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Short Time Distortion<br />

• DEFINITION<br />

Short time distortions cause amplitude changes, ringing, overshoot<br />

and undershoot in fast rise times and 21 pulses. The affected<br />

signal components range in duration from 0.100 microsecond<br />

to 1.0 microsecond.<br />

For PAL systems, distortions in the short time domain are most often<br />

characterised by measuring K2T or K pu | se /b ar . These measurements<br />

are described in the K Factor section of this booklet (page 44).<br />

Alternatively, the aberrations in a T rise time bar can be described<br />

in terms of the "percent SD" method described in this section.<br />

• PICTURE EFFECTS<br />

Short time distortions produce fuzzy vertical edges. Ringing<br />

can sometimes be interpreted as chrominance information<br />

(cross colour), causing colour artifacts near vertical edges.<br />

Figure 28. A J rise time bar has a 10% to 90% rise<br />

time of nominally 100 nanoseconds.<br />

• TEST SIGNALS<br />

2T pulses are generally specified when K Factor and pulse-to-bar<br />

methods are used to characterise short time distortion. In order<br />

to use the "percent SD" method, however, a signal with a T rise<br />

time white bar is required. As shown in Figure 28, a T rise time<br />

bar has a 10%-to-90% rise time of nominally 100 nanoseconds.<br />

(See Appendix B for a discussion of the time interval T.)<br />

It is very important to make sure you are using a T rise time bar<br />

with the short time distortion graticule. Many common test<br />

signals have 2T rather that T rise times, and 2T bars are not<br />

suitable for this measurement. It should also be noted that T<br />

rise times cannot survive transmission, because they contain<br />

fast components which do not pass through the 5 or 6 MHz<br />

lowpass filter. Short time distortion measurements made on<br />

transmitted signals will therefore evaluate only those components<br />

in approximately the 200 nanosecond to 1 microsecond range.<br />

• MEASUREMENT METHODS<br />

Measurements of the undershoot, overshoot and ringing at the<br />

edge of a T rise bar are not generally quoted directly as a<br />

percent of the transition amplitude, but rather are expressed in<br />

terms of an amplitude-weighting system that yields results in<br />

"percent SD". This weighting is necessary because the amount<br />

of distortion depends not only on the distortion amplitude, but<br />

also on the time the distortion occurs with respect to the transition.<br />

Although results can be calculated from the time and<br />

amplitude of the measured ringing lobes, special graticules,<br />

conversion tables or nomographs are used in practice.<br />

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