# Oscillograph, Cathode-Ray

The following article is from The Great Soviet Encyclopedia (1979). It might be outdated or ideologically biased.

## Oscillograph, Cathode-Ray

an instrument for observing the relationship between two or more parameters or functions, which can be electrical or convertible into electrical impulses. The electrical signals that represent the parameter or function are fed to two mutually perpendicular pairs of deflection plates in a cathode-ray tube. The cathode ray produces a graphic image—an oscillogram—on the tube’s screen that can be observed, measured, and photographed. An oscillogram usually depicts the shape of an electrical signal with respect to time. From it can be determined the polarity, amplitude, and duration of the signal.

An oscillograph is frequently calibrated in volts on the vertical scale of the tube’s screen and in seconds on the horizontal scale. Thus, the amplitude and temporal characteristics of an entire signal or parts of a signal can be simultaneously measured and observed, as well as the parameters of random signals or signals that appear only once and are not prolonged. In some apparatus, the image of the signal under study is compared with that of a calibrating signal or the balanced method of measurement is used (seeBALANCED METHOD).

Figure 1. Simplified block diagram of a cathode-ray oscillograph

Figure 1 is a simplified diagram of an oscillograph circuit. The signal under study, A, is fed to the input amplifier for vertical deflection, which has an adjustable gain and is designed to make the magnitude of the beam deflection correspond to the magnitude of the input signal. The beam is moved horizontally by a time-base generator that produces a sawtooth voltage, D, which varies linearly with time. The sawtooth voltage is fed to the input of the horizontal-deflection amplifier, which in turn feeds its output voltage, F, to the horizontal-deflection plates of the tube. The electron beam is moved horizontally at a constant rate, thus creating the linear time base. The sweep rate is adjustable.

In order to project on the tube’s screen a stable image of the signal under study, every new sweep must begin at the same phase of the signal. This is achieved by passing the signal from the vertical amplifier to a synchronizer that forms a trigger pulse, C, for the time base at a selected point in the signal. In order that the electron beam may be visible only while it is sweeping forward, that is, when t2t1 > 0, the time base produces a pulse, E, to brighten the beam that is fed to the tube’s control grid, which acts as a modulator. The pulse is a square wave with positive polarity and a duration equal to that of the forward sweep of the beam. Since the signal under study triggers the time base, and since the synchronizer and time base do not respond instantly but with a delay of fractions of a microsecond, a delay line must be introduced in the vertical-deflection channel in order that the initial part of the signal be observed.

The delay line compensates for the operating times of the synchronizer and the time base, since these times are slightly shorter than the time delay of the signal. In the absence of a delay line, only that part of the signal (represented in Figure 1 by curve B) that appears after time t\ is visible on the tube’s screen. An oscillograph also includes high-voltage and low-voltage power supplies. The former only supplies the tube, while the latter supplies the electronic circuit of the other components and sub-units of the apparatus.

The important specifications of an oscillograph that determine its possible uses are (1) the deflection sensitivity, which is the ratio of the input-signal voltage to the beam deflection that is produced by the voltage and which is measured in volts (V) per cm or V per gradation; (2) the passband, which is the frequency range in which the deflection sensitivity drops no more than 3 decibels (dB) from its value at the middle, or reference, frequency; (3) the rise time, τr, during which the transient response of the oscillograph rises from 10 percent to 90 percent of the amplitude value, which is often used instead of the passband; the upper-boundary frequency fu of the passband is related to τr by the equation fu = 0.35/TR where fu is measured in megahertz (mHz) and τr in nanoseconds (nsec); (4) the deflection factor, which is the ratio of the time τr to the amount of beam deflection produced by the time-base voltage during τr, expressed in sec per cm or sec per gradation; and (5) the writing speed, which is the maximum speed at which the beam can move on the screen and still guarantee that a one-time signal will be photographed or—in storage oscillographs—retained. These specifications determine the amplitude, duration, and frequency ranges of the signals to be studied.

The degree of error in measurement of signals depends on the degrees of error in the deflection sensitivity and the deflection factor, which are usually about 2 to 5 percent. It also depends on the frequency and duration of the signal under study, on the passband, and on the rise time, Tr, of the signal. Signal parameters that are greater than or equal to 5 Tr can be reproduced on oscillograph screens with an error equal to or falling short of 2 percent.

