Modelica.Electrical.QuasiStationary.UsersGuide.Overview Modelica.Electrical.QuasiStationary.UsersGuide.Overview


The Modelica.Electrical.QuasiStationary library addresses the analysis of electrical circuits with purely sinusoidal voltages and currents. The main characteristics of the library are:

The main intention of this library is the modeling of quasi stationary behavior of single and multi phase AC circuits with fixed and variable frequency. Quasi stationary theory and applications can be found in [Dorf1993], [Burton1994], [Landolt1936], [Philippow1967], [Weyh1967], [Vaske1973].

Note

A general electrical circuit can be a DC circuit, an AC circuit with periodic sinusoidal or non-sinusodial voltages and currents or a transient circuit without particular waveform of voltages and currents. Therefore a coupling model between a quasi stationary circuit and a general (transient) electrical circuit has to be designed carefully taking the specific application into account. As an exmaple, you may look at the ideal AC DC converter, which is used in the rectifier example.

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Package Content

NameDescription
Modelica.Electrical.QuasiStationary.UsersGuide.Overview.Introduction Introduction Introduction to phasors
Modelica.Electrical.QuasiStationary.UsersGuide.Overview.ACCircuit ACCircuit AC circuit
Modelica.Electrical.QuasiStationary.UsersGuide.Overview.Power Power Real and reactive power
Modelica.Electrical.QuasiStationary.UsersGuide.Overview.ReferenceSystem ReferenceSystem Reference system


Modelica.Electrical.QuasiStationary.UsersGuide.Overview.Introduction Modelica.Electrical.QuasiStationary.UsersGuide.Overview.Introduction



The purely sinusoidal voltage


v=\sqrt{2}V_{\mathrm{RMS}}\cos(\omega t+\varphi_{v})

in the time domain can be represented by a complex rms phasor


\underline{v}=V_{\mathrm{RMS}}e^{j\varphi_{v}}.

For these quasi stationary phasor the following relationship applies:

\begin{displaymath}
v=\mathrm{Re}(\sqrt{2}\underline{v}e^{j\omega t})\end{displaymath}

This equation is also illustrated in Fig. 1.

Fig. 1: Relationship between voltage phasor and time domain voltage

From the above equation it is obvious that for t = 0 the time domain voltage is v = cos(φv). The complex representation of the phasor corresponds with this instance, too, since the phasor is leading the real axis by the angle φv.

The explanation given for sinusoidal voltages can certainly also be applied to sinusoidal currents.

See also

AC circuit, Power, Reference system

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Modelica.Electrical.QuasiStationary.UsersGuide.Overview.ACCircuit Modelica.Electrical.QuasiStationary.UsersGuide.Overview.ACCircuit


A simple example of a series connection of a resistor, an inductor and a capacitor as depicted in Fig. 1 should be explained in the following. For various frequencies, the voltage drops across the resistor, the inductor and the capacitor should be determined.

Fig. 1: Series AC circuit of a resistor and an inductor at variable frequency

The voltage drop across the resistor


\underline{v}_{r}=R\underline{i}

and the inductor


\underline{v}_{l}=j\omega L\underline{i}

and the capacitor


\underline{v}_{l}=j\omega L\underline{i}

add up to the total voltage


\underline{v}=\underline{v}_{r}+\underline{v}_{l}

as illustrated in the phasor diagram of Fig. 2.

Fig. 2: Phasor diagram of a resistor and inductance series connection

Due to the series connection of the resistor, inductor and capacitor, the three currents are all equal:

See also

Introduction, Power, Reference system

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Modelica.Electrical.QuasiStationary.UsersGuide.Overview.Power Modelica.Electrical.QuasiStationary.UsersGuide.Overview.Power



For periodic waveforms, the average value of the instantaneous power is real power P. Reactive power Q is a term associated with inductors and capacitors. For pure inductors and capacitors, real power is equal to zero. Yet, there is instantaneous power exchanged with connecting network.

The series resonance circuit which was also adressed in the AC circuit will be investigated.
Power of a resistor

The instantaneous voltage and current are in phase:


Therefore, the instantaneous power is

A graphical representation of these equations is depicted in Fig. 1

Fig. 1: Instantaneous voltage, current of power of a resistor

Real power of the resistor is the average of instantaneous power:

Power of an inductor

The instantaneous voltage leads the current by a quarter of the period:


Therefore, the instantaneous power is

A graphical representation of these equations is depicted in Fig. 2

Fig. 2: Instantaneous voltage, current of power of an inductor

Reqactive power of the inductor is:

Power of a capacitor

The instantaneous voltage lags the current by a quarter of the period:


Therefore, the instantaneous power is

A graphical representation of these equations is depicted in Fig. 3

Fig. 3: Instantaneous voltage, current of power of a capacitor

Reqactive power of the capacitor is:

Complex apparent power

For an arbitrary component with two pins, real and reactive power can be determined by the complex phasors:

In this equation * represents the conjugate complex operator

See also

Introduction, AC circuit, Reference system

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Modelica.Electrical.QuasiStationary.UsersGuide.Overview.ReferenceSystem Modelica.Electrical.QuasiStationary.UsersGuide.Overview.ReferenceSystem


The reference angle gamma:

Designing new components, the guidelines of the Modelica Specification dealing with Overconstrained Equation Operators for Connection Graphs have to be taken into account.

See also

Introduction, AC circuit, Power

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