chapter 14: rlc circuits and resonance
TRANSCRIPT
Learning with PurposeSlide 1
Learning with PurposeSlide 1
Chapter 14: RLC Circuits and Resonance
Instructor: Jean-Franรงois MILLITHALER
http://faculty.uml.edu/JeanFrancois_Millithaler/FunElec/Spring2017
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๐๐ฟ = 2๐๐๐ฟ
๐๐ถ =1
2๐๐๐ถ
IMPEDANCE AND PHASE ANGLE OF SERIES RLC CIRCUITS
๐tot = ๐๐ + ๐๐ฟ + ๐๐ถ
๐tot = ๐ + ๐๐๐ฟ +1
๐๐๐ถ
๐tot = ๐ + ๐ ๐๐ฟ โ1
๐๐ถ
๐tot = ๐ 2 + ๐๐ฟ โ1
๐๐ถ
2
๐ = ๐ก๐๐โ1๐๐ฟ โ
1๐๐ถ
๐
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In a series RLC circuit, the circuit can be capacitive or inductive, depending on the frequency.
At the frequency where ๐ฟ๐ช = ๐ฟ๐ณ, the circuit is at series resonance.
Below the resonant frequency, the circuit is predominantly capacitive.
Above the resonant frequency, the circuit is predominantly inductive.
Variation of ๐ฟ๐ณ and ๐ฟ๐ช with frequency
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Exercice
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Example
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The voltages across the RLC components must add to the source voltage in accordance with KVL. Because of the opposite phase shift due to L and C, VL and VC effectively subtract.
Notice that VC is out of phase with VL. When they are algebraically added, the result isโฆ
Voltages in a series RLC circuits
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Exercice
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At series resonance, XC and XL cancel. VC and VL also cancel because the voltages are equal and opposite. The circuit is purely resistive at resonance.
Series Resonance
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Series Resonance
At the resonant frequency, ๐๐, the voltages across C and L are equal in magnitude.
Since they are 180๐ out of phase with each other, they cancel, leaving 0 V across the CL combination (point A to point B).
The section of the circuit from A to B effectively looks like a short at resonance (neglecting winding resistance).
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For a given series RLC circuit, resonance occurs at only one specific frequency. A formula for this resonant frequency is developed as follows:
Substitute the reactance formulas, and solve for the resonant frequency, ๐๐
Take the square root of both sides. The formula for resonant frequency is
Series Resonance
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Exercice
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Frequency Response
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The general shape of the impedance versus frequency for a series RLC circuit is superimposed on the curves for XL and XC. Notice that at the resonant frequency, the circuit is resistive, and Z = R
Impedance of series RLC circuits
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Summary of important concepts for series resonance:
โข Capacitive and inductive reactances are equal.
โข Total impedance is a minimum and is resistive.
โข The current is maximum.
โข The phase angle between VS and IS is zero.
โข ๐๐ is given by ๐๐ =1
2๐ ๐ฟ๐ถ
Series Resonance
Summary