%" />
<col style="width: 8%" />
</colgroup>
<tbody>
<tr class="odd">
<td></td>
<td colspan="11"><strong>Temperature</strong></td>
</tr>
<tr class="even">
<td><strong>Freq. (Hz)</strong></td>
<td><strong>25C</strong></td>
<td><strong>0C</strong></td>
<td><strong>-25C</strong></td>
<td><strong>-50C</strong></td>
<td><strong>-75C</strong></td>
<td><strong>-100C</strong></td>
<td><strong>-125C</strong></td>
<td><strong>-150C</strong></td>
<td><strong>-175C</strong></td>
<td><strong>-190C</strong></td>
<td><p><strong>25C</strong></p>
<p><strong>post</strong></p></td>
</tr>
<tr class="odd">
<td><strong>10</strong></td>
<td>9.703</td>
<td>9.698</td>
<td>9.692</td>
<td>9.685</td>
<td>9.676</td>
<td>9.666</td>
<td>9.655</td>
<td>9.641</td>
<td>9.626</td>
<td>9.618</td>
<td>9.703</td>
</tr>
<tr class="even">
<td><strong>50</strong></td>
<td>9.702</td>
<td>9.698</td>
<td>9.692</td>
<td>9.684</td>
<td>9.675</td>
<td>9.666</td>
<td>9.654</td>
<td>9.640</td>
<td>9.625</td>
<td>9.617</td>
<td>9.702</td>
</tr>
<tr class="odd">
<td><strong>100</strong></td>
<td>9.702</td>
<td>9.698</td>
<td>9.692</td>
<td>9.684</td>
<td>9.675</td>
<td>9.666</td>
<td>9.654</td>
<td>9.640</td>
<td>9.625</td>
<td>9.617</td>
<td>9.702</td>
</tr>
<tr class="even">
<td><strong>200</strong></td>
<td>9.702</td>
<td>9.697</td>
<td>9.691</td>
<td>9.684</td>
<td>9.675</td>
<td>9.665</td>
<td>9.653</td>
<td>9.640</td>
<td>9.625</td>
<td>9.617</td>
<td>9.701</td>
</tr>
<tr class="odd">
<td><strong>500</strong></td>
<td>9.702</td>
<td>9.697</td>
<td>9.691</td>
<td>9.683</td>
<td>9.675</td>
<td>9.665</td>
<td>9.653</td>
<td>9.640</td>
<td>9.625</td>
<td>9.617</td>
<td>9.701</td>
</tr>
<tr class="even">
<td><strong>1K</strong></td>
<td>9.702</td>
<td>9.698</td>
<td>9.691</td>
<td>9.684</td>
<td>9.675</td>
<td>9.665</td>
<td>9.654</td>
<td>9.641</td>
<td>9.625</td>
<td>9.618</td>
<td>9.701</td>
</tr>
<tr class="odd">
<td><strong>2K</strong></td>
<td>9.702</td>
<td>9.697</td>
<td>9.691</td>
<td>9.684</td>
<td>9.675</td>
<td>9.665</td>
<td>9.654</td>
<td>9.640</td>
<td>9.625</td>
<td>9.617</td>
<td>9.702</td>
</tr>
<tr class="even">
<td><strong>5K</strong></td>
<td>9.702</td>
<td>9.698</td>
<td>9.692</td>
<td>9.684</td>
<td>9.676</td>
<td>9.666</td>
<td>9.654</td>
<td>9.641</td>
<td>9.625</td>
<td>9.618</td>
<td>9.702</td>
</tr>
<tr class="odd">
<td><strong>10K</strong></td>
<td>9.705</td>
<td>9.700</td>
<td>9.694</td>
<td>9.686</td>
<td>9.678</td>
<td>9.667</td>
<td>9.656</td>
<td>9.642</td>
<td>9.627</td>
<td>9.619</td>
<td>9.704</td>
</tr>
<tr class="even">
<td><strong>20K</strong></td>
<td>9.706</td>
<td>9.702</td>
<td>9.695</td>
<td>9.687</td>
<td>9.679</td>
<td>9.669</td>
<td>9.657</td>
<td>9.643</td>
<td>9.628</td>
<td>9.620</td>
<td>9.706</td>
</tr>
<tr class="odd">
<td><strong>50K</strong></td>
<td>9.710</td>
<td>9.705</td>
<td>9.699</td>
<td>9.691</td>
<td>9.682</td>
<td>9.672</td>
<td>9.660</td>
<td>9.646</td>
<td>9.630</td>
<td>9.622</td>
<td>9.710</td>
</tr>
<tr class="even">
<td><strong>100K</strong></td>
<td>9.714</td>
<td>9.709</td>
<td>9.702</td>
<td>9.694</td>
<td>9.685</td>
<td>9.674</td>
<td>9.662</td>
<td>9.648</td>
<td>9.633</td>
<td>9.624</td>
<td>9.713</td>
</tr>
<tr class="odd">
<td><strong>200K</strong></td>
<td>9.721</td>
<td>9.716</td>
<td>9.709</td>
<td>9.701</td>
<td>9.691</td>
<td>9.680</td>
<td>9.667</td>
<td>9.653</td>
<td>9.638</td>
<td>9.629</td>
<td>9.721</td>
</tr>
<tr class="even">
<td><strong>500K</strong></td>
<td>9.740</td>
<td>9.735</td>
<td>9.725</td>
<td>9.717</td>
<td>9.704</td>
<td>9.691</td>
<td>9.678</td>
<td>9.665</td>
<td>9.648</td>
<td>9.638</td>
<td>9.737</td>
</tr>
</tbody>
</table>

Table A-IV. Resistance measurements for 1 k wirewound resistor as a
function of frequency and temperature.

<table>
<colgroup>
<col style="width: 8%" />
<col style="width: 8%" />
<col style="width: 8%" />
<col style="width: 8%" />
<col style="width: 8%" />
<col style="width: 8%" />
<col style="width: 8%" />
<col style="width: 8%" />
<col style="width: 8%" />
<col style="width: 8%" />
<col style="width: 8%" />
<col style="width: 8%" />
</colgroup>
<tbody>
<tr class="odd">
<td></td>
<td colspan="11"><strong>Temperature</strong></td>
</tr>
<tr class="even">
<td><strong>Freq. (Hz)</strong></td>
<td><strong>25C</strong></td>
<td><strong>0C</strong></td>
<td><strong>-25C</strong></td>
<td><strong>-50C</strong></td>
<td><strong>-75C</strong></td>
<td><strong>-100C</strong></td>
<td><strong>-125C</strong></td>
<td><strong>-150C</strong></td>
<td><strong>-175C</strong></td>
<td><strong>-190C</strong></td>
<td><p><strong>25C</strong></p>
<p><strong>post</strong></p></td>
</tr>
<tr class="odd">
<td><strong>10</strong></td>
<td>984.86</td>
<td>984.63</td>
<td>984.32</td>
<td>983.90</td>
<td>983.37</td>
<td>982.73</td>
<td>981.97</td>
<td>981.07</td>
<td>979.98</td>
<td>979.37</td>
<td>984.84</td>
</tr>
<tr class="even">
<td><strong>50</strong></td>
<td>984.81</td>
<td>984.57</td>
<td>984.26</td>
<td>983.82</td>
<td>983.30</td>
<td>982.66</td>
<td>981.90</td>
<td>980.99</td>
<td>979.90</td>
<td>979.28</td>
<td>984.79</td>
</tr>
<tr class="odd">
<td><strong>100</strong></td>
<td>984.79</td>
<td>984.56</td>
<td>984.24</td>
<td>983.82</td>
<td>983.29</td>
<td>982.64</td>
<td>981.89</td>
<td>980.96</td>
<td>979.90</td>
<td>979.28</td>
<td>984.77</td>
</tr>
<tr class="even">
<td><strong>200</strong></td>
<td>984.79</td>
<td>984.56</td>
<td>984.25</td>
<td>983.82</td>
<td>983.31</td>
<td>982.66</td>
<td>981.90</td>
<td>980.97</td>
<td>979.90</td>
<td>979.29</td>
<td>984.78</td>
</tr>
<tr class="odd">
<td><strong>500</strong></td>
<td>984.80</td>
<td>984.57</td>
<td>984.24</td>
<td>983.82</td>
<td>983.31</td>
<td>982.64</td>
<td>981.89</td>
<td>980.96</td>
<td>979.89</td>
<td>979.28</td>
<td>984.78</td>
</tr>
<tr class="even">
<td><strong>1K</strong></td>
<td>984.80</td>
<td>984.62</td>
<td>984.28</td>
<td>983.83</td>
<td>983.33</td>
<td>982.71</td>
<td>981.92</td>
<td>981.02</td>
<td>979.91</td>
<td>979.31</td>
<td>984.79</td>
</tr>
<tr class="odd">
<td><strong>2K</strong></td>
<td>984.83</td>
<td>984.61</td>
<td>984.27</td>
<td>983.86</td>
<td>983.34</td>
<td>982.70</td>
<td>981.92</td>
<td>980.99</td>
<td>979.92</td>
<td>979.31</td>
<td>984.81</td>
</tr>
<tr class="even">
<td><strong>5K</strong></td>
<td>984.84</td>
<td>984.62</td>
<td>984.28</td>
<td>983.86</td>
<td>983.34</td>
<td>982.71</td>
<td>981.92</td>
<td>980.99</td>
<td>979.92</td>
<td>979.32</td>
<td>984.81</td>
</tr>
<tr class="odd">
<td><strong>10K</strong></td>
<td>984.83</td>
<td>984.60</td>
<td>984.29</td>
<td>983.85</td>
<td>983.32</td>
<td>982.68</td>
<td>981.91</td>
<td>980.98</td>
<td>979.90</td>
<td>979.29</td>
<td>984.83</td>
</tr>
<tr class="even">
<td><strong>20K</strong></td>
<td>984.77</td>
<td>984.57</td>
<td>984.25</td>
<td>983.83</td>
<td>983.31</td>
<td>982.66</td>
<td>981.88</td>
<td>980.97</td>
<td>979.87</td>
<td>979.26</td>
<td>984.77</td>
</tr>
<tr class="odd">
<td><strong>50K</strong></td>
<td>984.78</td>
<td>984.59</td>
<td>984.27</td>
<td>983.82</td>
<td>983.28</td>
<td>982.66</td>
<td>981.89</td>
<td>980.98</td>
<td>979.88</td>
<td>979.28</td>
<td>984.76</td>
</tr>
<tr class="even">
<td><strong>100K</strong></td>
<td>984.77</td>
<td>984.53</td>
<td>984.21</td>
<td>983.80</td>
<td>983.23</td>
<td>982.58</td>
<td>981.82</td>
<td>980.87</td>
<td>979.88</td>
<td>979.11</td>
<td>984.69</td>
</tr>
<tr class="odd">
<td><strong>200K</strong></td>
<td>988.30</td>
<td>988.15</td>
<td>987.84</td>
<td>987.38</td>
<td>986.90</td>
<td>986.23</td>
<td>985.32</td>
<td>984.36</td>
<td>983.29</td>
<td>982.46</td>
<td>985.81</td>
</tr>
<tr class="even">
<td><strong>500K</strong></td>
<td>999.93</td>
<td>1000.92</td>
<td>1000.31</td>
<td>1000.77</td>
<td>999.96</td>
<td>999.25</td>
<td>998.61</td>
<td>997.56</td>
<td>995.84</td>
<td>994.85</td>
<td>978.31</td>
</tr>
</tbody>
</table>

Table A-V. Resistance measurements for 33 thin film resistor as a
function of frequency and temperature.

