CA1256196A - Measurement of subcarrier to horizontal sync phase using a polar display - Google Patents

Abstract

Abstract:
The present invention relates to an instrument for use in indicating subcarrier to horizontal sync (SC/H) phase of a composite video signal. The instrument is comprised of a display device for providing a polar display, including a unit for generating from a reference subcarrier burst of the video signal a first input signal for the display device such as to cause the display device to display an indication at a predetermined angular position of the polar display. The instrument further comprises a phase determining and indicating unit for determining a time difference between a sync point and that zero crossing of the extrapolated subcarrier wave which is closest to the sync point and for generating from the time difference a second input signal for the display device such as to cause the display device to display an indication at a position of the polar display that is angularly spaced from a pre-determined axis of the polar display by an angle given by the fraction having as its denominator the period of the reference subcarrier wave and as its numerator the product of the time difference and 360 degrees.

Description

~2S~

Measurerlent of subcarr~er to h~r~zontal_sync phase using a ~olar dis~lay This is a division of copending Canadian Patent Application Serial No. 477,368 which was filed on March 25, 1985.
This invention relates to the measurement of subcarrier to horizontal sync (SC~H) phase using a polar display.
The background for this invention will be disclosed in detail hereinbelow.

Summary of the Invention According to an aspect of the present invention there is provided an instrument for use in indicating SC/H phase of a composite video signal, comprising a display device for providing a polar display, a device for generating from the reference subcarrier burst of the video signal a first input signal for the display device such as to cause the display device to display an indication at a predetermined angular position of the polar display, phase determining and indicating means for determining the time difference between the sync point and that zero crossing of the extended subcarrier wave which is closest to the sync point and for generating from said time difference a second input signal for the display device such as to cause the display device to display an indication at a position of the polar display that is angularly spaced from a predetermined axis of the polar display by an angle ~256196 given by the fraction having as its denominator the period of the reference subcarrier wave and as its numerator the product of said time difference and 360 degrees.
The present invention may be used to enable a vector-scope to provide an indication of SC/H phase. In theconventional vectorscope, the reference subcarrier burst is indicated by a vector on the 180 degree radius (-x direction in Cartesian coordinates). In accordance with the present invention, the time difference between the sync point and the closest zero crossing of the extended subcarrier wave is determined and the time difference is converted to an angular measure within the subcarrier wave cycle. The vectorscope can then be used to display an indication in accordance with the angle corresponding to the time difference, preferably in the form of a dot. In the event that the datum radius from which the angle is measured is the 180 degree radius, the dot is aligned with the subcarrier vector when the subcarrier is in phase with - horizontal sync. Thus, the present invention enables a vectorscope to be used to provide an indication of SC/H
phase.

