Device for measuring the average value of pulse signals

Pulse or digital communications – Testing – Signal noise

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Details

364575, 364734, H04B 346, H04B 1700

Patent

active

054167981

DESCRIPTION:

BRIEF SUMMARY
FIELD OF THE INVENTION

The present invention relates to a device for measuring the average value of pulse signals such as impulsive noises.


BACKGROUND ART

FIG. 1 shows a pulse noise average value measuring and display device which is used in a conventional field intensity measuring instrument or field intensity meter. An input signal from an input terminal 11 is adjusted by a variable attenuator 12 to a proper level and is then supplied to a frequency converter 13. The frequency converter 13 is supplied with a local signal from a local oscillator 14, and the input signal converted by the frequency converter 13 to an intermediate frequency is amplified by an intermediate-frequency amplifier 15. By a suitable selection of the frequency of the local signal from the local oscillator 14, an input signal of a desired frequency can be obtained as the output of the intermediate-frequency amplifier 15. From the output of the intermediate-frequency amplifier 15 is extracted by a band-pass filter 16 a specified frequency component (9 kHz or 120 kHz) according to the rules of the Comite International Special des Perturbations Radioelectriques (CISPR), and the output of the band-pass filter 16 is provided to a linear detector (or envelope detector) 17, wherein its peak value is detected, and the detected output is integrated by an integrating circuit 18. The integrated output is amplified by an amplifier 19 and its level is displayed on a display 21.
When such impulsive noises 22 as shown in FIG. 2A are provided as input signals to the input terminal 11, the linear detector 17 yields an impulse 23 corresponding to the waveform of each impulsive noise at one polarity side as shown in FIG. 2B. Such impulses are averaged by the integrating circuit 18 as depicted in FIG. 2C. That is, the area of the impulse 23 and the area of that portion of the integrated output above the zero level become equal to each other in FIG. 2A-2D.
In the case where the pulse width is remarkably small and the pulse interval T.sub.1 is long relative to the peak value of the impulsive noise 22, the level of the integrated output becomes very low. For instance, when the pass frequency of the band-pass filter 16 is 120 kHz, the smallest pulse width W.sub.1 of the pulse 23 available from the linear detector 17 is 0.9 .mu.S (1/120 kHz). If the repetition frequency of the impulsive noise 22 is 100 kHz, the output of the integrating circuit 18, that is, the average value of the pulse 23, becomes 90 .mu.V, even if the peak value V.sub.p1 of the pulse 23 is 1 V. Thus the level difference between the peak value of the pulse 23 and the integrated output is as large as 81 dB.
As mentioned above, when the impulsive noise 22 is very short and its period of generation T.sub.1 is long, the output level of the integrating circuit 18 drops very low, sometimes, close to or below the noise level. If the attenuation of the variable attenuator 12 is set small so as to avoid such a situation, the frequency converter 13 and the intermediate-frequency amplifier 15 are supplied with pulse signals of large peak values and become saturated, providing waveform distortions. For these reasons, it has been impossible to accurately measure the average value of pulse signals of extremely long pulse intervals.
The integrating circuit 18 performs integration through use of a CR circuit. To remove ripples from the integrated output and hence sufficiently smooth it, the CR time constant for the integration needs to be selected sufficiently larger, for example, about 100 times larger than the interval T.sub.1 of the impulsive noise 22. Since the interval T.sub.1 is 1 sec or so in some cases, the above-mentioned time constant is usually set to approximately 100 sec. This poses another problem that a large amount of time is needed to obtain accurate measured values.
The prior art uses a spectrum analyzer to measure the frequency components of impulsive noises. The conventional spectrum analyzer is shown in FIG. 3. The input signal from the input terminal 11 is adjusted by the variabl

REFERENCES:
patent: 4596024 (1986-06-01), Thomson
patent: 4680540 (1987-07-01), Niki et al.
patent: 4714929 (1987-12-01), Davidson
patent: 5052027 (1991-09-01), Poklemba et al.

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