<table>
<colgroup>
<col style="width: 8%" />
<col style="width: 8%" />
<col style="width: 8%" />
<col style="width: 8%" />
<col style="width: 8%" />
<col style="width: 8%" />
<col style="width: 8%" />
<col style="width: 8%" />
<col style="width: 8%" />
<col style="width: 8%" />
<col style="width: 8%" />
<col style="width: 8%" />
</colgroup>
<tbody>
<tr class="odd">
<td></td>
<td colspan="11"><strong>Temperature</strong></td>
</tr>
<tr class="even">
<td><strong>Freq. (Hz)</strong></td>
<td><strong>25C</strong></td>
<td><strong>0C</strong></td>
<td><strong>-25C</strong></td>
<td><strong>-50C</strong></td>
<td><strong>-75C</strong></td>
<td><strong>-100C</strong></td>
<td><strong>-125C</strong></td>
<td><strong>-150C</strong></td>
<td><strong>-175C</strong></td>
<td><strong>-190C</strong></td>
<td><p><strong>25C</strong></p>
<p><strong>post</strong></p></td>
</tr>
<tr class="odd">
<td><strong>10</strong></td>
<td>33.068</td>
<td>33.049</td>
<td>33.049</td>
<td>33.074</td>
<td>33.135</td>
<td>33.246</td>
<td>33.418</td>
<td>33.668</td>
<td>34.036</td>
<td>34.335</td>
<td>33.063</td>
</tr>
<tr class="even">
<td><strong>50</strong></td>
<td>33.067</td>
<td>33.049</td>
<td>33.047</td>
<td>33.073</td>
<td>33.133</td>
<td>33.244</td>
<td>33.416</td>
<td>33.663</td>
<td>34.033</td>
<td>34.329</td>
<td>33.062</td>
</tr>
<tr class="odd">
<td><strong>100</strong></td>
<td>33.067</td>
<td>33.048</td>
<td>33.047</td>
<td>33.072</td>
<td>33.132</td>
<td>33.243</td>
<td>33.415</td>
<td>33.663</td>
<td>34.032</td>
<td>34.324</td>
<td>33.062</td>
</tr>
<tr class="even">
<td><strong>200</strong></td>
<td>33.065</td>
<td>33.047</td>
<td>33.046</td>
<td>33.071</td>
<td>33.131</td>
<td>33.241</td>
<td>33.414</td>
<td>33.662</td>
<td>34.027</td>
<td>34.323</td>
<td>33.061</td>
</tr>
<tr class="odd">
<td><strong>500</strong></td>
<td>33.065</td>
<td>33.047</td>
<td>33.046</td>
<td>33.070</td>
<td>33.130</td>
<td>33.240</td>
<td>33.414</td>
<td>33.662</td>
<td>34.026</td>
<td>34.323</td>
<td>33.060</td>
</tr>
<tr class="even">
<td><strong>1K</strong></td>
<td>33.067</td>
<td>33.047</td>
<td>33.046</td>
<td>33.070</td>
<td>33.132</td>
<td>33.243</td>
<td>33.414</td>
<td>33.664</td>
<td>34.029</td>
<td>34.324</td>
<td>33.062</td>
</tr>
<tr class="odd">
<td><strong>2K</strong></td>
<td>33.067</td>
<td>33.048</td>
<td>33.047</td>
<td>33.072</td>
<td>33.132</td>
<td>33.242</td>
<td>33.415</td>
<td>33.663</td>
<td>34.031</td>
<td>34.325</td>
<td>33.062</td>
</tr>
<tr class="even">
<td><strong>5K</strong></td>
<td>33.068</td>
<td>33.049</td>
<td>33.048</td>
<td>33.073</td>
<td>33.133</td>
<td>33.244</td>
<td>33.416</td>
<td>33.663</td>
<td>34.033</td>
<td>34.327</td>
<td>33.064</td>
</tr>
<tr class="odd">
<td><strong>10K</strong></td>
<td>33.069</td>
<td>33.051</td>
<td>33.050</td>
<td>33.075</td>
<td>33.135</td>
<td>33.245</td>
<td>33.417</td>
<td>33.663</td>
<td>34.035</td>
<td>34.327</td>
<td>33.068</td>
</tr>
<tr class="even">
<td><strong>20K</strong></td>
<td>33.068</td>
<td>33.049</td>
<td>33.048</td>
<td>33.073</td>
<td>33.133</td>
<td>33.244</td>
<td>33.415</td>
<td>33.665</td>
<td>34.034</td>
<td>34.325</td>
<td>33.063</td>
</tr>
<tr class="odd">
<td><strong>50K</strong></td>
<td>33.068</td>
<td>33.049</td>
<td>33.048</td>
<td>33.073</td>
<td>33.133</td>
<td>33.243</td>
<td>33.414</td>
<td>33.664</td>
<td>34.034</td>
<td>34.325</td>
<td>33.063</td>
</tr>
<tr class="even">
<td><strong>100K</strong></td>
<td>33.071</td>
<td>33.053</td>
<td>33.052</td>
<td>33.077</td>
<td>33.137</td>
<td>33.247</td>
<td>33.418</td>
<td>33.669</td>
<td>34.035</td>
<td>34.327</td>
<td>33.066</td>
</tr>
<tr class="odd">
<td><strong>200K</strong></td>
<td>33.073</td>
<td>33.055</td>
<td>33.055</td>
<td>33.080</td>
<td>33.140</td>
<td>33.249</td>
<td>33.422</td>
<td>33.671</td>
<td>34.035</td>
<td>34.328</td>
<td>33.069</td>
</tr>
<tr class="even">
<td><strong>500K</strong></td>
<td>33.066</td>
<td>33.053</td>
<td>33.054</td>
<td>33.080</td>
<td>33.139</td>
<td>33.243</td>
<td>33.419</td>
<td>33.659</td>
<td>34.031</td>
<td>34.320</td>
<td>33.075</td>
</tr>
</tbody>
</table>

Table A-VI. Resistance measurements for 1 k thin film resistor as a
function of frequency and temperature.

<table>
<colgroup>
<col style="width: 8%" />
<col style="width: 8%" />
<col style="width: 8%" />
<col style="width: 8%" />
<col style="width: 8%" />
<col style="width: 8%" />
<col style="width: 8%" />
<col style="width: 8%" />
<col style="width: 8%" />
<col style="width: 8%" />
<col style="width: 8%" />
<col style="width: 8%" />
</colgroup>
<tbody>
<tr class="odd">
<td></td>
<td colspan="11"><strong>Temperature</strong></td>
</tr>
<tr class="even">
<td><strong>Freq. (Hz)</strong></td>
<td><strong>25C</strong></td>
<td><strong>0C</strong></td>
<td><strong>-25C</strong></td>
<td><strong>-50C</strong></td>
<td><strong>-75C</strong></td>
<td><strong>-100C</strong></td>
<td><strong>-125C</strong></td>
<td><strong>-150C</strong></td>
<td><strong>-175C</strong></td>
<td><strong>-190C</strong></td>
<td><p><strong>25C</strong></p>
<p><strong>post</strong></p></td>
</tr>
<tr class="odd">
<td><strong>10</strong></td>
<td>995.42</td>
<td>995.02</td>
<td>994.92</td>
<td>995.13</td>
<td>995.74</td>
<td>996.78</td>
<td>998.37</td>
<td>1000.70</td>
<td>1004.51</td>
<td>1007.86</td>
<td>995.06</td>
</tr>
<tr class="even">
<td><strong>50</strong></td>
<td>995.39</td>
<td>995.01</td>
<td>994.88</td>
<td>995.09</td>
<td>995.69</td>
<td>996.75</td>
<td>998.33</td>
<td>1000.66</td>
<td>1004.46</td>
<td>1007.87</td>
<td>995.01</td>
</tr>
<tr class="odd">
<td><strong>100</strong></td>
<td>995.38</td>
<td>994.99</td>
<td>994.87</td>
<td>995.09</td>
<td>995.68</td>
<td>996.73</td>
<td>998.32</td>
<td>1000.62</td>
<td>1004.41</td>
<td>1007.88</td>
<td>994.99</td>
</tr>
<tr class="even">
<td><strong>200</strong></td>
<td>995.38</td>
<td>994.99</td>
<td>994.88</td>
<td>995.10</td>
<td>995.69</td>
<td>996.73</td>
<td>998.30</td>
<td>1000.60</td>
<td>1004.38</td>
<td>1007.90</td>
<td>995.00</td>
</tr>
<tr class="odd">
<td><strong>500</strong></td>
<td>995.38</td>
<td>994.99</td>
<td>994.88</td>
<td>995.10</td>
<td>995.70</td>
<td>996.75</td>
<td>998.29</td>
<td>1000.66</td>
<td>1004.43</td>
<td>1007.90</td>
<td>994.99</td>
</tr>
<tr class="even">
<td><strong>1K</strong></td>
<td>995.41</td>
<td>994.99</td>
<td>994.89</td>
<td>995.13</td>
<td>995.71</td>
<td>996.75</td>
<td>998.38</td>
<td>1000.67</td>
<td>1004.48</td>
<td>1007.88</td>
<td>995.01</td>
</tr>
<tr class="odd">
<td><strong>2K</strong></td>
<td>995.40</td>
<td>995.01</td>
<td>994.90</td>
<td>995.14</td>
<td>995.73</td>
<td>996.79</td>
<td>998.35</td>
<td>1000.71</td>
<td>1004.48</td>
<td>1007.95</td>
<td>995.03</td>
</tr>
<tr class="even">
<td><strong>5K</strong></td>
<td>995.43</td>
<td>995.04</td>
<td>994.91</td>
<td>995.15</td>
<td>995.73</td>
<td>996.80</td>
<td>998.38</td>
<td>1000.72</td>
<td>1004.50</td>
<td>1007.96</td>
<td>995.07</td>
</tr>
<tr class="odd">
<td><strong>10K</strong></td>
<td>995.43</td>
<td>995.04</td>
<td>994.94</td>
<td>995.16</td>
<td>995.75</td>
<td>996.81</td>
<td>998.40</td>
<td>1000.73</td>
<td>1004.47</td>
<td>1007.97</td>
<td>995.17</td>
</tr>
<tr class="even">
<td><strong>20K</strong></td>
<td>995.32</td>
<td>994.94</td>
<td>994.81</td>
<td>995.05</td>
<td>995.63</td>
<td>996.70</td>
<td>998.27</td>
<td>1000.60</td>
<td>1004.30</td>
<td>1007.91</td>
<td>994.97</td>
</tr>
<tr class="odd">
<td><strong>50K</strong></td>
<td>995.13</td>
<td>994.75</td>
<td>994.63</td>
<td>994.83</td>
<td>995.40</td>
<td>996.45</td>
<td>998.01</td>
<td>1000.31</td>
<td>1004.05</td>
<td>1007.53</td>
<td>994.92</td>
</tr>
<tr class="even">
<td><strong>100K</strong></td>
<td>994.40</td>
<td>994.06</td>
<td>993.89</td>
<td>994.11</td>
<td>994.57</td>
<td>995.53</td>
<td>997.15</td>
<td>999.41</td>
<td>1002.98</td>
<td>1006.44</td>
<td>994.91</td>
</tr>
<tr class="odd">
<td><strong>200K</strong></td>
<td>992.77</td>
<td>992.16</td>
<td>991.91</td>
<td>991.93</td>
<td>992.23</td>
<td>993.05</td>
<td>994.27</td>
<td>996.37</td>
<td>999.76</td>
<td>1002.10</td>
<td>994.73</td>
</tr>
<tr class="even">
<td><strong>500K</strong></td>
<td>976.45</td>
<td>975.16</td>
<td>974.43</td>
<td>973.48</td>
<td>973.19</td>
<td>972.85</td>
<td>972.90</td>
<td>973.63</td>
<td>974.97</td>
<td>973.41</td>
<td>993.44</td>
</tr>
</tbody>
</table>

