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CIRCUITS and SYSTEMS – part II Prof. dr hab. Stanisław Osowski Electrical Engineering (B.Sc.) Projekt współfinansowany przez Unię Europejską w ramach Europejskiego Funduszu Społecznego. Publikacja dystrybuowana jest bezpłatnie
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Lecture 8 Circuits at nonsinusoidal excitation
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Fourier series -Dirichlet conditions f(t) periodic of period T f(t) absolutely integrable, i.e. finite number of minimum and maximum points At non-continuous points we have
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Trigonometric form of Fourier series General form Sinusoidal form k – multiplicity of harmonic component F k – magnitude of kth harmonic component – phase of kth harmonic component – angular frequency of of kth harmonic component – DC component T – period of nonsinusodal periodic signal
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Fourier coefficients and
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Example Decompose the given f(t) into Fourier series
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Fourier coefficients Trigonometric series coefficients Trigonometric form of the time function
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Simplified series At T 1 =1/4T we have Magnitude characteristicsPhase characteristics
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Fourier approximation of the pulse
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Exponential form of Fourier series Definition of trigonometric functions Exponential form Basic relations
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Final exponential form where
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Example Find the exponential Fourier series of f(t) After applying definition of sinus and cosine functions we get
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Example (cont.) Magnitude spectrum Phase spectrum Frequency spectra of the signal
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Parseval theorem The mean value over the period of the product of two periodic functions can be expressed in the form where f k and g k represent the exponential form coefficients of kth harmonics of f(t) and g(t).
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The rms value of nonsinusoidal signal Given the voltage and current signals Their rms values are expressed in the form Total harmonic distortion (TDH)
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Powers at nonsinuoidal signals The general expressions for real, reactive and apparent power The distortion power D
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Analysis of circuits at nonsinusoidal excitations Voltage excitation
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Analysis of circuits at nonsinusoidal excitations (cont.) Current excitation
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Example Consider the circuit given below. Assume : R1=1Ω, R2=2 Ω, L1=1H, L2=2H, C1=1/4F, C2=1/2F, ω=1. Calculate the rms values of the currents and powers of the source.,,,,
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DC component
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First harmonic component Reactances Currents and power of the source
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Second harmonic component Reactances and equivalent impedance Currents and power of the source
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Total responses rms values of currents Powers calculation
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