{"id":2662,"date":"2018-10-10T11:09:53","date_gmt":"2018-10-10T11:09:53","guid":{"rendered":"https:\/\/35.94.173.37\/blog\/?p=2662"},"modified":"2024-11-05T11:12:15","modified_gmt":"2024-11-05T11:12:15","slug":"bandwidth-vs-rise-time","status":"publish","type":"post","link":"https:\/\/www.apexwaves.com\/blog\/bandwidth-vs-rise-time\/","title":{"rendered":"Bandwidth vs. Rise Time"},"content":{"rendered":"

PULSE DEFINITIONS<\/p>\n

In digital techniques, it can happen that two pulses appear in a time\u00adrelated sequence, but that the second pulse appears a little later, with a delay, with respect to the first one.<\/p>\n

If in one signal the successive pulses do not have the same repetition time, it is said that the signal has jitter.<\/p>\n

\"Screen<\/figure>\n

BANDWIDTH VERSUS RISE TIME (BTr = 0.35)<\/strong><\/p>\n

The bandwidth denotes one of the characteristics of an amplifier and the phase another characteristic. The effect of both can be studied by applying an \u201cideal\u201d square-wave pulse to the input of the amplifier and studying the output voltage. This can be understood if one considers the square wave as being composed of a series (infinite) of sine waves. For example, imagine a pulse is approximated by 5 harmonics, each with its own amplitude and mutual phase. For an exact replica of the waveform, infinite harmonics are needed. The formula for the waveform is given by the Fourier analysis<\/p>\n

V(t) = v4<\/p>\n

1T<\/p>\n

(sin wt + \u00bd sin 3wt + !- sin 5wt\u00a0 + \u00b7 \u00b7 \u00b7)<\/p>\n

After amplification with a factor A, the output voltage V0(t) will be<\/p>\n

V (t) = A \u00b7 4<\/p>\n

(sin wt + \u00bd sin 3wt +! sin 5wt + \u00b7 \u00b7 \u00b7)<\/p>\n

0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0 V<\/p>\n

1T<\/p>\n

It will be clear that due to this behavior of the amplifier the \u201cideal\u201d input square wave appears distorted at the output. For example, the rise time Tr is not 0 but has a certain value. The more harmonics are amplified \u201clinearly\u201d (in the right way: same amplification factor and phase shift), the better the result and the shorter the rise time Tr at the output. The value of Tr depends on the frequency of the harmonics, which are of course determined by the frequency of the square wave.<\/p>\n

It can thus be stated that the shorter the rise time Tr of the output pulse as a response to an ideal input pulse, the more harmonics are amplified linearly and the higher the bandwidth B of the amplifier. It can be shown that for an amplifier with a bandwidth B, the rise time Tr is related to it according to<\/p>\n

BTr\u00a0\u00a0 = 0.35<\/p>\n

where B = bandwidth, Hz<\/p>\n

Tr = rise time, S<\/p>\n

Example: For the Philips 50-MHz oscilloscope PM 3240, the rise time is<\/p>\n

0.35<\/p>\n

Tr=\u00a0\u00a0\u00a0\u00a0\u00a0 50 X 106 S<\/p>\n

= 7 ns<\/p>\n

This oscilloscope thus shows a 7-ns rise time as a response to an \u201cideal\u201d input square wave. As a matter of fact, this is the way the oscilloscope is tested. A pulse for which Tr <<7ns[for example, Tr\u00a0 =\u00a0 l00ps(=\u00a0 10-10\u00a0 s)], is applied to the input, and the rise time is measured from the screen.<\/p>\n

References<\/strong><\/p>\n

https:\/\/www.eetimes.com\/document.asp?doc_id=1276244<\/a><\/p>\n

https:\/\/www.edn.com\/design\/test-and-measurement\/4442988\/Oscilloscope-rise-time-and-noise-explained<\/a><\/p>\n

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