Brief DescriE~on of_ he Drawin~s The present invention taken in conjunction with the invention described in copending Canadian Patent Application Serial No. 477,368 which was filed on March 25, 1985, will be described in detail hereinbelow with the aid of the accompanying drawings, in which:
FIG. 1 illustrates diagrammatically the waveform of the NTSC video signal during the horizontal blanking interval, FIG. 2 illustrates in block form the major components of a conventional vectorscope for use in the NTSC system, FIGq 3 illustrates in block form a vectorscope embodying the present invention, adapted for use in the NTSC system, ~256~96 FIG. 4 illustrates waveforms useful in understanding operation of the FIG. 3 vectorscope, FIG. 5 illustrates the display provided by the FIG. 3 vectorscope, 5FIG. 6 illustrates in block form a second vectorscope embodying the present invention, FIG. 7 illustrates the display provided by the FIG. 6 vectorscope, FIG. 8 (appearing on the same sheet of drawings as Figure 5) illustrates a waveform useful in understanding operation of a vectorscope embodying the invention, adapted for use in the PAL system, FIG. 9 (appearing on the same sheet of drawings as Figure 5) illustrates the display provided by the FIG. 3 vectorscope, adapted for use in the PAL system, and FIGS. 10, 11 and 12 illustrate in block form additional embodiments of the invention.
Detailed Description It is well known that the composite color video signals that are conventionally broadcast, for example in the NTSC format, contain not only picture information (luminance and chrominance components) but also timing information (vertical sync pulses and horizontal sync pulses) and other reference information (e.g. equalizing pulses and color burst). As shown in FIG. 1, the horizontal sync pulse 2 and burst 4 both occur in the horizontal blanking interval, i.e., the interval between the active line times of consecutive horizontal scan lines. The horizontal sync pulse is a negative-going pulse having an amplitude of 40 IRE units, the 50 percent point 6 of the leading edge of the sync pulse regarded as the horizontal sync point. Burst follows the horizontal sync pulse in the horizontal blanking interval and comprises a sinusoidal wave. The peak-to-peak amplitude of the burst is 40 IRE units, and immediately before and after the burst the signal is at blanking level (zero IRE). The burst ideally has a sin-squared envelope, and builds up from, and decays to, blanking level within one or two cycles of the burst wave. In accordance with EIA
(Electronics Industries Associationl standard RS 170 A, the start of burst is defined by the zero-crossing (positive or negative slope) that precedes the first half cycle of subcarrier that is 50 percent or greater of the burst amplitude, i.e., 40 IRE. The reference subcarrier burst is used in the television receiver to control a phase-locked oscillator which generates a continuous wave at subcarrier frequency and is used to extract the chrominance information from the composite video signal.
Although the NTSC frame is made up of 525 lines which are scanned in two interlaced fields of 262.5 lines each, the NTSC color signal requires a four field sequence. In accordance with the definitions of the fields contained in standard RS 170 A, the zero crossing of the extrapolated color burst (the continuous wave at subcarrier frequency and in phase with burst) must be coincident with the sync point of the immediately preceding horizontal sync pulse on even numbered lines, and the pattern of sync and burst information for fields 1 and 3 is identical except for the phase of burst. Thus, in field 1, the positive-going zero crossing of the extrapolated color burst coincides with the sync point on even numbered lines whereas in field 3 it is the negative-going zero crossing that coincides with the sync point on even numbered lines. Standards such as that set forth in RS 170 A are required in order to facilitate matching between video signals from different sources and also to facilitate operation of video signal recording and processing equipment. Accordingly, in order to identify the different fields of the four field color sequence, and to adjust the subcarrier to horizontal sync (SC/H) phase so as to achieve the desired coincidence between the zero crossing point of the extrapolated color burst and the sync point, it is necessary to be able to measure the phase of the subcarrier burst relative to the sync point.

12~196 Several attempts have previously been made to measuee SC/H phase. For example, using the Tektronix 1410 signal generator, it is possible to generate a subcarrier in the middle of an unused line. Since the leading edges of the equalizing pulses are midway between sync pulses, a measurement of subcarrier to horizontal sync phase can be implied by comparing the subcarrier with the equalizing pulse timing. Alternatively the 1410 signal generator can generate a burst phased subcarrier during horizontal blanking which replaces a sync pulse and which can be compared with the remaining sync pulses. However, this equipment is not always available to technicians who need to make SC/H phase measurements. The GVG 3258 SC/H phase meter provides a digital output of the phase difference between subcarrier and horizontal sync, but this again requires availability of dedicated equipment.
The vectorscope, which provides a polar display of the amplitude and phase of signal components at subcarrier frequency, is commonly used by video engineers and technicians, but the coventional vectorscope cannot be used to measure SC/H phase.
As used in this description and the appended claims, the term "vectorscope" means an instrument having an input terminal, a display surface, means for generating a visible dot on the display surface, X and Y deflection means for deflecting the position of the visible dot in mutually perpendicular rectilinear directions, a subcarrier re-generator connected to the input terminal for generating a continuous wave signal at subcarrier frequency from, and phase-locked to, the subcarrier burst of a video signal, first and second demodulators having their outputs con-nected to the X and Y deflection means respectively and each having first and second inputs, means connecting the , ~2 S 6~LS~6 output of the subcarrier regenerator to the first inputs of the first and second demodulators with a quarter-period relative phase difference, and a filter which passes the subcarrier burst of the video signal and has an output terminal for connection to the second inputs of the first and second demodulators. The vectorscope provides a polar display of the amplitude and phase of signal components at subcarrier frequency.
FIG. 2 of the drawings illustrates in block form the major components of a conventional vectorscope having a CRT 10. The composite video input signal is applied by way of an input terminal 12 to both a 3.8 MHz bandpass filter 14 and a burst locked oscillator 16. The burst locked oscillator 16 generates a continuous wave signal lS. at subcarrier frequency (3.58 MHz) phase locked to burst.
The bandpass filter 14 passes components of the compo-~25S196 site video signal that have a frequency of 3.58MHz, i. e., burst and the color components present during the active line time of the video signal.
The output signal from the filter 14 is applied to two demodulators 18 and 20, which may simply be multipliers. The output of the oscillator 16 is applied through a variable phase shifter 22 directly to the demodulator 18 and to the demodula-tor 20 through a quarter period lof subcarrier frequency) delay 24. The output of the demodulator 18 is applied to the %-deflection plates of the CRT
10. The output of the demodulator 20 is applied to the Y-deflection plates of the CRT. It will thus be understood that the vectorscope provides a dis-play in polar coordinates of the amplitude andphase relative to burst of each of the color compo-nents present in the composite video signal. By using the phase shifter 22 to rotate the entire display and align the vector representing burst with a predetermined axis of the display, usually the -X axis, a technician can determine whether the subcarrier components present in a test signal comply with prescribed standads defined by fixed graticule markinqs. However, the conventional vectorscope display yields no information concer-ning SC/H phase.
In the case of the vectorscope shown in FIG.
3, the composite video signal is also used to generate a signal representative of SC/H phase.
As shown in FIG. 3, the composite video signal is applied to a phase locked oscillator 28 which generates a continuous wave 3.58 MHz signal. On even numbered lines, a positive-going zero crossing of the continuous wave signal coincides in time with the sync point and on odd numbered lines a ~25619~;