Table A-VII. Resistance measurements for 100 thick film resistor as a
function of frequency and temperature.

<table>
<colgroup>
<col style="width: 8%" />
<col style="width: 8%" />
<col style="width: 8%" />
<col style="width: 8%" />
<col style="width: 8%" />
<col style="width: 8%" />
<col style="width: 8%" />
<col style="width: 8%" />
<col style="width: 8%" />
<col style="width: 8%" />
<col style="width: 8%" />
<col style="width: 8%" />
</colgroup>
<tbody>
<tr class="odd">
<td></td>
<td colspan="11"><strong>Temperature</strong></td>
</tr>
<tr class="even">
<td><strong>Freq. (Hz)</strong></td>
<td><strong>25C</strong></td>
<td><strong>0C</strong></td>
<td><strong>-25C</strong></td>
<td><strong>-50C</strong></td>
<td><strong>-75C</strong></td>
<td><strong>-100C</strong></td>
<td><strong>-125C</strong></td>
<td><strong>-150C</strong></td>
<td><strong>-175C</strong></td>
<td><strong>-190C</strong></td>
<td><p><strong>25C</strong></p>
<p><strong>post</strong></p></td>
</tr>
<tr class="odd">
<td><strong>10</strong></td>
<td>100.00</td>
<td>100.02</td>
<td>100.12</td>
<td>100.31</td>
<td>100.64</td>
<td>101.14</td>
<td>101.88</td>
<td>102.84</td>
<td>104.32</td>
<td>105.44</td>
<td>99.99</td>
</tr>
<tr class="even">
<td><strong>50</strong></td>
<td>100.00</td>
<td>100.02</td>
<td>100.12</td>
<td>100.31</td>
<td>100.64</td>
<td>101.13</td>
<td>101.87</td>
<td>102.83</td>
<td>104.32</td>
<td>105.42</td>
<td>99.99</td>
</tr>
<tr class="odd">
<td><strong>100</strong></td>
<td>100.00</td>
<td>100.02</td>
<td>100.12</td>
<td>100.31</td>
<td>100.64</td>
<td>101.14</td>
<td>101.88</td>
<td>102.88</td>
<td>104.32</td>
<td>105.43</td>
<td>99.99</td>
</tr>
<tr class="even">
<td><strong>200</strong></td>
<td>99.99</td>
<td>100.01</td>
<td>100.12</td>
<td>100.31</td>
<td>100.64</td>
<td>101.14</td>
<td>101.87</td>
<td>102.86</td>
<td>104.30</td>
<td>105.42</td>
<td>99.98</td>
</tr>
<tr class="odd">
<td><strong>500</strong></td>
<td>99.99</td>
<td>100.01</td>
<td>100.11</td>
<td>100.31</td>
<td>100.64</td>
<td>101.14</td>
<td>101.87</td>
<td>102.87</td>
<td>104.28</td>
<td>105.42</td>
<td>99.98</td>
</tr>
<tr class="even">
<td><strong>1K</strong></td>
<td>99.99</td>
<td>100.02</td>
<td>100.12</td>
<td>100.31</td>
<td>100.64</td>
<td>101.15</td>
<td>101.87</td>
<td>102.86</td>
<td>104.26</td>
<td>105.42</td>
<td>99.98</td>
</tr>
<tr class="odd">
<td><strong>2K</strong></td>
<td>99.99</td>
<td>100.01</td>
<td>100.12</td>
<td>100.31</td>
<td>100.64</td>
<td>101.14</td>
<td>101.86</td>
<td>102.85</td>
<td>104.30</td>
<td>105.43</td>
<td>99.98</td>
</tr>
<tr class="even">
<td><strong>5K</strong></td>
<td>99.99</td>
<td>100.01</td>
<td>100.12</td>
<td>100.31</td>
<td>100.64</td>
<td>101.14</td>
<td>101.86</td>
<td>102.84</td>
<td>104.31</td>
<td>105.43</td>
<td>99.99</td>
</tr>
<tr class="odd">
<td><strong>10K</strong></td>
<td>99.99</td>
<td>100.02</td>
<td>100.12</td>
<td>100.31</td>
<td>100.64</td>
<td>101.13</td>
<td>101.85</td>
<td>102.83</td>
<td>104.32</td>
<td>105.43</td>
<td>99.99</td>
</tr>
<tr class="even">
<td><strong>20K</strong></td>
<td>100.00</td>
<td>100.02</td>
<td>100.12</td>
<td>100.32</td>
<td>100.64</td>
<td>101.14</td>
<td>101.85</td>
<td>102.87</td>
<td>104.32</td>
<td>105.42</td>
<td>99.98</td>
</tr>
<tr class="odd">
<td><strong>50K</strong></td>
<td>99.99</td>
<td>100.01</td>
<td>100.11</td>
<td>100.31</td>
<td>100.63</td>
<td>101.13</td>
<td>101.86</td>
<td>102.87</td>
<td>104.32</td>
<td>105.42</td>
<td>99.98</td>
</tr>
<tr class="even">
<td><strong>100K</strong></td>
<td>99.98</td>
<td>100.01</td>
<td>100.11</td>
<td>100.31</td>
<td>100.63</td>
<td>101.14</td>
<td>101.86</td>
<td>102.88</td>
<td>104.29</td>
<td>105.42</td>
<td>99.98</td>
</tr>
<tr class="odd">
<td><strong>200K</strong></td>
<td>99.96</td>
<td>99.99</td>
<td>100.09</td>
<td>100.29</td>
<td>100.61</td>
<td>101.11</td>
<td>101.84</td>
<td>102.85</td>
<td>104.24</td>
<td>105.40</td>
<td>99.95</td>
</tr>
<tr class="even">
<td><strong>500K</strong></td>
<td>99.94</td>
<td>99.96</td>
<td>100.07</td>
<td>100.26</td>
<td>100.60</td>
<td>101.10</td>
<td>101.81</td>
<td>102.71</td>
<td>104.10</td>
<td>105.24</td>
<td>99.93</td>
</tr>
</tbody>
</table>

Table A-VIII. Resistance measurements for 1 k thick film resistor as a
function of frequency and temperature.

