Electrical Circuits Dr inż. Agnieszka Wardzińska Room: 105 Polanka

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Presentation transcript:

Electrical Circuits Dr inż. Agnieszka Wardzińska Room: 105 Polanka agnieszka.wardzinska@put.poznan.pl cygnus.et.put.poznan.pl/~award Advisor hours: Monday: 9.30-10.15 Wednesday: 10.15-11.00

Remarks about phasor diagrams

Phasor Relationships for Resistor Time domain Phasor domain Phasor diagram

Phasor Relationships for Inductor Time domain Phasor domain Phasor diagram

Phasor Relationships for Capacitor Time domain Phasor domain Phasor diagram

Examples

Mixed Frequency signals A sinusoidal waveform is one shaped exactly like a sine wave. A non-sinusoidal waveform can be anything from a distorted sine-wave shape to something completely different like a square wave. Mixed-frequency waveforms can be accidently created, purposely created, or simply exist out of necessity. Most musical tones, for instance, are not composed of a single frequency sine-wave, but are rich blends of different frequencies.

Mixed Frequency signals When multiple sine waveforms are mixed together (as is often the case in music), the lowest frequency sine-wave is called the fundamental, and the other sine-waves whose frequencies are whole-number multiples of the fundamental wave are called harmonics. An overtone is a harmonic produced by a particular device. The “first” overtone is the first frequency greater than the fundamental, while the “second” overtone is the next greater frequency produced. Successive overtones may or may not correspond to incremental harmonics, depending on the device producing the mixed frequencies. Some devices and systems do not permit the establishment of certain harmonics, and so their overtones would only include some (not all) harmonic frequencies.

Any regular (repeating), non-sinusoidal waveform is equivalent to a particular series of sine/cosine waves of different frequencies, phases, and amplitudes, plus a DC offset voltage if necessary. The mathematical process for determining the sinusoidal waveform equivalent for any waveform is called Fourier analysis. Multiple-frequency voltage sources can be simulated for analysis by connecting several single-frequency voltage sources in series. Analysis of voltages and currents is accomplished by using the superposition theorem. NOTE: superimposed voltages and currents of different frequencies cannot be added together in complex number form, since complex numbers only account for amplitude and phase shift, not frequency! Harmonics can cause problems by impressing unwanted (“noise”) voltage signals upon nearby circuits. These unwanted signals may come by way of capacitive coupling, inductive coupling, electromagnetic radiation, or a combination thereof.

Any waveform at all, so long as it is repetitive, can be reduced to a series of sinusoidal waveforms added together. Different waveshapes consist of different blends of sine-wave harmonics. Rectification of AC to DC is a very common source of harmonics within industrial power systems.

Square wave signals 1 V (peak) repeating square wave at 50 Hz is equivalent to: (1 V peak sine wave at 50 Hz) + 4 π (1/3 V peak sine wave at 150 Hz) (1/5 V peak sine wave at 250 Hz) (1/7 V peak sine wave at 350 Hz) (1/9 V peak sine wave at 450 Hz) + . . . ad infinitum

Other shapes of nonsinusoidal waveforms

RMS value of mixed signals

Parseval’s Theorem The integral of the square of a function is equal with the integral of the squared components od its spectrum. This means that the total energy of a waveform can be found in total energy of the waveform’s components. As each signal forming the arbitrary signals can be docomposed in iths spectrum componennts, all these components contribute to the total energy of the arbitrary waveform and the RMS value is the square root of the sum of swuares of each spectrum component.

Power in mixed signals Active Power in Watts are equal to sum of active power of all harmonics and power of DC component Reactive power in var are equal to sum of reactive power of all harmonics

Power in mixed signals NOTE The sum of squares of active and reactive power of mixed signal IS NOT equal of the square of apparent power

Examples