negative-going zero crossing of the continuous wave coincides with the sync point. This phase reversal of the continuous wave, which may be accomplished by switching in a half-period delay on alternate lines, compensates for the 180 degree change in the phase relationship between sync and burst on conse-cutive lines in the NTSC system, and consequently the phase relationship between burst and the con-tinuous wave signal does not change from line to line.
The sync locked CW signal and the output of the chroma filter 14 are applied to a switch 30, which is controlled by a control logic circuit 32.
~he control logic 32 controls not only selection between the filter 4 and the oscillator 28 but also Z-axis blanking of the CRT 10 by a blanking circuit 34. The manner of operation of the control logic 32 when the vectorscope is in SC/H phase display , mode is indicated in FIG. 4, in which the waveform (a) represents the composite video signal, the waveform ~b~ represents the state of the switch 30 and the waveform (c) represents the state of the blanking circuit 34. When the vectorscope is in . its normal display mode, the control logic 32 causes the switch 30 to select continuously the filter 14, and the vectorscope functions in ~he manner described with reference to FIG; 2. When the vectorscope is operating in its SC/H phase display mode, the control logic 32 causes the switch to select the output of the filter 14 (wave-form (b) low) only during sync and burst time, and to select the sync locked CW (waveform (b) high) during the remainder of the line time. The control loqic 32 also controls the Z-axis blanking circuit 34 to blank the CRT 10 (waveform (c) low) during ~259fil9~;