<table>
<colgroup>
<col style="width: 8%" />
<col style="width: 8%" />
<col style="width: 8%" />
<col style="width: 8%" />
<col style="width: 8%" />
<col style="width: 8%" />
<col style="width: 8%" />
<col style="width: 8%" />
<col style="width: 8%" />
<col style="width: 8%" />
<col style="width: 8%" />
<col style="width: 8%" />
</colgroup>
<tbody>
<tr class="odd">
<td></td>
<td colspan="11"><strong>Temperature</strong></td>
</tr>
<tr class="even">
<td><strong>Freq. (Hz)</strong></td>
<td><strong>25C</strong></td>
<td><strong>0C</strong></td>
<td><strong>-25C</strong></td>
<td><strong>-50C</strong></td>
<td><strong>-75C</strong></td>
<td><strong>-100C</strong></td>
<td><strong>-125C</strong></td>
<td><strong>-150C</strong></td>
<td><strong>-175C</strong></td>
<td><strong>-190C</strong></td>
<td><p><strong>25C</strong></p>
<p><strong>post</strong></p></td>
</tr>
<tr class="odd">
<td><strong>10</strong></td>
<td>998.72</td>
<td>998.30</td>
<td>998.03</td>
<td>997.95</td>
<td>998.07</td>
<td>998.36</td>
<td>998.86</td>
<td>999.69</td>
<td>1001.30</td>
<td>1003.22</td>
<td>998.74</td>
</tr>
<tr class="even">
<td><strong>50</strong></td>
<td>998.68</td>
<td>998.28</td>
<td>998.00</td>
<td>997.92</td>
<td>998.04</td>
<td>998.33</td>
<td>998.82</td>
<td>999.65</td>
<td>1001.32</td>
<td>1003.21</td>
<td>998.68</td>
</tr>
<tr class="odd">
<td><strong>100</strong></td>
<td>998.67</td>
<td>998.27</td>
<td>997.99</td>
<td>997.92</td>
<td>998.02</td>
<td>998.32</td>
<td>998.82</td>
<td>999.62</td>
<td>1001.30</td>
<td>1003.19</td>
<td>998.65</td>
</tr>
<tr class="even">
<td><strong>200</strong></td>
<td>998.67</td>
<td>998.27</td>
<td>997.99</td>
<td>997.92</td>
<td>998.03</td>
<td>998.32</td>
<td>998.82</td>
<td>999.62</td>
<td>1001.31</td>
<td>1003.16</td>
<td>998.64</td>
</tr>
<tr class="odd">
<td><strong>500</strong></td>
<td>998.68</td>
<td>998.27</td>
<td>997.99</td>
<td>997.92</td>
<td>998.03</td>
<td>998.32</td>
<td>998.83</td>
<td>999.63</td>
<td>1001.29</td>
<td>1003.17</td>
<td>998.63</td>
</tr>
<tr class="even">
<td><strong>1K</strong></td>
<td>998.70</td>
<td>998.29</td>
<td>998.03</td>
<td>997.94</td>
<td>998.09</td>
<td>998.33</td>
<td>998.85</td>
<td>999.70</td>
<td>1001.27</td>
<td>1003.22</td>
<td>998.68</td>
</tr>
<tr class="odd">
<td><strong>2K</strong></td>
<td>998.71</td>
<td>998.31</td>
<td>998.02</td>
<td>997.96</td>
<td>998.07</td>
<td>998.36</td>
<td>998.85</td>
<td>999.69</td>
<td>1001.29</td>
<td>1003.21</td>
<td>998.66</td>
</tr>
<tr class="even">
<td><strong>5K</strong></td>
<td>998.72</td>
<td>998.32</td>
<td>998.05</td>
<td>997.98</td>
<td>998.09</td>
<td>998.38</td>
<td>998.87</td>
<td>999.72</td>
<td>1001.36</td>
<td>1003.24</td>
<td>998.70</td>
</tr>
<tr class="odd">
<td><strong>10K</strong></td>
<td>998.73</td>
<td>998.34</td>
<td>998.07</td>
<td>998.01</td>
<td>998.12</td>
<td>998.41</td>
<td>998.90</td>
<td>999.73</td>
<td>1001.39</td>
<td>1003.26</td>
<td>998.79</td>
</tr>
<tr class="even">
<td><strong>20K</strong></td>
<td>998.65</td>
<td>998.26</td>
<td>997.98</td>
<td>997.93</td>
<td>998.04</td>
<td>998.34</td>
<td>998.80</td>
<td>999.64</td>
<td>1001.32</td>
<td>1003.15</td>
<td>998.58</td>
</tr>
<tr class="odd">
<td><strong>50K</strong></td>
<td>998.61</td>
<td>998.25</td>
<td>997.97</td>
<td>997.88</td>
<td>998.01</td>
<td>998.31</td>
<td>998.80</td>
<td>999.61</td>
<td>1001.28</td>
<td>1003.13</td>
<td>998.52</td>
</tr>
<tr class="even">
<td><strong>100K</strong></td>
<td>998.60</td>
<td>998.23</td>
<td>997.91</td>
<td>997.86</td>
<td>997.99</td>
<td>998.25</td>
<td>998.75</td>
<td>999.50</td>
<td>1001.19</td>
<td>1003.02</td>
<td>998.52</td>
</tr>
<tr class="odd">
<td><strong>200K</strong></td>
<td>999.52</td>
<td>999.31</td>
<td>998.97</td>
<td>998.83</td>
<td>998.85</td>
<td>999.01</td>
<td>999.62</td>
<td>1000.29</td>
<td>1001.35</td>
<td>1003.37</td>
<td>998.33</td>
</tr>
<tr class="even">
<td><strong>500K</strong></td>
<td>993.46</td>
<td>992.99</td>
<td>993.31</td>
<td>992.67</td>
<td>993.00</td>
<td>992.99</td>
<td>993.64</td>
<td>993.85</td>
<td>994.45</td>
<td>996.08</td>
<td>997.05</td>
</tr>
</tbody>
</table>

Table A-IX. Resistance measurements for 10 carbon film resistor as a
function of frequency and temperature.

<table>
<colgroup>
<col style="width: 8%" />
<col style="width: 8%" />
<col style="width: 8%" />
<col style="width: 8%" />
<col style="width: 8%" />
<col style="width: 8%" />
<col style="width: 8%" />
<col style="width: 8%" />
<col style="width: 8%" />
<col style="width: 8%" />
<col style="width: 8%" />
<col style="width: 8%" />
</colgroup>
<tbody>
<tr class="odd">
<td></td>
<td colspan="11"><strong>Temperature</strong></td>
</tr>
<tr class="even">
<td><strong>Freq. (Hz)</strong></td>
<td><strong>25C</strong></td>
<td><strong>0C</strong></td>
<td><strong>-25C</strong></td>
<td><strong>-50C</strong></td>
<td><strong>-75C</strong></td>
<td><strong>-100C</strong></td>
<td><strong>-125C</strong></td>
<td><strong>-150C</strong></td>
<td><strong>-175C</strong></td>
<td><strong>-190C</strong></td>
<td><p><strong>25C</strong></p>
<p><strong>post</strong></p></td>
</tr>
<tr class="odd">
<td><strong>10</strong></td>
<td>9.958</td>
<td>10.001</td>
<td>10.055</td>
<td>10.109</td>
<td>10.166</td>
<td>10.226</td>
<td>10.288</td>
<td>10.355</td>
<td>10.428</td>
<td>10.463</td>
<td>9.958</td>
</tr>
<tr class="even">
<td><strong>50</strong></td>
<td>9.957</td>
<td>10.000</td>
<td>10.055</td>
<td>10.109</td>
<td>10.165</td>
<td>10.225</td>
<td>10.289</td>
<td>10.355</td>
<td>10.427</td>
<td>10.463</td>
<td>9.957</td>
</tr>
<tr class="odd">
<td><strong>100</strong></td>
<td>9.957</td>
<td>10.000</td>
<td>10.054</td>
<td>10.108</td>
<td>10.165</td>
<td>10.225</td>
<td>10.288</td>
<td>10.355</td>
<td>10.427</td>
<td>10.462</td>
<td>9.957</td>
</tr>
<tr class="even">
<td><strong>200</strong></td>
<td>9.956</td>
<td>10.000</td>
<td>10.054</td>
<td>10.108</td>
<td>10.164</td>
<td>10.224</td>
<td>10.288</td>
<td>10.354</td>
<td>10.426</td>
<td>10.462</td>
<td>9.956</td>
</tr>
<tr class="odd">
<td><strong>500</strong></td>
<td>9.956</td>
<td>9.999</td>
<td>10.054</td>
<td>10.108</td>
<td>10.164</td>
<td>10.224</td>
<td>10.287</td>
<td>10.354</td>
<td>10.426</td>
<td>10.461</td>
<td>9.956</td>
</tr>
<tr class="even">
<td><strong>1K</strong></td>
<td>9.957</td>
<td>10.000</td>
<td>10.054</td>
<td>10.108</td>
<td>10.165</td>
<td>10.225</td>
<td>10.287</td>
<td>10.354</td>
<td>10.426</td>
<td>10.462</td>
<td>9.956</td>
</tr>
<tr class="odd">
<td><strong>2K</strong></td>
<td>9.956</td>
<td>10.000</td>
<td>10.054</td>
<td>10.108</td>
<td>10.165</td>
<td>10.225</td>
<td>10.287</td>
<td>10.353</td>
<td>10.427</td>
<td>10.460</td>
<td>9.956</td>
</tr>
<tr class="even">
<td><strong>5K</strong></td>
<td>9.956</td>
<td>9.999</td>
<td>10.054</td>
<td>10.108</td>
<td>10.165</td>
<td>10.225</td>
<td>10.287</td>
<td>10.355</td>
<td>10.426</td>
<td>10.461</td>
<td>9.956</td>
</tr>
<tr class="odd">
<td><strong>10K</strong></td>
<td>9.957</td>
<td>10.001</td>
<td>10.055</td>
<td>10.109</td>
<td>10.166</td>
<td>10.226</td>
<td>10.287</td>
<td>10.355</td>
<td>10.427</td>
<td>10.461</td>
<td>9.957</td>
</tr>
<tr class="even">
<td><strong>20K</strong></td>
<td>9.957</td>
<td>10.000</td>
<td>10.054</td>
<td>10.108</td>
<td>10.165</td>
<td>10.226</td>
<td>10.287</td>
<td>10.355</td>
<td>10.427</td>
<td>10.462</td>
<td>9.957</td>
</tr>
<tr class="odd">
<td><strong>50K</strong></td>
<td>9.957</td>
<td>10.001</td>
<td>10.055</td>
<td>10.109</td>
<td>10.166</td>
<td>10.226</td>
<td>10.289</td>
<td>10.355</td>
<td>10.426</td>
<td>10.461</td>
<td>9.957</td>
</tr>
<tr class="even">
<td><strong>100K</strong></td>
<td>9.957</td>
<td>10.001</td>
<td>10.055</td>
<td>10.109</td>
<td>10.166</td>
<td>10.226</td>
<td>10.288</td>
<td>10.355</td>
<td>10.426</td>
<td>10.461</td>
<td>9.957</td>
</tr>
<tr class="odd">
<td><strong>200K</strong></td>
<td>9.958</td>
<td>10.002</td>
<td>10.056</td>
<td>10.110</td>
<td>10.168</td>
<td>10.227</td>
<td>10.290</td>
<td>10.357</td>
<td>10.428</td>
<td>10.462</td>
<td>9.958</td>
</tr>
<tr class="even">
<td><strong>500K</strong></td>
<td>9.959</td>
<td>10.003</td>
<td>10.057</td>
<td>10.110</td>
<td>10.167</td>
<td>10.225</td>
<td>10.288</td>
<td>10.354</td>
<td>10.424</td>
<td>10.458</td>
<td>9.960</td>
</tr>
</tbody>
</table>

Table A-X. Resistance measurements for 1 k carbon film resistor as a
function of frequency and temperature.

