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Which is true for series resonance?
Z=R
XL=XC
I=RV
All of above
All of above
Quick Summary: In an RLC series circuit, resonance occurs when the inductive reactance equals the capacitive reactance, causing them to cancel each other out. This results in the circuit behaving as a purely resistive load, where impedance is minimum and current is maximum.
In an RLC series circuit, resonance occurs when the inductive reactance equals the capacitive reactance, causing them to cancel each other out. This results in the circuit behaving as a purely resistive load, where impedance is minimum and current is maximum.
XL=2πfrL — Inductive Reactance
XC=2πfrC1 — Capacitive Reactance
Z=R2+(XL−XC)2 — Total Impedance
fr=2πLC1 — Resonant Frequency
The inductive reactance XL=2πfL increases with frequency, while capacitive reactance XC=2πfC1 decreases. At the resonant frequency fr, these magnitudes equalize (XL=XC), nullifying the imaginary part of the impedance Z=R+j(XL−XC). Consequently, the total impedance Z simplifies to the resistance R, and the circuit power factor becomes unity.
At resonance, the phase angle between voltage and current is zero.
The circuit provides minimum impedance to the source at the resonant frequency.
Voltage magnification occurs across the inductor and capacitor.
The circuit acts as a band-pass filter configuration.
Maximum current flow for a given voltage source
Selectivity in radio tuning circuits
Risk of voltage breakdown due to high Q-factor
Sensitive to frequency variations
Radio frequency tuning circuits
Band-pass filter designs
Induction heating systems
The Q-factor (Quality Factor) determines the sharpness of the resonance curve: Q=R1CL.
If XL>XC, the circuit is inductive (lagging pf); if XC>XL, it is capacitive (leading pf).
D is correct — All listed conditions (Z=R, XL=XC, I=V/R) define the state of resonance in an RLC series circuit.
Always remember that resonance in series circuits leads to minimum impedance, while in parallel circuits, it leads to maximum impedance.