91Ó°ÊÓ

1. Amplitude of emf, ${\mathrm{Î\mu }}_m=220\text{V}$
2. Driving frequency,$f_d=400\text{Hz}$
3. Resistance,$R=220\text{Ω}$
4. Inductance,$L=150\text{mH}$
5. Capacitance, $C=24.0\text{μ¹ó}$

In the given circuit, the resistor, capacitor, and inductor are in series. To find the impedance in the circuit, we have to find out the capacitive and inductive reactance. Then by using impedance, we can find the amplitude of current and phase angle. Then a second capacitor is connected in series with the other components. We can find the equivalence capacitance for the modified circuit and corresponding capacitive reactance. We can also find the impedance and the current of the modified circuit.

The impedance of theLCRcircuit for the driving frequency$\left({\mathrm{Ó\neg }}_d\right)$,

$\mathbf{Z}\mathbf{=}\sqrt{{\mathbf{R}}^{\mathbf{2}}\mathbf{+}{\left({\mathbf{X}}_{\mathbf{L}}\mathbf{-}{\mathbf{X}}_{\mathbf{c}}\right)}^{\mathbf{2}}}$ ...(1)

The capacitive reactance of the capacitor,

${\mathit{X}}_{\mathit{C}}\mathbf{=}\frac{\mathbf{1}}{{\mathit{Ó\neg }}_{\mathit{d}}\mathit{C}}$ ...(2)

The inductive reactance of the inductor,

${\mathit{X}}_{\mathit{L}}\mathbf{=}{\mathit{Ó\neg }}_{\mathit{d}}\mathit{L}$ …(3)

The angular frequency of the LC oscillation,
${\mathit{Ó\neg }}_{\mathit{d}}\mathbf{=}\mathbf{2}\mathit{Ï€}{\mathit{f}}_{\mathit{d}}$ …(4)

The current equation using Ohm’s law,

$\mathit{I}\mathbf{=}\frac{{\mathit{Î\mu }}_{\mathit{m}}}{\mathit{Z}}$ …(5)

The equivalent capacitance of a series combination,

$\frac{\mathbf{1}}{{\mathbf{C}}_{\mathbf{eq}}}\mathbf{=}\underset{\mathbf{i}}{\overset{\mathbf{n}}{∑}}\frac{\mathbf{1}}{{\mathbf{C}}_{\mathbf{i}}}$ …(6)

Here, R is the resistance of the resistor, Cis the capacitance of the capacitor, L is the inductance of the inductor and${\mathit{f}}_{\mathit{d}}$is the frequency of the LC oscillation.

For the given value of frequency, equation (5) gives-

$$\begin{gathered} {\mathrm{Ó\neg }}_d=2\mathrm{Ï€}×400\text{Hz} \\ =2513.28\text{rad/s} \end{gathered}$$

Capacitive reactance is given using equation (1) as:

$$\begin{gathered} X_c=\frac{1}{2513.28\text{rad/s}×24.0×{10}^{-6}\text{F}} \\ =16.57\text{Ω} \\ ≈16.6\text{Ω} \end{gathered}$$

Hence, the capacitive reactance is role="math" localid="1662813034707" $16.6\text{Ω}$.

Inductive reactance is given using equation (2) as:

$$\begin{gathered} X_L=2513.28\text{rad/s}×150×{10}^{-3}\text{H} \\ =376.99\text{Ω} \\ ≈377\text{Ω} \end{gathered}$$

Now, the impedance of the RLC circuit can be given using equation (3) as:

$$\begin{gathered} Z=\sqrt{{\left(220\text{Ω}\right)}^2+{\left\{377\text{Ω}-16.6\text{Ω}\right\}}^2} \\ =422.24\text{Ω} \\ ≈422\text{Ω} \end{gathered}$$

Hence, the impedance is $422\text{Ω}$.

Amplitude of current is given using the data in equation (4) as follows:

$$\begin{gathered} I=\frac{220V}{422\text{Ω}} \\ =0.521\text{A} \end{gathered}$$

Hence, the current amplitude is $0.521\text{A}$.

Now, the second capacitor ofthesame capacitance is connected in series.

Then, the equivalent capacitance is given using equation (6) as follows:

$$\begin{gathered} \frac{1}{C_{eq}}=\frac{1}{C}+\frac{1}{C} \\ {C}_{eq}=\frac{C}{2} \\ =\frac{24.0×{10}^{-6}\text{F}}{2} \\ =12.0×{10}^{-6}\text{F} \end{gathered}$$

Thus, the modified capacitive reactance is given using equation (1) as follows:

$$\begin{gathered} X_c=\frac{1}{2513.28\text{rad/s}×12.0×{10}^{-6}\text{F}} \\ =33.2\text{Ω} \end{gathered}$$

Thus, the modified capacitive reactance increases

Modified impedance is given using the above values in equation (iii) as follows:

$$\begin{gathered} Z=\sqrt{{\left(220\text{Ω}\right)}^2+{\left\{377\text{Ω}-33.2\text{Ω}\right\}}^2} \\ =408.16\text{Ω} \end{gathered}$$

Thus, the modified impedance decreases.

Modified amplitude of currentis given using the above values in equation (iv) as follows:

$$\begin{gathered} I=\frac{220\text{V}}{408.16\text{Ω}} \\ =0.539\text{A} \end{gathered}$$

Therefore, the modified current increases.