<table>
<colgroup>
<col style="width: 8%" />
<col style="width: 8%" />
<col style="width: 8%" />
<col style="width: 8%" />
<col style="width: 8%" />
<col style="width: 8%" />
<col style="width: 8%" />
<col style="width: 8%" />
<col style="width: 8%" />
<col style="width: 8%" />
<col style="width: 8%" />
<col style="width: 8%" />
</colgroup>
<tbody>
<tr class="odd">
<td></td>
<td colspan="11"><strong>Temperature</strong></td>
</tr>
<tr class="even">
<td><strong>Freq. (Hz)</strong></td>
<td><strong>25C</strong></td>
<td><strong>0C</strong></td>
<td><strong>-25C</strong></td>
<td><strong>-50C</strong></td>
<td><strong>-75C</strong></td>
<td><strong>-100C</strong></td>
<td><strong>-125C</strong></td>
<td><strong>-150C</strong></td>
<td><strong>-175C</strong></td>
<td><strong>-190C</strong></td>
<td><p><strong>25C</strong></p>
<p><strong>post</strong></p></td>
</tr>
<tr class="odd">
<td><strong>10</strong></td>
<td>980.32</td>
<td>985.18</td>
<td>991.33</td>
<td>997.37</td>
<td>1003.73</td>
<td>1010.42</td>
<td>1017.41</td>
<td>1024.58</td>
<td>1032.34</td>
<td>1035.97</td>
<td>980.18</td>
</tr>
<tr class="even">
<td><strong>50</strong></td>
<td>980.25</td>
<td>985.13</td>
<td>991.29</td>
<td>997.34</td>
<td>1003.68</td>
<td>1010.37</td>
<td>1017.34</td>
<td>1024.49</td>
<td>1032.32</td>
<td>1035.77</td>
<td>980.12</td>
</tr>
<tr class="odd">
<td><strong>100</strong></td>
<td>980.24</td>
<td>985.11</td>
<td>991.26</td>
<td>997.32</td>
<td>1003.82</td>
<td>1010.47</td>
<td>1017.39</td>
<td>1024.56</td>
<td>1032.26</td>
<td>1035.80</td>
<td>980.10</td>
</tr>
<tr class="even">
<td><strong>200</strong></td>
<td>980.25</td>
<td>985.12</td>
<td>991.26</td>
<td>997.32</td>
<td>1003.74</td>
<td>1010.47</td>
<td>1017.36</td>
<td>1024.79</td>
<td>1032.22</td>
<td>1035.84</td>
<td>980.11</td>
</tr>
<tr class="odd">
<td><strong>500</strong></td>
<td>980.26</td>
<td>985.12</td>
<td>991.27</td>
<td>997.32</td>
<td>1003.79</td>
<td>1010.48</td>
<td>1017.36</td>
<td>1024.58</td>
<td>1032.17</td>
<td>1035.87</td>
<td>980.12</td>
</tr>
<tr class="even">
<td><strong>1K</strong></td>
<td>980.30</td>
<td>985.13</td>
<td>991.28</td>
<td>997.39</td>
<td>1003.79</td>
<td>1010.49</td>
<td>1017.35</td>
<td>1024.77</td>
<td>1032.38</td>
<td>1035.83</td>
<td>980.13</td>
</tr>
<tr class="odd">
<td><strong>2K</strong></td>
<td>980.30</td>
<td>985.16</td>
<td>991.29</td>
<td>997.38</td>
<td>1003.79</td>
<td>1010.48</td>
<td>1017.31</td>
<td>1024.63</td>
<td>1032.33</td>
<td>1035.88</td>
<td>980.15</td>
</tr>
<tr class="even">
<td><strong>5K</strong></td>
<td>980.29</td>
<td>985.16</td>
<td>991.31</td>
<td>997.40</td>
<td>1003.79</td>
<td>1010.46</td>
<td>1017.29</td>
<td>1024.55</td>
<td>1032.34</td>
<td>1035.91</td>
<td>980.16</td>
</tr>
<tr class="odd">
<td><strong>10K</strong></td>
<td>980.28</td>
<td>985.16</td>
<td>991.29</td>
<td>997.35</td>
<td>1003.73</td>
<td>1010.39</td>
<td>1017.22</td>
<td>1024.45</td>
<td>1032.27</td>
<td>1035.82</td>
<td>980.16</td>
</tr>
<tr class="even">
<td><strong>20K</strong></td>
<td>980.21</td>
<td>985.08</td>
<td>991.19</td>
<td>997.32</td>
<td>1003.64</td>
<td>1010.30</td>
<td>1017.14</td>
<td>1024.47</td>
<td>1032.24</td>
<td>1035.78</td>
<td>980.10</td>
</tr>
<tr class="odd">
<td><strong>50K</strong></td>
<td>980.07</td>
<td>984.95</td>
<td>991.03</td>
<td>997.09</td>
<td>1003.41</td>
<td>1010.05</td>
<td>1017.06</td>
<td>1024.36</td>
<td>1031.88</td>
<td>1035.43</td>
<td>979.91</td>
</tr>
<tr class="even">
<td><strong>100K</strong></td>
<td>979.59</td>
<td>984.29</td>
<td>990.56</td>
<td>996.37</td>
<td>1002.69</td>
<td>1009.30</td>
<td>1016.07</td>
<td>1023.32</td>
<td>1030.73</td>
<td>1034.25</td>
<td>979.18</td>
</tr>
<tr class="odd">
<td><strong>200K</strong></td>
<td>981.12</td>
<td>985.76</td>
<td>991.67</td>
<td>997.61</td>
<td>1003.40</td>
<td>1009.93</td>
<td>1016.22</td>
<td>1023.03</td>
<td>1030.01</td>
<td>1033.32</td>
<td>977.51</td>
</tr>
<tr class="even">
<td><strong>500K</strong></td>
<td>984.73</td>
<td>987.93</td>
<td>992.48</td>
<td>997.55</td>
<td>1001.78</td>
<td>1006.22</td>
<td>1010.14</td>
<td>1014.61</td>
<td>1019.06</td>
<td>1020.53</td>
<td>961.65</td>
</tr>
</tbody>
</table>

Table A-XI. Resistance measurements for 15 carbon composition resistor
as a function of frequency and temperature.

<table>
<colgroup>
<col style="width: 8%" />
<col style="width: 8%" />
<col style="width: 8%" />
<col style="width: 8%" />
<col style="width: 8%" />
<col style="width: 8%" />
<col style="width: 8%" />
<col style="width: 8%" />
<col style="width: 8%" />
<col style="width: 8%" />
<col style="width: 8%" />
<col style="width: 8%" />
</colgroup>
<tbody>
<tr class="odd">
<td></td>
<td colspan="11"><h1 id="temperature">Temperature</h1></td>
</tr>
<tr class="even">
<td><strong>Freq. (Hz)</strong></td>
<td><strong>25C</strong></td>
<td><strong>0C</strong></td>
<td><strong>-25C</strong></td>
<td><strong>-50C</strong></td>
<td><strong>-75C</strong></td>
<td><strong>-100C</strong></td>
<td><strong>-125C</strong></td>
<td><strong>-150C</strong></td>
<td><strong>-175C</strong></td>
<td><strong>-190C</strong></td>
<td><p><strong>25C</strong></p>
<p><strong>post</strong></p></td>
</tr>
<tr class="odd">
<td><strong>10</strong></td>
<td>14.648</td>
<td>14.788</td>
<td>14.948</td>
<td>15.112</td>
<td>15.284</td>
<td>15.470</td>
<td>15.671</td>
<td>15.897</td>
<td>16.163</td>
<td>16.345</td>
<td>14.782</td>
</tr>
<tr class="even">
<td><strong>50</strong></td>
<td>14.648</td>
<td>14.787</td>
<td>14.947</td>
<td>15.110</td>
<td>15.282</td>
<td>15.469</td>
<td>15.675</td>
<td>15.895</td>
<td>16.161</td>
<td>16.342</td>
<td>14.781</td>
</tr>
<tr class="odd">
<td><strong>100</strong></td>
<td>14.647</td>
<td>14.786</td>
<td>14.946</td>
<td>15.110</td>
<td>15.281</td>
<td>15.469</td>
<td>15.672</td>
<td>15.893</td>
<td>16.162</td>
<td>16.343</td>
<td>14.782</td>
</tr>
<tr class="even">
<td><strong>200</strong></td>
<td>14.646</td>
<td>14.785</td>
<td>14.945</td>
<td>15.109</td>
<td>15.280</td>
<td>15.468</td>
<td>15.672</td>
<td>15.892</td>
<td>16.160</td>
<td>16.344</td>
<td>14.781</td>
</tr>
<tr class="odd">
<td><strong>500</strong></td>
<td>14.646</td>
<td>14.785</td>
<td>14.945</td>
<td>15.108</td>
<td>15.280</td>
<td>15.467</td>
<td>15.671</td>
<td>15.898</td>
<td>16.162</td>
<td>16.343</td>
<td>14.780</td>
</tr>
<tr class="even">
<td><strong>1K</strong></td>
<td>14.647</td>
<td>14.785</td>
<td>14.945</td>
<td>15.109</td>
<td>15.279</td>
<td>15.468</td>
<td>15.671</td>
<td>15.895</td>
<td>16.161</td>
<td>16.342</td>
<td>14.782</td>
</tr>
<tr class="odd">
<td><strong>2K</strong></td>
<td>14.646</td>
<td>14.785</td>
<td>14.945</td>
<td>15.109</td>
<td>15.280</td>
<td>15.467</td>
<td>15.670</td>
<td>15.897</td>
<td>16.160</td>
<td>16.342</td>
<td>14.782</td>
</tr>
<tr class="even">
<td><strong>5K</strong></td>
<td>14.646</td>
<td>14.785</td>
<td>14.945</td>
<td>15.109</td>
<td>15.281</td>
<td>15.467</td>
<td>15.669</td>
<td>15.896</td>
<td>16.158</td>
<td>16.344</td>
<td>14.783</td>
</tr>
<tr class="odd">
<td><strong>10K</strong></td>
<td>14.647</td>
<td>14.786</td>
<td>14.946</td>
<td>15.110</td>
<td>15.282</td>
<td>15.467</td>
<td>15.669</td>
<td>15.897</td>
<td>16.161</td>
<td>16.344</td>
<td>14.786</td>
</tr>
<tr class="even">
<td><strong>20K</strong></td>
<td>14.646</td>
<td>14.785</td>
<td>14.945</td>
<td>15.110</td>
<td>15.281</td>
<td>15.466</td>
<td>15.671</td>
<td>15.895</td>
<td>16.160</td>
<td>16.344</td>
<td>14.783</td>
</tr>
<tr class="odd">
<td><strong>50K</strong></td>
<td>14.645</td>
<td>14.785</td>
<td>14.945</td>
<td>15.109</td>
<td>15.280</td>
<td>15.466</td>
<td>15.669</td>
<td>15.892</td>
<td>16.161</td>
<td>16.344</td>
<td>14.783</td>
</tr>
<tr class="even">
<td><strong>100K</strong></td>
<td>14.645</td>
<td>14.785</td>
<td>14.945</td>
<td>15.109</td>
<td>15.280</td>
<td>15.468</td>
<td>15.671</td>
<td>15.892</td>
<td>16.161</td>
<td>16.344</td>
<td>14.784</td>
</tr>
<tr class="odd">
<td><strong>200K</strong></td>
<td>14.644</td>
<td>14.786</td>
<td>14.946</td>
<td>15.110</td>
<td>15.281</td>
<td>15.469</td>
<td>15.672</td>
<td>15.894</td>
<td>16.163</td>
<td>16.343</td>
<td>14.788</td>
</tr>
<tr class="even">
<td><strong>500K</strong></td>
<td>14.637</td>
<td>14.789</td>
<td>14.951</td>
<td>15.112</td>
<td>15.283</td>
<td>15.472</td>
<td>15.675</td>
<td>15.893</td>
<td>16.162</td>
<td>16.344</td>
<td>14.792</td>
</tr>
</tbody>
</table>

Table A-XII. Resistance measurements for 1 k carbon composition resistor
as a function of frequency and temperature.

