T 7.2.1.3 Amplitude Modulation
T 7.2.1.3 Amplitude Modulation
T 7.2.1.3 Amplitude Modulation
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TPS <strong>7.2.1.3</strong><br />
Solutions<br />
Solutions<br />
2.3 A measurement example<br />
1. Manual operation with analog voltmeter<br />
The amplitude S R (1) of the fundamental harmonic<br />
is greater than the square-wave amplitude A R by a<br />
factor 4/π = 1.27. The formation law for the spectrum<br />
of a symmetrical square-wave signal is:<br />
S<br />
R<br />
4 AR<br />
( n)<br />
=<br />
π ( 2n<br />
−1)<br />
n: 1, 2, 3...<br />
Diagram 2.3-1:<br />
Spectrum of the square-wave signal A R<br />
= 5 V, τ/T P<br />
= 0.5<br />
Table 2.3-1: Spectrum square wave signal<br />
Signal parameter<br />
A R : 5 V<br />
τ/T P : 5/10<br />
f R : 2.00 kHz<br />
n<br />
f<br />
kHz<br />
Analyzer settings<br />
V 1 : 1<br />
b : 500 Hz<br />
f r : 20 kHz<br />
T : 20 s<br />
Measurement<br />
S(n) S R (n)<br />
V 2<br />
V<br />
V<br />
Theory<br />
S (n)<br />
R<br />
V<br />
1 2.0 6.6 1 6.6 6.37<br />
2 4.0 ---- - ---- ----<br />
3 6.0 2.1 1 2.1 2.12<br />
4 8.0 ---- - ---- ----<br />
5 10.0 6.6 5 1.32 1.27<br />
6 12.0 ---- - ---- ----<br />
7 14.0 4.7 5 0.94 0.91<br />
8 16.0 ---- - ---- ----<br />
9 18.0 3.6 5 0.72 0.71<br />
10 20.0 ---- - ---- ----<br />
2. Automatic operation with the XY recorder<br />
or the storage oscilloscope<br />
The reduction in the bandwidth b narrows the<br />
spectral window. The manual frequency setting<br />
thus becomes increasingly difficult, while at the<br />
same time the spectral lines become clearer.<br />
Even when using an oscilloscope as a display unit<br />
which operates (almost) without any inertia, the<br />
spectrum is no longer reproduced with full amplitude.<br />
The reason for this lies in the time law of<br />
electrical communications engineering. The filters<br />
of the analyzer no longer reach the transient<br />
recovery state. If mechanical measuring instruments<br />
subject to inertia are used as display units,<br />
e.g. a multimeter instrument or an XY recorder,<br />
then the lowpass response of the entire system is<br />
further improved. There is practically no pointer<br />
deflection. The following general statements can<br />
be made about the spectrum of the symmetrical<br />
square-wave signal:<br />
– The spectrum has a line structure.<br />
– The spectral lines occur at odd numbered multiples<br />
of the fundamental frequency f R . (3 f R ,<br />
5 f R , 7 f R , ...)<br />
– The amplitudes S R (n) respond inversely proportional<br />
to the odd numbered multiples of the<br />
fundamental frequency.(1/3, 1/5, 1/7, ...). The<br />
envelope curve has the characteristic 1/f.<br />
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