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Question: In LCR circuit at resonance, current in the circuit is \(10\sqrt 2 A\). If now the frequency of the ...

In LCR circuit at resonance, current in the circuit is 102A10\sqrt 2 A. If now the frequency of the source is changed such that current lags by450{45^0} than the applied voltage in the circuit then, which of the following is correct?
(A)\left( {\text{A}} \right) Frequency must be increased and current after the change is 10A{\text{10A}}.
(B)\left( {\text{B}} \right) Frequency must be decreased and current after the change is 10A{\text{10A}}.
(C)\left( {\text{C}} \right) Frequency must be decreased and current is the same as that of initial value.
(D)\left( {\text{D}} \right) The given information is insufficient to conclude anything.

Explanation

Solution

The resonance phenomenon is exhibited by a circuit only if both L{\text{L}} and C{\text{C}} are present in the circuit. Only then, the voltage across L{\text{L}} and C{\text{C}} cancel each other so that the voltage across R{\text{R}} is equal to the source voltage.

Complete step by step answer:
Consider a circuit containing an inductor, capacitor and resistor are connected in series across an alternating source of voltage V{\text{V}} or emf ε\varepsilon .

Let the source supplies a sinusoidal voltage which is given by,
V=V0sinωtV = {V_0}\sin \omega t
Where, V0{V_0} is the peak value of voltage ω\omega is the angular frequency and tt is the time period.
Let qq be the charge on the capacitor and ii be the current in the circuit at any instant of time tt .
Let VR,VL,VC{V_R},{V_L},{V_C} represent the voltage across the resistor, inductor, and capacitor respectively.
Then, the voltage across the resistor, VR=i0R{V_R} = {i_0}R
The voltage across an inductor, VL=i0XL{V_L} = {i_0}{X_L}
The voltage across a capacitor, VC=i0XC{V_C} = {i_0}{X_C}
Where, i0{i_0} is the peak value of current, XC{X_C} is capacitive reactance, XL{X_L} is the inductive reactance, and R{\text{R}} is the resistance of the resistor.
It is stated in the questions that are the current lags by450{45^0} that is,ϕ=450\phi = {45^0}
Then, cosϕ=RZ\cos \phi = \dfrac{R}{Z}
cos450=RZ\cos {45^0} = \dfrac{R}{Z}
Here cos450=12\cos {45^0} = \dfrac{1}{{\sqrt 2 }}
So we can write it as,
12=RZ\dfrac{1}{{\sqrt 2 }} = \dfrac{R}{Z}
Taking cross multiplication we get,
Z=2R\Rightarrow Z = \sqrt 2 R
At resonance condition,XL=XC{X_L} = {X_C}
Then impedance Z=(R2+(XLXC)2)Z = \sqrt {\left( {{R^2} + {{\left( {{X_L} - {X_C}} \right)}^2}} \right)} becomes, Z=RZ = R
There is a maximum value of current is flowing in the circuit Irms=102A{I_{rms}} = 10\sqrt 2 A
That is, Irms=I02{I_{rms}} = \dfrac{{{I_0}}}{{\sqrt 2 }}
102=I0210\sqrt 2 = \dfrac{{{I_0}}}{{\sqrt 2 }}
After simplification we get,
I0=10A{I_0} = 10A
Now we already have an given that, current lags behind the applied voltage by   45\;45 degree, then XL>XC{X_L} > {X_C} for this condition angular frequency ω\omega must be increases, so that XL{X_L} will increase and XC{X_C} will decrease.
Therefore, the frequency must be increased and current after the change is 10A{\text{10A}}.

The correct option is A

Note:
Inductive reactance is the opposition offered by an inductance to the ac through it.
Capacitive reactance is the effective opposition offered by the capacitance to the ac through it.
Impedance of an ace circuit is the effective opposition offered by the circuit to the alternating current through it.