<table>
<colgroup>
<col style="width: 8%" />
<col style="width: 8%" />
<col style="width: 8%" />
<col style="width: 8%" />
<col style="width: 8%" />
<col style="width: 8%" />
<col style="width: 8%" />
<col style="width: 8%" />
<col style="width: 8%" />
<col style="width: 8%" />
<col style="width: 8%" />
<col style="width: 8%" />
</colgroup>
<tbody>
<tr class="odd">
<td></td>
<td colspan="11"><strong>Temperature</strong></td>
</tr>
<tr class="even">
<td><strong>Freq. (Hz)</strong></td>
<td><strong>25C</strong></td>
<td><strong>0C</strong></td>
<td><strong>-25C</strong></td>
<td><strong>-50C</strong></td>
<td><strong>-75C</strong></td>
<td><strong>-100C</strong></td>
<td><strong>-125C</strong></td>
<td><strong>-150C</strong></td>
<td><strong>-175C</strong></td>
<td><strong>-190C</strong></td>
<td><p><strong>25C</strong></p>
<p><strong>post</strong></p></td>
</tr>
<tr class="odd">
<td><strong>10</strong></td>
<td>1013.25</td>
<td>1027.54</td>
<td>1045.34</td>
<td>1064.66</td>
<td>1087.29</td>
<td>1114.87</td>
<td>1148.51</td>
<td>1191.58</td>
<td>1250.45</td>
<td>1296.42</td>
<td>1015.09</td>
</tr>
<tr class="even">
<td><strong>50</strong></td>
<td>1013.23</td>
<td>1027.52</td>
<td>1045.35</td>
<td>1064.61</td>
<td>1087.16</td>
<td>1114.83</td>
<td>1148.21</td>
<td>1191.44</td>
<td>1250.43</td>
<td>1296.74</td>
<td>1015.47</td>
</tr>
<tr class="odd">
<td><strong>100</strong></td>
<td>1013.21</td>
<td>1027.49</td>
<td>1045.36</td>
<td>1064.61</td>
<td>1087.13</td>
<td>1114.73</td>
<td>1148.01</td>
<td>1191.11</td>
<td>1250.05</td>
<td>1296.75</td>
<td>1015.71</td>
</tr>
<tr class="even">
<td><strong>200</strong></td>
<td>1013.23</td>
<td>1027.50</td>
<td>1045.36</td>
<td>1064.62</td>
<td>1087.12</td>
<td>1114.61</td>
<td>1148.60</td>
<td>1190.86</td>
<td>1249.38</td>
<td>1296.97</td>
<td>1015.78</td>
</tr>
<tr class="odd">
<td><strong>500</strong></td>
<td>1013.22</td>
<td>1027.49</td>
<td>1045.37</td>
<td>1064.62</td>
<td>1087.12</td>
<td>1114.54</td>
<td>1148.59</td>
<td>1190.50</td>
<td>1248.97</td>
<td>1296.77</td>
<td>1015.81</td>
</tr>
<tr class="even">
<td><strong>1K</strong></td>
<td>1013.29</td>
<td>1027.53</td>
<td>1045.39</td>
<td>1064.81</td>
<td>1087.39</td>
<td>1114.53</td>
<td>1148.71</td>
<td>1190.34</td>
<td>1250.08</td>
<td>1296.54</td>
<td>1015.93</td>
</tr>
<tr class="odd">
<td><strong>2K</strong></td>
<td>1013.26</td>
<td>1027.54</td>
<td>1045.40</td>
<td>1064.77</td>
<td>1087.31</td>
<td>1115.01</td>
<td>1148.77</td>
<td>1191.77</td>
<td>1250.21</td>
<td>1296.83</td>
<td>1016.00</td>
</tr>
<tr class="even">
<td><strong>5K</strong></td>
<td>1013.26</td>
<td>1027.52</td>
<td>1045.36</td>
<td>1064.82</td>
<td>1087.40</td>
<td>1114.86</td>
<td>1148.50</td>
<td>1191.55</td>
<td>1250.16</td>
<td>1297.05</td>
<td>1016.04</td>
</tr>
<tr class="odd">
<td><strong>10K</strong></td>
<td>1013.28</td>
<td>1027.53</td>
<td>1045.40</td>
<td>1064.74</td>
<td>1087.37</td>
<td>1115.09</td>
<td>1148.40</td>
<td>1191.78</td>
<td>1250.72</td>
<td>1297.30</td>
<td>1016.27</td>
</tr>
<tr class="even">
<td><strong>20K</strong></td>
<td>1013.21</td>
<td>1027.48</td>
<td>1045.34</td>
<td>1064.64</td>
<td>1087.31</td>
<td>1114.90</td>
<td>1148.06</td>
<td>1191.58</td>
<td>1250.40</td>
<td>1297.19</td>
<td>1016.18</td>
</tr>
<tr class="odd">
<td><strong>50K</strong></td>
<td>1013.16</td>
<td>1027.40</td>
<td>1045.28</td>
<td>1064.61</td>
<td>1087.20</td>
<td>1114.75</td>
<td>1147.92</td>
<td>1191.38</td>
<td>1249.96</td>
<td>1297.15</td>
<td>1016.19</td>
</tr>
<tr class="even">
<td><strong>100K</strong></td>
<td>1013.06</td>
<td>1027.35</td>
<td>1045.22</td>
<td>1064.42</td>
<td>1086.96</td>
<td>1114.49</td>
<td>1148.65</td>
<td>1190.93</td>
<td>1249.12</td>
<td>1296.46</td>
<td>1016.31</td>
</tr>
<tr class="odd">
<td><strong>200K</strong></td>
<td>1014.05</td>
<td>1028.44</td>
<td>1046.22</td>
<td>1065.61</td>
<td>1087.92</td>
<td>1115.37</td>
<td>1149.01</td>
<td>1191.31</td>
<td>1249.14</td>
<td>1296.29</td>
<td>1016.18</td>
</tr>
<tr class="even">
<td><strong>500K</strong></td>
<td>1007.75</td>
<td>1021.96</td>
<td>1039.64</td>
<td>1058.62</td>
<td>1081.20</td>
<td>1107.52</td>
<td>1141.08</td>
<td>1182.06</td>
<td>1240.25</td>
<td>1283.51</td>
<td>1014.91</td>
</tr>
</tbody>
</table>

Table A-XIII. Resistance measurements for 10 ceramic composition
resistor as a function of frequency and temperature.

<table>
<colgroup>
<col style="width: 8%" />
<col style="width: 8%" />
<col style="width: 8%" />
<col style="width: 8%" />
<col style="width: 8%" />
<col style="width: 8%" />
<col style="width: 8%" />
<col style="width: 8%" />
<col style="width: 8%" />
<col style="width: 8%" />
<col style="width: 8%" />
<col style="width: 8%" />
</colgroup>
<tbody>
<tr class="odd">
<td></td>
<td colspan="11"><strong>Temperature</strong></td>
</tr>
<tr class="even">
<td><strong>Freq. (Hz)</strong></td>
<td><strong>25C</strong></td>
<td><strong>0C</strong></td>
<td><strong>-25C</strong></td>
<td><strong>-50C</strong></td>
<td><strong>-75C</strong></td>
<td><strong>-100C</strong></td>
<td><strong>-125C</strong></td>
<td><strong>-150C</strong></td>
<td><strong>-175C</strong></td>
<td><strong>-190C</strong></td>
<td><p><strong>25C</strong></p>
<p><strong>post</strong></p></td>
</tr>
<tr class="odd">
<td><strong>10</strong></td>
<td>9.496</td>
<td>9.702</td>
<td>9.949</td>
<td>10.174</td>
<td>10.385</td>
<td>10.575</td>
<td>10.735</td>
<td>10.864</td>
<td>10.960</td>
<td>10.994</td>
<td>9.488</td>
</tr>
<tr class="even">
<td><strong>50</strong></td>
<td>9.495</td>
<td>9.701</td>
<td>9.948</td>
<td>10.174</td>
<td>10.385</td>
<td>10.574</td>
<td>10.734</td>
<td>10.864</td>
<td>10.960</td>
<td>10.994</td>
<td>9.487</td>
</tr>
<tr class="odd">
<td><strong>100</strong></td>
<td>9.494</td>
<td>9.701</td>
<td>9.948</td>
<td>10.174</td>
<td>10.385</td>
<td>10.573</td>
<td>10.733</td>
<td>10.864</td>
<td>10.960</td>
<td>10.995</td>
<td>9.486</td>
</tr>
<tr class="even">
<td><strong>200</strong></td>
<td>9.494</td>
<td>9.700</td>
<td>9.947</td>
<td>10.173</td>
<td>10.384</td>
<td>10.573</td>
<td>10.735</td>
<td>10.863</td>
<td>10.959</td>
<td>10.994</td>
<td>9.486</td>
</tr>
<tr class="odd">
<td><strong>500</strong></td>
<td>9.493</td>
<td>9.700</td>
<td>9.947</td>
<td>10.173</td>
<td>10.384</td>
<td>10.574</td>
<td>10.735</td>
<td>10.862</td>
<td>10.959</td>
<td>10.994</td>
<td>9.485</td>
</tr>
<tr class="even">
<td><strong>1K</strong></td>
<td>9.494</td>
<td>9.700</td>
<td>9.948</td>
<td>10.173</td>
<td>10.384</td>
<td>10.574</td>
<td>10.735</td>
<td>10.862</td>
<td>10.959</td>
<td>10.994</td>
<td>9.485</td>
</tr>
<tr class="odd">
<td><strong>2K</strong></td>
<td>9.493</td>
<td>9.700</td>
<td>9.947</td>
<td>10.173</td>
<td>10.384</td>
<td>10.575</td>
<td>10.735</td>
<td>10.861</td>
<td>10.959</td>
<td>10.994</td>
<td>9.485</td>
</tr>
<tr class="even">
<td><strong>5K</strong></td>
<td>9.493</td>
<td>9.700</td>
<td>9.947</td>
<td>10.173</td>
<td>10.383</td>
<td>10.575</td>
<td>10.735</td>
<td>10.862</td>
<td>10.960</td>
<td>10.994</td>
<td>9.485</td>
</tr>
<tr class="odd">
<td><strong>10K</strong></td>
<td>9.494</td>
<td>9.701</td>
<td>9.949</td>
<td>10.174</td>
<td>10.384</td>
<td>10.575</td>
<td>10.734</td>
<td>10.864</td>
<td>10.960</td>
<td>10.994</td>
<td>9.486</td>
</tr>
<tr class="even">
<td><strong>20K</strong></td>
<td>9.494</td>
<td>9.701</td>
<td>9.948</td>
<td>10.173</td>
<td>10.384</td>
<td>10.575</td>
<td>10.734</td>
<td>10.864</td>
<td>10.961</td>
<td>10.994</td>
<td>9.486</td>
</tr>
<tr class="odd">
<td><strong>50K</strong></td>
<td>9.494</td>
<td>9.702</td>
<td>9.949</td>
<td>10.174</td>
<td>10.384</td>
<td>10.575</td>
<td>10.734</td>
<td>10.864</td>
<td>10.960</td>
<td>10.994</td>
<td>9.486</td>
</tr>
<tr class="even">
<td><strong>100K</strong></td>
<td>9.494</td>
<td>9.702</td>
<td>9.949</td>
<td>10.174</td>
<td>10.385</td>
<td>10.575</td>
<td>10.736</td>
<td>10.865</td>
<td>10.960</td>
<td>10.994</td>
<td>9.486</td>
</tr>
<tr class="odd">
<td><strong>200K</strong></td>
<td>9.495</td>
<td>9.703</td>
<td>9.951</td>
<td>10.176</td>
<td>10.387</td>
<td>10.576</td>
<td>10.737</td>
<td>10.866</td>
<td>10.961</td>
<td>10.995</td>
<td>9.487</td>
</tr>
<tr class="even">
<td><strong>500K</strong></td>
<td>9.496</td>
<td>9.705</td>
<td>9.954</td>
<td>10.179</td>
<td>10.389</td>
<td>10.579</td>
<td>10.739</td>
<td>10.865</td>
<td>10.960</td>
<td>10.994</td>
<td>9.489</td>
</tr>
</tbody>
</table>