In place of the degrees of error in deflection sensitivity and deflection factor, similar degrees of error in the amplitude measurement of a standard signal and a time-interval measurement are often used. The standard signal is a sinusoid at a specified frequency or a square-wave pulse of significant duration.

In order to study two or more signals simultaneously, multi-trace oscillographs and a multichannel electronic switch in the vertical-deflection channel are used. The electronic switch permits the image of several signals to be obtained on a single-beam tube by successively connecting the sources of these signals to the vertical-deflection channel. Electronic switches are generally used to study the phase relationships between several synchronous signals.

In order to examine a portion of a signal, for instance, a portion that appears much later than the signal’s initiation, the time base is stretched: part of the sawtooth voltage that is fed to the input of the horizontal-deflection amplifier is amplified several times, a process that is equivalent to increasing the length of the time base. Another method is to delay triggering the time base, which is equivalent to stretching the time base by a factor of several thousand.

The most widely applicable oscillograph is one with interchangeable units for vertical and horizontal deflection. By rearranging the units it is possible to design several types of oscillographs, including wide-band, high-sensitivity, two- or four-channel, and differential ones. Depending on its circuit features, an oscillograph can be all-purpose, storage, sampling, high-speed, or specialized (see Table 1). The oscillograph on which Figure 1 is based is an all-purpose type.

Storage oscillographs have charge-storage tubes. They retain an image of a signal for a long time and are therefore useful in studying one-time and infrequently repeated signals. The writing speed of storage oscillographs attains several thousand km per sec. The playback time of a recorded image ranges from 1 to 30 minutes for various models. As a rule, these oscillographs are able to store an image over a span of several days, even when the apparatus has been turned off during that time. The block diagram of a storage oscillograph differs from Figure 1 in having an extra unit that controls the operations of the storage tube, including writing, image-reproduction, and image irradication.

The sampling oscillograph successively samples the instantaneous values of a signal in order to transform the signal’s spectrum; each time the signal is repeated, its instantaneous value is determined at one point. When the next signal arrives, the sampling point is shifted along the signal; this process continues until the entire signal has been sampled. The transformed signal consists of a series of instantaneous values for the original

Table 1. Specifications of some types of oscillographs
All-purpose . .USSRS1=650–355–50.01–0.05
All-purpose . . .USSRS1=750–25010–10.002–0.11,500
All-purpose . . .USATektronix-4850–3505–50.001–0.524,000
High-speed . . .USSRS7 = 10A0–1,500100–0.22.5 × 10–5–0.1 × 10–6
Sampling . . .USSRS7 = 110–5,0005–0.25 × 10–5–1 × 10–5
Storage. . . . .NetherlandsPhilips PM-32510–502–200.1–0.510
Storage. . . . .USSRS8 = 120–5010–50.01–154,000
Storage. . . . .USSRS8 = 130–10.5–200.01–155
Sampling . . . . .JapanIwatsu0–18,00010–0.210–5–5 × 10–2
Specialized … (television)USSRSAS-5009B S9 = 570–1510–100.1–0.02

input signal, whose shape it reproduces. The duration of the transformed signal is many times longer than that of the original, and therefore the original spectrum is compressed; this is equivalent to a corresponding broadening of the passband. A sampling oscillograph has the widest bandwidth and accommodates periodic signals with a duration of about 10–11 secs.

High-speed oscillographs have tubes with traveling-wave vertical deflection. Their features include a broad band—from 1 to 5 × 109 mHz—and high writing speed. The high-speed oscillographs have no amplifier in the vertical-deflection channel and, in contrast to the sampling types, are able to examine not only periodic but also one-time high-speed signals. Specialized oscillographs are used to study, for example, television or high-voltage signals.

### REFERENCES

Vishenchuk, I. M., E. P. Sogolovskii, and B. I. Shvetskii. Elektronnoluchevoi ostsillograf i ego primenenie v izmeritel’noi tekhnike. Moscow, 1957.
Novopol’skii, V. A. Elektronnoluchevoi ostsillograf. Moscow, 1969.
Czech, I. Ostsillografy v izmeritel’noi tekhnike. Moscow, 1965. (Translated from German.)
Vyrazhenie svoistv elektronnoluchevykh ostsillografov. Rekomendatsii po standartizatsii Mezhdunarodnoi elektrotekhnicheskoi komissii, no. 351. Moscow, 1971.
Ostsillografy elektronnoluchevye: Katalog. Moscow, 1971.

A. A. KALAMKAROV and A. I. FEDORENCHIK