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Question: In LC circuit the inductance L=40 mH and capacitance C=100 μF. If a voltage V(t)=10sin(314t) is appl...

In LC circuit the inductance L=40 mH and capacitance C=100 μF. If a voltage V(t)=10sin(314t) is applied to the circuit, the current in the circuit is given as:

Answer

I(t) = 0.5185 cos(314t) A

Explanation

Solution

The problem asks for the current in an ideal LC circuit when an AC voltage source is applied.

  1. Identify Given Parameters:

    • Inductance, L = 40 mH = 40 × 10⁻³ H = 0.04 H
    • Capacitance, C = 100 μF = 100 × 10⁻⁶ F = 10⁻⁴ F
    • Applied Voltage, V(t) = 10sin(314t) V
  2. Extract Voltage Amplitude and Angular Frequency:

    From the given voltage equation V(t) = V₀sin(ωt), we can identify:

    • Peak voltage, V₀ = 10 V
    • Angular frequency, ω = 314 rad/s
  3. Calculate Reactances:

    • Inductive Reactance (X_L): XL=ωLX_L = \omega L XL=314rad/s×0.04HX_L = 314 \, \text{rad/s} \times 0.04 \, \text{H} XL=12.56ΩX_L = 12.56 \, \Omega

    • Capacitive Reactance (X_C): XC=1ωCX_C = \frac{1}{\omega C} XC=1314rad/s×104FX_C = \frac{1}{314 \, \text{rad/s} \times 10^{-4} \, \text{F}} XC=10.0314ΩX_C = \frac{1}{0.0314} \, \Omega XC31.847ΩX_C \approx 31.847 \, \Omega

  4. Determine Total Impedance (Z):

    For a series LC circuit, the impedance is the absolute difference between the inductive and capacitive reactances: Z=XLXCZ = |X_L - X_C| Since XC(31.847Ω)>XL(12.56Ω)X_C (31.847 \, \Omega) > X_L (12.56 \, \Omega), the circuit is capacitive. Z=XCXLZ = X_C - X_L Z=31.847Ω12.56ΩZ = 31.847 \, \Omega - 12.56 \, \Omega Z=19.287ΩZ = 19.287 \, \Omega

  5. Calculate Peak Current (I₀):

    The peak current is given by Ohm's law for AC circuits: I0=V0ZI_0 = \frac{V_0}{Z} I0=10V19.287ΩI_0 = \frac{10 \, \text{V}}{19.287 \, \Omega} I00.5185AI_0 \approx 0.5185 \, \text{A}

  6. Determine the Phase Relationship:

    In a series LC circuit:

    • If XL>XCX_L > X_C, the circuit is inductive, and current lags the voltage by 90° (π/2 radians).
    • If XC>XLX_C > X_L, the circuit is capacitive, and current leads the voltage by 90° (π/2 radians).
    • If XL=XCX_L = X_C, the circuit is at resonance, and current is in phase with voltage (ideally infinite current in an ideal LC circuit).

    In this case, XC>XLX_C > X_L, so the circuit is capacitive, and the current leads the voltage by π/2 radians. Since the applied voltage is V(t)=V0sin(ωt)V(t) = V_0\sin(\omega t), the current will be I(t)=I0sin(ωt+π2)I(t) = I_0\sin(\omega t + \frac{\pi}{2}). Using the trigonometric identity sin(x+π2)=cos(x)\sin(x + \frac{\pi}{2}) = \cos(x), we get: I(t)=I0cos(ωt)I(t) = I_0\cos(\omega t)

  7. Write the Current Equation:

    Substitute the calculated values of I0I_0 and ω\omega: I(t)=0.5185cos(314t)AI(t) = 0.5185 \cos(314t) \, \text{A}

The final answer is I(t)=0.5185cos(314t)A\boxed{I(t) = 0.5185 \cos(314t) \, \text{A}}.

Explanation of the solution:

  1. Calculate inductive reactance (XL=ωLX_L = \omega L) and capacitive reactance (XC=1/(ωC)X_C = 1/(\omega C)) using the given L, C, and ω from the voltage equation.
  2. Determine the total impedance (Z=XLXCZ = |X_L - X_C|). Since XC>XLX_C > X_L, the circuit is capacitive.
  3. Calculate the peak current (I0=V0/ZI_0 = V_0/Z).
  4. Since the circuit is capacitive, the current leads the voltage by π/2\pi/2. Given V(t)=V0sin(ωt)V(t) = V_0\sin(\omega t), the current will be I(t)=I0sin(ωt+π/2)=I0cos(ωt)I(t) = I_0\sin(\omega t + \pi/2) = I_0\cos(\omega t).

Answer: The current in the circuit is given as: I(t)=0.5185cos(314t)AI(t) = 0.5185 \cos(314t) \, \text{A}