An inductor of inductance l and resistor of resistance r are joined in series and connected by source of frequency power dissipated in the circuit is
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Answer:
Given is series R – L circuit
Hence impedance = Z = √[R^2 + XL^2]
current I = [V / {|Z|}] = [V / √{R^2 + XL^2}]
power dissipated in the circuit is P = I2^R = [{V}/√{R^2 + XL^2}]^2 ∙ R
∴ P = [{V^2R}/{R^2 + XL^2}] = [{V^2R}/{R^2 + ω^2L^2}].
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An inductor of inductance l and resistor of resistance r are joined in series and connected by source of frequency power dissipated in the circuit is
P = V^2R / (R^2 + w^2L^2)
- Given:
- Inductor and Resistor are in series
- Implies, the impedance
- Z = √(R^2 + XL^2)
- Current, I
- I = V / |Z|
- ⇒ I = V / √(R^2 + XL^2)
- Now, the power dissipated in the circuit, is given by,
- P = I^2R
- = [V / √(R^2 + XL^2)]^2 * R
- ⇒ P = V^2R / (R^2 + XL^2)
- ∴ P = V^2R / (R^2 + w^2L^2)
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