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In an circuit, V and I are given by V=15...

In an circuit, V and I are given by `V=150sin(150t) V` and `I =150sin(150t+(pi)/(3))A`. The power dissipated in the circuit is

A

106 W

B

150W

C

5625 W

D

zero

Text Solution

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The correct Answer is:
To find the power dissipated in the circuit given the voltage and current equations, we can follow these steps: ### Step 1: Identify the RMS values of voltage and current The voltage \( V(t) \) is given by: \[ V(t) = 150 \sin(150t) \, V \] The peak voltage \( V_0 \) is 150 V. The RMS (Root Mean Square) value of voltage is calculated as: \[ V_{RMS} = \frac{V_0}{\sqrt{2}} = \frac{150}{\sqrt{2}} = 75\sqrt{2} \, V \] The current \( I(t) \) is given by: \[ I(t) = 150 \sin\left(150t + \frac{\pi}{3}\right) \, A \] The peak current \( I_0 \) is also 150 A. The RMS value of current is: \[ I_{RMS} = \frac{I_0}{\sqrt{2}} = \frac{150}{\sqrt{2}} = 75\sqrt{2} \, A \] ### Step 2: Determine the phase difference From the equations, we can see that the current leads the voltage by an angle of \( \phi = \frac{\pi}{3} \). ### Step 3: Calculate the power dissipated The average power \( P \) dissipated in the circuit can be calculated using the formula: \[ P = V_{RMS} \times I_{RMS} \times \cos(\phi) \] Substituting the values we found: \[ P = (75\sqrt{2}) \times (75\sqrt{2}) \times \cos\left(\frac{\pi}{3}\right) \] We know that \( \cos\left(\frac{\pi}{3}\right) = \frac{1}{2} \): \[ P = (75\sqrt{2}) \times (75\sqrt{2}) \times \frac{1}{2} \] Calculating \( (75\sqrt{2})^2 \): \[ (75\sqrt{2})^2 = 75^2 \times 2 = 5625 \times 2 = 11250 \] Thus, \[ P = \frac{11250}{2} = 5625 \, W \] ### Final Answer: The power dissipated in the circuit is \( 5625 \, W \). ---

To find the power dissipated in the circuit given the voltage and current equations, we can follow these steps: ### Step 1: Identify the RMS values of voltage and current The voltage \( V(t) \) is given by: \[ V(t) = 150 \sin(150t) \, V \] The peak voltage \( V_0 \) is 150 V. The RMS (Root Mean Square) value of voltage is calculated as: ...
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