Table A-XIV. Resistance measurements for 1 k ceramic composition
resistor as a function of frequency and temperature.

<table>
<colgroup>
<col style="width: 8%" />
<col style="width: 8%" />
<col style="width: 8%" />
<col style="width: 8%" />
<col style="width: 8%" />
<col style="width: 8%" />
<col style="width: 8%" />
<col style="width: 8%" />
<col style="width: 8%" />
<col style="width: 8%" />
<col style="width: 8%" />
<col style="width: 8%" />
</colgroup>
<tbody>
<tr class="odd">
<td></td>
<td colspan="11"><strong>Temperature</strong></td>
</tr>
<tr class="even">
<td><strong>Freq. (Hz)</strong></td>
<td><strong>25C</strong></td>
<td><strong>0C</strong></td>
<td><strong>-25C</strong></td>
<td><strong>-50C</strong></td>
<td><strong>-75C</strong></td>
<td><strong>-100C</strong></td>
<td><strong>-125C</strong></td>
<td><strong>-150C</strong></td>
<td><strong>-175C</strong></td>
<td><strong>-190C</strong></td>
<td><p><strong>25C</strong></p>
<p><strong>post</strong></p></td>
</tr>
<tr class="odd">
<td><strong>10</strong></td>
<td>993.11</td>
<td>1015.67</td>
<td>1042.71</td>
<td>1067.48</td>
<td>1090.87</td>
<td>1113.07</td>
<td>1132.11</td>
<td>1148.68</td>
<td>1162.15</td>
<td>1167.51</td>
<td>992.35</td>
</tr>
<tr class="even">
<td><strong>50</strong></td>
<td>993.06</td>
<td>1015.64</td>
<td>1042.64</td>
<td>1067.49</td>
<td>1090.83</td>
<td>1113.00</td>
<td>1131.95</td>
<td>1148.54</td>
<td>1162.04</td>
<td>1167.46</td>
<td>992.32</td>
</tr>
<tr class="odd">
<td><strong>100</strong></td>
<td>993.04</td>
<td>1015.61</td>
<td>1042.61</td>
<td>1067.47</td>
<td>1090.92</td>
<td>1112.97</td>
<td>1131.81</td>
<td>1148.66</td>
<td>1161.96</td>
<td>1167.47</td>
<td>992.30</td>
</tr>
<tr class="even">
<td><strong>200</strong></td>
<td>993.04</td>
<td>1015.60</td>
<td>1042.61</td>
<td>1067.49</td>
<td>1090.94</td>
<td>1112.94</td>
<td>1131.78</td>
<td>1148.62</td>
<td>1161.89</td>
<td>1167.47</td>
<td>992.31</td>
</tr>
<tr class="odd">
<td><strong>500</strong></td>
<td>993.04</td>
<td>1015.59</td>
<td>1042.62</td>
<td>1067.52</td>
<td>1090.97</td>
<td>1112.89</td>
<td>1132.00</td>
<td>1148.57</td>
<td>1161.86</td>
<td>1167.48</td>
<td>992.31</td>
</tr>
<tr class="even">
<td><strong>1K</strong></td>
<td>993.09</td>
<td>1015.63</td>
<td>1042.59</td>
<td>1067.62</td>
<td>1091.00</td>
<td>1112.86</td>
<td>1131.98</td>
<td>1148.57</td>
<td>1162.00</td>
<td>1167.51</td>
<td>992.31</td>
</tr>
<tr class="odd">
<td><strong>2K</strong></td>
<td>993.07</td>
<td>1015.62</td>
<td>1042.64</td>
<td>1067.58</td>
<td>1090.96</td>
<td>1112.80</td>
<td>1132.03</td>
<td>1148.43</td>
<td>1162.07</td>
<td>1167.55</td>
<td>992.34</td>
</tr>
<tr class="even">
<td><strong>5K</strong></td>
<td>993.08</td>
<td>1015.62</td>
<td>1042.61</td>
<td>1067.54</td>
<td>1090.91</td>
<td>1112.71</td>
<td>1132.00</td>
<td>1148.35</td>
<td>1162.04</td>
<td>1167.58</td>
<td>992.35</td>
</tr>
<tr class="odd">
<td><strong>10K</strong></td>
<td>993.06</td>
<td>1015.60</td>
<td>1042.59</td>
<td>1067.55</td>
<td>1090.89</td>
<td>1112.83</td>
<td>1132.01</td>
<td>1148.62</td>
<td>1162.08</td>
<td>1167.62</td>
<td>992.35</td>
</tr>
<tr class="even">
<td><strong>20K</strong></td>
<td>992.99</td>
<td>1015.55</td>
<td>1042.54</td>
<td>1067.43</td>
<td>1090.77</td>
<td>1112.84</td>
<td>1131.90</td>
<td>1148.49</td>
<td>1161.93</td>
<td>1167.54</td>
<td>992.27</td>
</tr>
<tr class="odd">
<td><strong>50K</strong></td>
<td>992.96</td>
<td>1015.48</td>
<td>1042.47</td>
<td>1067.36</td>
<td>1090.67</td>
<td>1112.79</td>
<td>1131.76</td>
<td>1148.49</td>
<td>1161.77</td>
<td>1167.46</td>
<td>992.24</td>
</tr>
<tr class="even">
<td><strong>100K</strong></td>
<td>992.93</td>
<td>1015.42</td>
<td>1042.45</td>
<td>1067.20</td>
<td>1090.66</td>
<td>1112.72</td>
<td>1131.40</td>
<td>1148.19</td>
<td>1161.46</td>
<td>1167.08</td>
<td>992.12</td>
</tr>
<tr class="odd">
<td><strong>200K</strong></td>
<td>996.39</td>
<td>1019.09</td>
<td>1046.29</td>
<td>1071.42</td>
<td>1094.82</td>
<td>1116.82</td>
<td>1135.71</td>
<td>1152.32</td>
<td>1165.57</td>
<td>1170.90</td>
<td>992.97</td>
</tr>
<tr class="even">
<td><strong>500K</strong></td>
<td>1009.09</td>
<td>1032.75</td>
<td>1061.00</td>
<td>1086.72</td>
<td>1110.61</td>
<td>1132.83</td>
<td>1151.85</td>
<td>1167.92</td>
<td>1180.66</td>
<td>1185.43</td>
<td>986.69</td>
</tr>
</tbody>
</table>

Table A-XV. Resistance measurements for 10 power film resistor as a
function of frequency and temperature.

