MIL-STD-202H.pdf - 第268页

MI L - S TD - 202 - 308 CO NT E N T S PARAGRAPH PAG E FOREW ORD … ………………………………………………………. ii 1. SCOPE 1 1.1 Purpose …… ………………… …………………. …… .. …………. 1 1.2 Precaution s …………………… …………. ……. ……. . …………. 1 1.3 Checks for c o nf…

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MIL-STD-202-308
FOREWORD
1. This standard is approved for use by all Departments and Agencies of the Department of Defense.
2. This entire standard has been revised. This revision has resulted in many changes to the format, but the most
significant one is the splitting the document into test methods. See MIL-STD-202 for the change summary.
3. Comments, suggestions, or questions on this document should be emailed to std202@dla.mil or addressed to:
Commander, Defense Logistics Agency, DLA Land and Maritime, ATTN: VAT, P.O. Box 3990, Columbus, OH
432183990. Since contact information can change, you may want to verify the currency of this address
information using the ASSIST Online database at https://assist.dla.mil.
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MIL-STD-202-308
CONTENTS
PARAGRAPH PAGE
FOREWORD………………………………………………………. ii
1. SCOPE 1
1.1 Purpose………………………………………….……..…………. 1
1.2 Precautions……………………………….…….……..…………. 1
1.3 Checks for conflicts………………..……………………………. 1
2. APPLICABLE DOCUMENTS 1
3. DEFINTIONS 2
4. GENERAL REQUIREMENTS 2
4.1 Apparatus…………….…….……..……………..........……. 2
4.1.1 Test system............................................................................ 2
4.1.1.1 DC measurement considerations…….………………..………. 2
4.1.1.2 AC measurement considerations….…………………..………. 2
4.1.1.3 Calibration technique…………………..…………………….…. 2
4.1.2 Synopsis….….…….………….………….………...…………. 2
4.2. Procedure…………….………………………..….….………….. 3
4.2.1 Operating conditions………………………..……..……………. 3
4.2.2 Measurements…….……………………………….…………….. 3
4.2.2.1 Calibration….……………………………………….…………….. 3
4.2.2.2 System noise (S)…………………………………..…………….. 5
4.2.2.3 Total noise (T)………....…………………………..…………….. 5
4.2.3 Determination of the "microvolts-per-volt-in-a-decade" index.. 6
4.3 Errors…………………………………………………………….. 6
5. DETAILED REQUIREMENTS 8
5.1 Summary…………………………………………..…..…………. 8
5.2. Examination and measurements………………………....…. 8
5.2.1 Marking resistance to solvents…….……………..……………. 8
5.2.2 Component protective coating, encapsulation material
and sleeve material resistance….……………..………………. 8
6. NOTES 8
6.1 Supersession data……………………………………………. 8
FIGURES PAGE
1. Block diagram of system ..……………………….……………………… 3
TABLES PAGE
1. Standard operating conditions ..……………….……………….…… 4
2. Correction factor for presence of "system noise".………………….…… 7
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MIL-STD-202-308
METHOD 308
CURRENT-NOISE TEST FOR FIXED RESISTORS
1. SCOPE
1.1 Purpose. This resistor noise test method is performed for the purpose of establishing the "noisiness" or "noise
quality" of a resistor in order to determine its suitability for use in electronic circuits having critical noise requirements.
This method is intended as a standard reference for the determination of current noise present in a resistor, for use in
an application with specific current-noise requirements. It is not intended as a general specification requirement.
Interference caused by the generation of spurious noise signals in parts tends to mask the desired output signal, thus
resulting in loss of information. For low-level audio frequency and other low-frequency circuits, where low-noise parts
are used, resistors may become an important source of interfering noise. One source of noise in a resistor is
molecular thermal motion which generates a fluctuation voltage termed "thermal noise". It is not necessary to
determine the magnitude of thermal noise by measurement since the mean-square value of the fluctuation voltage is
predictable from Nyquist's equation, which shows the mean-square value to be proportional to the product of
resistance, temperature, and the pass band of the measuring system. Generally, an increase in fluctuation voltage
appears when direct current (dc) is passed through resistive circuit elements. The increase in fluctuation voltage is
termed "excess noise" or "current noise". The magnitude of current noise is dependent upon many inherent
properties of the resistor such as resistive material and other factors such as processing, fabrication, size and shape
of resistive element, etc. Since there is no apparent functional relationship between current noise and many of these
factors, current noise generally cannot be predicted from physical constants. Therefore, it is necessary to measure
current noise to determine its magnitude. The method employed in this test has been designed to evaluate
accurately the "noisiness" or "noise quality" of individual resistors in terms of a noise-quality index. The noise-quality
index, expressed in decibels (dB), is a measure of the ratio of the root-mean-square (rms) value of current-noise
voltage, in microvolts (µv), to the applied dc voltage, in volts. The pass band associated with the noise-quality index
is one frequency decade, geometrically centered at 1,000 hertz (Hz). This index is termed the "microvolts-per-volt-in-
a-decade" index. In the design of circuits, an added advantage accrues from the definitiveness of the index which
allows the estimation of interference attributable to current noise. Conversely, for a given limit of current-noise
interference in a particular circuit design, a maximum acceptable value of the index may be established. Ordinarily, it
is not necessary to duplicate the operating conditions of the particular circuit design when measuring the current
noise. The noise quality of populations of resistors may be reasonably estimated by measurement of the index of
representative groups of resistors using suitable sampling procedures. Measurements on sample groups tend to
have a normal distribution and once representative parameter values for the distribution have been established (the
mean and standard deviation), such parameter values would serve as norms in judging "noisiness" and product
uniformity insofar as noise is concerned.
1.2 Precautions. Adherence to the ambient temperature specified in 4.2.1 is emphasized as an important
consideration of this method. It is also necessary, in making noise measurements, using the apparatus of this
method, to delay reading the noise meter for a period of time no less than four times the effective time constant of the
detector to allow the meter sufficient time to reach at least 98 percent of the representative average value. The
effective time constant of the apparatus is normally adjusted to a value close to 1 second and therefore, a minimum
time delay of 4 seconds is normally required for the noise meter to indicate a valid average. Immediately after this 4
second delay, the meter should be read even though it continues to fluctuate as the noise signal varies. Normally,
the operator in making a visual reading of the fluctuating meter pointer, should estimate an average for a short
duration, in the order of 1/2 to 1 second.
1.3 Checks for conflicts. When this test is referenced, care should be exercised to assure that conflicting
requirements, as far as the properties of the specified finishes and markings are concerned, are not invoked.
2. APPLICABLE DOCUMENTS
This section not applicable to this standard.
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