the switches between the filter 34 and the oscilla-tor 28 and to unblank the CRT (waveform ~c) high) for a portion of the time for which the filter 14 is selected, so as to provide the center dot 40 and S burst vector 42 on the display, as shown in FIG. 5.
~he CRT is also unblanked for a portion of the active line time, during which the sync locked CW
is selected, to display a vector representing the phase and amplitude of the sync locked CW on those lines. The duration of the latter unblanking is varia~l~ to control the intensity of the display of the sync locked CW vector relative to the burst vector and center dot. Preferably, the unblanking time is chosen so that only the outer extremity of the sync locked CW vector is visible, and therefore the sync locked CW vector is indicated by a dot 44.
The amplitude of the sync locked CW is greater than that of burst, and therefore the sync locked CW
vector extends beyond the burst vector and the dot 44 indicating sync locked CW is visually distin-guishable from the burst vector even when it is disposed at the same angular position of the polar display. If the sync locked CW is in phase with burst, the dot 44 is at the same angular position of the polar display as the burst vector 42.
If the phase of the CW signal provided by the oscillator were not reversed on consecutive lines, the change in phase relationship between sync and burst on consecutive lines would result in display of two sync locked CW vectors (or dots) for odd ` numbered lines and even numbered lines respective-ly, and it might be difficult to determine which vector ~or dot) represents the sync locked CW for even numbered lines. An alternative way of avoiding this problem would be to proqram the con-trol logic 32 so that the CRT remains blankedduring the entire active line time for odd numbered lines.
In the production of a television transmission using several video signal sources, it is necessary in order to avoid unacceptable signal degradation upon switching from a first source to a second source to ensure that the correct color frame rela-tionship exists between the signals from the two sources. This can be done by ensuring that the subcarrier burst of each signal is in phase with sync of that signal, and that the bursts of the respective signals are in phase with each other.
The vectorscope shown in FIG. 6 can be used to examine simultaneously the SC/H phase of two video signals.
In the case of FIG. 6, the signal being trans-mitted Ithe reference signal~ is applied through an , input terminal 46 to the burst locked oscillator 16 and to a first sync locked oscillator 28a. The signal that is to be selected (the selected signal) is applied through an input terminal 48 to a second sync locked oscillator 28b and to the bandpass filter 14. The outputs of the filter 14 and the oscillators 28 are applied to a switch 30' which selects among these outputs under control of the control logic 32'. The control logic causes the switch to select the output of the filter 14 only during burst and sync time of the selected video signal, the output of the oscillator 28a during ; line 1 of field 1 of the reference signal, and the output of the oscillator 28b at other times. The CRT 10 is blanked during switches between the oscillators 28a and 28b and the filter 14, and is unblanked for a portlon of the time for which the ,- .

125~196 filter 14 is selected. Accordingly, the CRT dis-plays a sync dot 44a at an angular position repre-senting SC/H phase of the reference signal and a vector 42b and a sync dot 44b whose relative angu-lar positions represent SC/H phase of the selectedvideo signal. The CW output signals provided by sync locked oscillators 28a and 28b are of dif-ferent amplitudes, and therefore the two sync dots can be readily distinguished based on radial dis-tance from the center dot.
The CRT does not display a vector representingphase of the reference color burst. On initial set-up, the reference signal may be connected to both terminals 46 and 48, in which case a vector indicated 42a and representing the phase of reference burst will be displayed, and by adjusting the phase shifter 22 the vector 42a may be aligned with a predetermined radius, e. g., the 180 degree radius, of the polar display. Thereafter, changes in the phase of reference burst will cause the entire display to rotate, whereas changes in the angular position of only the sync dot 44a represent changes in reference SC/H phase.
A vectorscope embodying the invention and adapted for use in the PAL system comprises essen-tially the same functional elements as are shown in FIG. 3 or 6. However, in order to accomodate the 25 Hz offset that exists between burst and sync in the PAL system, the controls performed by the con-trol logic 32 or 32' are somewhat different. Thus,if the control logic 32 of the FIG. 3 vectorscope carried out only the controls indicated by the waveforms shown in FIG. 4, the sync dot would describe a complete circle, because SC/H phase is different for every line of each field. In accor-~256~96 dance with the PAL standard, SC/H phase is definedon line 1 o~ field 1. In the PAL version of the FIG. 3 vectorscope, the control logic 32 is usd to blank the sync dot for a ~ew lines before and after line 1, as indicated in FIG. 8. The resulting display is shown in FIG. 9, and it will be seen that the part circle formed by the unblanked sync dot on either side of the blanked portions aid in locatinq the dot 44' representing the sync locked CW vector for line 1. The resulting gaps in the circle form a coarse display of SC/H phase which is usable from a distance. For reasons that are well understood by persons skilled in the art, two burst vectors 42' are shown in FIG. 9. Similarly, in the case of the PAL version of the FIG. 6 vectorscope, the control logic 32' blanks the sync dot for a few lines before and after line 1 of the reference signal.
It will be appreciated that the invention is not restricted to the particular instruments that have been described with reference to FIGS. 3 and 6, since variations may be made therein without departing from the scope of the invention as defined in the appended claims, and equivalents thereof. For example whereas in the case of FIG. 3 the measure of sync timing relative to burst is obtained by generating the sync locked CW, and this CW signal is used directly as an input to the vectorscope and is processed through the vector-scope's conventional functional elements to providethe desired display, other means of generating a signal representative of the phase angle correspon-ding to the time difference between the sync point and the closest zero crossing of the extended subcarrier wave may be used. For example, as shown ~256196 in FIG. 10 it would be possible to use a sync detector 46 to generate a signal at the sync point and to use this signal to control a sampler 48 for sampling the extended subcarrier wave. The amplitude of the extended subcarrier S wave at the sample point is dependent upon SC/H phase, and may be used to address a look-up device 50 that generates signals for application to the X and Y plates of the CRT.
Alternatively, a burst pulse generator 52 may be used to generate a sampling pulse at the first positive-going zero crossing point of burst, and this pulse may be used to control a sampler 54 for sampling a sync locked continuous wave provided by an oscillator 55 (FIG. 11). Again, the amplitude of the wave at the sample point is representative of the SC/H phase and may be used to address a look-up device 56 that generates X and Y signals for the CRT.
Still further, a sync detector 58 could be used to generate a first pulse and the next positive-going zero crossing point of the burst could be used by a burst pulse generator 60 to generate a second pulse, and a simple time measuring circuit 62 could be used to determined the delay between the pulses (FIG. 12). This time difference could translated through a look-up device 64 into a measure of SC/H phase. In addition, if it were desired to compare two video signals, e.g., an input signal and a reference signal for color framing purposes, the vectorscope could be constructed with two sync locked oscillators fed by the two signals respectively. In this case, the outputs of the two oscillators would be applied to the switch 30 (FIG. 3), which would time multiplex these outputs and the output of the filter into the display to enable comparison of the timing ~'2S6~96 of the sync points of the two video signals to each other and to burst. Moreover, whereas in the case - of FIG. 6 the vectorscope displays the subcarrier frequency components of only the selected video S signal, if the vectorscope were used in a produc-tion facility that had only a small number of signal sources correct color framing of two video signals (the reference signal and the selected signal) may be achieved by comparing the two video signals directly. In this case, a second bandpass filter wo~ld be associated with the input terminal 46 and the switch 30' would select among four possible signals (two bursts and two sync locked CW
signals). It would then be possible to provide a technician with information that would permit the selected video signal to be brought into the correct color frame relationship with the reference signal.