<table>
<colgroup>
<col style="width: 8%" />
<col style="width: 8%" />
<col style="width: 8%" />
<col style="width: 8%" />
<col style="width: 8%" />
<col style="width: 8%" />
<col style="width: 8%" />
<col style="width: 8%" />
<col style="width: 8%" />
<col style="width: 8%" />
<col style="width: 8%" />
<col style="width: 8%" />
</colgroup>
<tbody>
<tr class="odd">
<td></td>
<td colspan="11"><h1 id="temperature-1">Temperature</h1></td>
</tr>
<tr class="even">
<td><strong>Freq. (Hz)</strong></td>
<td><strong>25C</strong></td>
<td><strong>0C</strong></td>
<td><strong>-25C</strong></td>
<td><strong>-50C</strong></td>
<td><strong>-75C</strong></td>
<td><strong>-100C</strong></td>
<td><strong>-125C</strong></td>
<td><strong>-150C</strong></td>
<td><strong>-175C</strong></td>
<td><strong>-190C</strong></td>
<td><p><strong>25C</strong></p>
<p><strong>post</strong></p></td>
</tr>
<tr class="odd">
<td><strong>10</strong></td>
<td>9.995</td>
<td>10.003</td>
<td>10.017</td>
<td>10.037</td>
<td>10.067</td>
<td>10.111</td>
<td>10.173</td>
<td>10.260</td>
<td>10.388</td>
<td>10.483</td>
<td>9.994</td>
</tr>
<tr class="even">
<td><strong>50</strong></td>
<td>9.995</td>
<td>10.003</td>
<td>10.017</td>
<td>10.037</td>
<td>10.067</td>
<td>10.111</td>
<td>10.173</td>
<td>10.260</td>
<td>10.386</td>
<td>10.484</td>
<td>9.994</td>
</tr>
<tr class="odd">
<td><strong>100</strong></td>
<td>9.995</td>
<td>10.003</td>
<td>10.017</td>
<td>10.037</td>
<td>10.067</td>
<td>10.111</td>
<td>10.173</td>
<td>10.261</td>
<td>10.387</td>
<td>10.484</td>
<td>9.994</td>
</tr>
<tr class="even">
<td><strong>200</strong></td>
<td>9.994</td>
<td>10.002</td>
<td>10.016</td>
<td>10.036</td>
<td>10.066</td>
<td>10.110</td>
<td>10.173</td>
<td>10.260</td>
<td>10.387</td>
<td>10.484</td>
<td>9.994</td>
</tr>
<tr class="odd">
<td><strong>500</strong></td>
<td>9.994</td>
<td>10.002</td>
<td>10.016</td>
<td>10.036</td>
<td>10.066</td>
<td>10.110</td>
<td>10.173</td>
<td>10.260</td>
<td>10.387</td>
<td>10.484</td>
<td>9.994</td>
</tr>
<tr class="even">
<td><strong>1K</strong></td>
<td>9.995</td>
<td>10.002</td>
<td>10.017</td>
<td>10.036</td>
<td>10.066</td>
<td>10.110</td>
<td>10.173</td>
<td>10.260</td>
<td>10.388</td>
<td>10.484</td>
<td>9.994</td>
</tr>
<tr class="odd">
<td><strong>2K</strong></td>
<td>9.994</td>
<td>10.002</td>
<td>10.016</td>
<td>10.036</td>
<td>10.066</td>
<td>10.110</td>
<td>10.173</td>
<td>10.259</td>
<td>10.388</td>
<td>10.484</td>
<td>9.994</td>
</tr>
<tr class="even">
<td><strong>5K</strong></td>
<td>9.994</td>
<td>10.002</td>
<td>10.016</td>
<td>10.036</td>
<td>10.066</td>
<td>10.110</td>
<td>10.173</td>
<td>10.259</td>
<td>10.387</td>
<td>10.484</td>
<td>9.994</td>
</tr>
<tr class="odd">
<td><strong>10K</strong></td>
<td>9.995</td>
<td>10.003</td>
<td>10.017</td>
<td>10.037</td>
<td>10.067</td>
<td>10.111</td>
<td>10.174</td>
<td>10.259</td>
<td>10.387</td>
<td>10.485</td>
<td>9.996</td>
</tr>
<tr class="even">
<td><strong>20K</strong></td>
<td>9.995</td>
<td>10.002</td>
<td>10.016</td>
<td>10.036</td>
<td>10.066</td>
<td>10.110</td>
<td>10.173</td>
<td>10.259</td>
<td>10.386</td>
<td>10.485</td>
<td>9.994</td>
</tr>
<tr class="odd">
<td><strong>50K</strong></td>
<td>9.994</td>
<td>10.002</td>
<td>10.016</td>
<td>10.036</td>
<td>10.066</td>
<td>10.109</td>
<td>10.172</td>
<td>10.259</td>
<td>10.387</td>
<td>10.484</td>
<td>9.995</td>
</tr>
<tr class="even">
<td><strong>100K</strong></td>
<td>9.993</td>
<td>10.001</td>
<td>10.015</td>
<td>10.035</td>
<td>10.065</td>
<td>10.109</td>
<td>10.171</td>
<td>10.258</td>
<td>10.386</td>
<td>10.483</td>
<td>9.995</td>
</tr>
<tr class="odd">
<td><strong>200K</strong></td>
<td>9.992</td>
<td>10.000</td>
<td>10.015</td>
<td>10.035</td>
<td>10.064</td>
<td>10.108</td>
<td>10.171</td>
<td>10.258</td>
<td>10.386</td>
<td>10.483</td>
<td>9.996</td>
</tr>
<tr class="even">
<td><strong>500K</strong></td>
<td>9.986</td>
<td>9.994</td>
<td>10.013</td>
<td>10.033</td>
<td>10.061</td>
<td>10.105</td>
<td>10.167</td>
<td>10.253</td>
<td>10.381</td>
<td>10.481</td>
<td>9.998</td>
</tr>
</tbody>
</table>

Table A-XVI. Resistance measurements for 1 k power film resistor as a
function of frequency and temperature.

<table>
<colgroup>
<col style="width: 8%" />
<col style="width: 8%" />
<col style="width: 8%" />
<col style="width: 8%" />
<col style="width: 8%" />
<col style="width: 8%" />
<col style="width: 8%" />
<col style="width: 8%" />
<col style="width: 8%" />
<col style="width: 8%" />
<col style="width: 8%" />
<col style="width: 8%" />
</colgroup>
<tbody>
<tr class="odd">
<td></td>
<td colspan="11"><strong>Temperature</strong></td>
</tr>
<tr class="even">
<td><strong>Freq. (Hz)</strong></td>
<td><strong>25C</strong></td>
<td><strong>0C</strong></td>
<td><strong>-25C</strong></td>
<td><strong>-50C</strong></td>
<td><strong>-75C</strong></td>
<td><strong>-100C</strong></td>
<td><strong>-125C</strong></td>
<td><strong>-150C</strong></td>
<td><strong>-175C</strong></td>
<td><strong>-190C</strong></td>
<td><p><strong>25C</strong></p>
<p><strong>post</strong></p></td>
</tr>
<tr class="odd">
<td><strong>10</strong></td>
<td>996.19</td>
<td>996.63</td>
<td>997.68</td>
<td>999.28</td>
<td>1001.73</td>
<td>1005.30</td>
<td>1010.45</td>
<td>1017.67</td>
<td>1028.55</td>
<td>1037.14</td>
<td>996.07</td>
</tr>
<tr class="even">
<td><strong>50</strong></td>
<td>996.15</td>
<td>996.60</td>
<td>997.65</td>
<td>999.25</td>
<td>1001.70</td>
<td>1005.27</td>
<td>1010.39</td>
<td>1017.60</td>
<td>1028.50</td>
<td>1037.13</td>
<td>996.02</td>
</tr>
<tr class="odd">
<td><strong>100</strong></td>
<td>996.14</td>
<td>996.59</td>
<td>997.62</td>
<td>999.23</td>
<td>1001.67</td>
<td>1005.25</td>
<td>1010.40</td>
<td>1017.53</td>
<td>1028.42</td>
<td>1037.10</td>
<td>996.01</td>
</tr>
<tr class="even">
<td><strong>200</strong></td>
<td>996.14</td>
<td>996.59</td>
<td>997.63</td>
<td>999.24</td>
<td>1001.67</td>
<td>1005.27</td>
<td>1010.44</td>
<td>1017.61</td>
<td>1028.35</td>
<td>1037.10</td>
<td>996.00</td>
</tr>
<tr class="odd">
<td><strong>500</strong></td>
<td>996.14</td>
<td>996.59</td>
<td>997.63</td>
<td>999.25</td>
<td>1001.67</td>
<td>1005.28</td>
<td>1010.44</td>
<td>1017.63</td>
<td>1028.42</td>
<td>1037.08</td>
<td>996.01</td>
</tr>
<tr class="even">
<td><strong>1K</strong></td>
<td>996.20</td>
<td>996.60</td>
<td>997.64</td>
<td>999.29</td>
<td>1001.70</td>
<td>1005.32</td>
<td>1010.51</td>
<td>1017.67</td>
<td>1028.45</td>
<td>1037.06</td>
<td>996.01</td>
</tr>
<tr class="odd">
<td><strong>2K</strong></td>
<td>996.17</td>
<td>996.63</td>
<td>997.67</td>
<td>999.28</td>
<td>1001.71</td>
<td>1005.31</td>
<td>1010.50</td>
<td>1017.69</td>
<td>1028.49</td>
<td>1037.07</td>
<td>996.05</td>
</tr>
<tr class="even">
<td><strong>5K</strong></td>
<td>996.18</td>
<td>996.64</td>
<td>997.69</td>
<td>999.29</td>
<td>1001.72</td>
<td>1005.32</td>
<td>1010.53</td>
<td>1017.66</td>
<td>1028.48</td>
<td>1037.07</td>
<td>996.09</td>
</tr>
<tr class="odd">
<td><strong>10K</strong></td>
<td>996.19</td>
<td>996.64</td>
<td>997.71</td>
<td>999.32</td>
<td>1001.76</td>
<td>1005.32</td>
<td>1010.53</td>
<td>1017.63</td>
<td>1028.42</td>
<td>1037.06</td>
<td>996.20</td>
</tr>
<tr class="even">
<td><strong>20K</strong></td>
<td>996.11</td>
<td>996.56</td>
<td>997.61</td>
<td>999.21</td>
<td>1001.66</td>
<td>1005.20</td>
<td>1010.38</td>
<td>1017.47</td>
<td>1028.27</td>
<td>1036.94</td>
<td>995.99</td>
</tr>
<tr class="odd">
<td><strong>50K</strong></td>
<td>995.98</td>
<td>996.44</td>
<td>997.46</td>
<td>999.05</td>
<td>1001.47</td>
<td>1005.02</td>
<td>1010.14</td>
<td>1017.35</td>
<td>1028.07</td>
<td>1036.67</td>
<td>995.94</td>
</tr>
<tr class="even">
<td><strong>100K</strong></td>
<td>995.64</td>
<td>996.00</td>
<td>996.96</td>
<td>998.51</td>
<td>1000.97</td>
<td>1004.48</td>
<td>1009.47</td>
<td>1016.64</td>
<td>1027.33</td>
<td>1035.61</td>
<td>995.94</td>
</tr>
<tr class="odd">
<td><strong>200K</strong></td>
<td>995.16</td>
<td>995.37</td>
<td>996.30</td>
<td>997.63</td>
<td>999.66</td>
<td>1002.80</td>
<td>1007.55</td>
<td>1014.24</td>
<td>1024.38</td>
<td>1032.00</td>
<td>995.77</td>
</tr>
<tr class="even">
<td><strong>500K</strong></td>
<td>985.01</td>
<td>984.50</td>
<td>984.88</td>
<td>984.88</td>
<td>985.67</td>
<td>987.94</td>
<td>990.80</td>
<td>995.26</td>
<td>1001.74</td>
<td>1005.54</td>
<td>994.48</td>
</tr>
</tbody>
</table>