Abstract
The most comprehensive information on alternating signals is obtained by observing their temporal evolution, i.e., by measuring continuously in time the value of the signal (current or voltage as required by the problem under consideration). This kind of measurement is generally carried out with devices capable of displaying the time development of the waveform as the oscilloscopes, instruments that we will deal with extensively in the following chapter.
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Notes
- 1.
In our context the term stationary does not refer to quantities that do not depend on time, we would use the term static instead. The alternating signals are time dependent but periodic and the infinitely repeated waveform justifies the term stationary to qualify them.
- 2.
To have an example of transient waveform, consider a capacitor being connected to a battery through a resistance. The current flowing to charge the capacitor has a transient waveform.
- 3.
A similar analysis can be carried out for the case of a block capacitor used to separate the continuous voltage component of different sections in the same circuit.
- 4.
Usually the moving coil motion is critically damped, as described in Sect. 4.3.2, and its characteristic frequency is \(\omega _M\simeq \sqrt{C/\mathscr {I}}\).
- 5.
The feedback is a feature of operational amplifiers whereby the circuit output is fed back to one of the inputs of the device. A detailed description of the design of an operational amplifier requires notions that are usually learned at a successive stage of the course of studies.
References
D.H. Sheinglod, Non Linear Circuits Handbook (Analog Devices Inc., Norwood, 1976)
R. Bartiromo, M. De Vincenzi, AJP 82, 1067–1076 (2014)
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Problems
Problems
Problem 1
An ADC digitizes a sinusoidal voltage signal taking N samples at constant time intervals covering a span equal to the signal period. Sampled values are affected by quantization errors, uncorrelated and identically distributed with variance equal to \(\sigma ^2\). Data are used to identify their maximum and minimum from which the peak-to-peak Xpp is computed. Evaluate the standard uncertainty on this last quantity. [A. \(u_{pp}=\sqrt{2}\sigma \).]
Problem 2
An ADC digitizes a sinusoidal voltage signal taking N samples at constant time intervals covering a span equal to the signal period. Sampled values are affected by quantization errors, uncorrelated and identically distributed with variance equal to \(\sigma ^2\). Show that the estimate of the effective value, obtained as the root mean square of the sampled values, is affected by a bias related to the variance of quantization errors. [A. \(\hat{V}_{rms}=\sqrt{V^2_{rms}+\sigma ^2}\).]
Problem 3
An ADC digitizes a sinusoidal voltage signal taking N samples at constant time intervals covering a span equal to the signal period. Sampled values are affected by quantization errors, uncorrelated and identically distributed with variance equal to \(\sigma ^2\). Show that the estimate of the effective value, obtained as the root mean square of the sampled values, besides being biased (see previous problem) is affected by a statistical uncertainty related to the variance of quantization errors. [A. \(u_V=\sigma /\sqrt{N}\).]
Problem 4
An ADC, with negligible quantization error, digitizes a sinusoidal voltage signal taking N samples at constant time intervals covering a span equal to the signal period. Sampled values are affected by an ambient noise, uncorrelated and identically distributed with variance equal to \(\sigma ^2_n\). Show that the estimate of the effective value, obtained as the root mean square of the sampled values, is affected by a bias related to the variance of ambient noise. [A. \(\hat{V}_{rms}=\sqrt{V^2_{rms}+\sigma ^2_n}\).]
Problem 5
An ADC, with negligible quantization error, digitizes a sinusoidal voltage signal taking N samples at constant time intervals covering a span equal to the signal period. Sampled values are affected by an ambient noise, uncorrelated and identically distributed with variance equal to \(\sigma ^2_n\). Show that the estimate of the effective value, obtained as the root mean square of the sampled values, besides being biased (see previous problem) is affected by a statistical uncertainty related to the noise variance. [A. \(u_V=\sigma _n/\sqrt{N}\).]
Problem 6
A resistor R is heated by Joule dissipation. To compute its temperature, assume that the resistor is cooled by thermal conduction and that the power lost to the environment is given by \(Q=-k(T-T_0)\). The resistor is in equilibrium with the environment at temperature \(T_0\) before being connected to an ideal voltage generator with output equal to \(V_0\). Denoting with C its thermal capacity, calculate the time evolution of the resistor temperature after the connection to the generator. [A. \(T=T_0+(P\tau /C)(1-\text{ e }^{-t/\tau }\) where \(P=V_0^2/R\) and \(\tau =C/k\).]
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Bartiromo, R., De Vincenzi, M. (2016). Measurement of Alternating Electrical Signals. In: Electrical Measurements in the Laboratory Practice. Undergraduate Lecture Notes in Physics. Springer, Cham. https://doi.org/10.1007/978-3-319-31102-9_7
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DOI: https://doi.org/10.1007/978-3-319-31102-9_7
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