. .

Claims (5)

Claims:

1. An instrument for use in indicating subscarrier to horizontal sync (SC/H) phase of a composite video signal, comprising a display device for providing a polar display, said display device including means for generating from a reference subcarrier burst of the video signal a first input signal for the display device such as to cause the display device to display an indication at a predetermined angular position of the polar display, and said instrument further comprising phase determining and indicating means for determining a time difference between a sync point and that zero crossing of the extrapolated subcarrier wave which is closest to the sync point and for generating from said time difference a second input signal for the display device such as to cause the display device to display an indication at a position of the polar display that is angularly spaced from a predetermined axis of the polar display by an angle given by the fraction having as its denominator the period of the reference subcarrier wave and as its numerator the product of said time difference and 360 degrees.

2. An instrument according to claim 1, wherein said display device comprises a subcarrier regenerator for regenerating from burst a continuous wave signal at subcarrier frequency and phase-locked to burst, and wherein the phase determining and indicating means comprise a sync detector for generating a pulse at the sync point, a sampler for sampling the regenerated sub-carrier wave with the pulse generated by the sync detector and providing an output signal representative of the magnitude of the continuous wave at the sync point, and means for converting said output signal into a signal representative of the angular position, within the reference subcarrier cycle, of the sync point.

3. An instrument according to claim 1, wherein the phase determining and indicating means comprise an oscillator for generating a signal at subcarrier frequency and phase-locked to horizontal sync, and means for determining the phase difference between burst and said signal at subcarrier frequency.

4. An instrument according to claim 1, wherein the phase determining and indicating means comprise an oscillator for generating a signal at subcarrier frequency and phase-locked to horizontal sync, means for generating a pulse at a predetermined zero crossing of burst, a sampler for sampling said signal at subcarrier frequency with said sampling pulse and providing an output signal representative of the magnitude of the sampled signal at the sample point, and means for converting said output signal into a signal representative of the angular position, within the reference subcarrier cycle, of the sync point.

5. An instrument according to claim 1, wherein the phase determining and indicating means comprise a first pulse generator for generating a pulse at a predetermined time relative to the sync point, a second pulse generator for generating a pulse at a predetermined time relative to the first positive-going zero crossing of burst, means for determining the time difference between said pulses, and means for converting said time difference into a signal representative of the angular position, within the reference subcarrier cycle, of the sync point.