When AC source is connected across series RLC combination maximum power loss will occur provided

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The figure describes an R LC series circuit. It shows a resistor R connected in series with an inductor L, connected to a capacitor C in series to an A C source V. The voltage of the A C source is given by V.When a pure resistance of R ohms, a pure inductance of L Henry and a pure capacitance of C farads are connected together in series combination with each other then RLC Series Circuit is formed. As all the three elements are connected in series, the current flowing through each element of the circuit will be the same as the total current I flowing in the circuit.R is denoted by ${V_r}$, L is denoted by${V_l}$ and C is denoted b${V_c}$ and in the RLC-circuit$\therefore $ ${X_L}$ =2$\pi $ fL and ${X_c}$ =$\dfrac{1}{2}$ $\pi $ fC${V_\pi }$= IR that is the voltage across the resistance R and is in phase with the current I.

${V_i}$ = I${X_L}$ that is the voltage across the inductance L and it leads the current I by an angle of 90 degrees.

${V_c}$ = I${X_c}$ that is the voltage across capacitor C and it lags the current I by an angle of 90 degrees.Step 2:The product of voltage and current is defined as P=VI$\cos \phi $ =I${R^2}$ Where, cos$\phi $ is the power factor of the circuit and expressed as: cos$\phi $=$\dfrac{{{V_r}}}{v}$ =$\dfrac{R}{Z}$ =$\dfrac{R}{{\sqrt {{{\left( {{X_c} - {X_l}} \right)}^2} + {R^2}} }}$ Hence this is the power in series by the RLC circuit in the AC source.

From the above equation option D is correct.

Note:For a series RLC circuit, an impedance triangle can be drawn by dividing each side of the voltage triangle by its current, I. The voltage drop across the resistive element is equal to IR, the voltage across the two reactive elements is IX = I${X_L}$ – I${X_c}$ while the source voltage is equal to IZ.

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