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The voltage E and the current I in an in...

The voltage E and the current I in an instrument are represented by the equations:
`E=2cos omegatV`
`I=2sin omegat A`
The average power dissipated in the instrument will be

A

zero

B

1.0 W

C

4 W

D

2.0 W

Text Solution

AI Generated Solution

The correct Answer is:
To solve the problem, we need to find the average power dissipated in the instrument given the voltage and current equations. Let's go through the solution step by step. ### Step 1: Identify the given equations The voltage \( E \) and current \( I \) are given by: \[ E = 2 \cos(\omega t) \quad \text{(in volts)} \] \[ I = 2 \sin(\omega t) \quad \text{(in amperes)} \] ### Step 2: Find the phase difference The voltage is expressed as a cosine function, while the current is expressed as a sine function. We can express the sine function in terms of cosine to find the phase difference. Recall that: \[ \sin(\theta) = \cos\left(\theta - \frac{\pi}{2}\right) \] Thus, we can rewrite the current as: \[ I = 2 \sin(\omega t) = 2 \cos\left(\omega t - \frac{\pi}{2}\right) \] This indicates that the current lags behind the voltage by \( \frac{\pi}{2} \) radians. ### Step 3: Determine the phase difference \( \phi \) From the equations, we see that the phase difference \( \phi \) between voltage and current is: \[ \phi = \frac{\pi}{2} \] ### Step 4: Calculate RMS values The RMS (Root Mean Square) values for voltage and current can be calculated as follows: \[ V_{\text{rms}} = \frac{E_{\text{max}}}{\sqrt{2}} = \frac{2}{\sqrt{2}} = \sqrt{2} \, \text{V} \] \[ I_{\text{rms}} = \frac{I_{\text{max}}}{\sqrt{2}} = \frac{2}{\sqrt{2}} = \sqrt{2} \, \text{A} \] ### Step 5: Use the average power formula The average power \( P \) dissipated in an AC circuit is given by: \[ P = V_{\text{rms}} \cdot I_{\text{rms}} \cdot \cos(\phi) \] Substituting the values we have: \[ P = \sqrt{2} \cdot \sqrt{2} \cdot \cos\left(\frac{\pi}{2}\right) \] Since \( \cos\left(\frac{\pi}{2}\right) = 0 \): \[ P = \sqrt{2} \cdot \sqrt{2} \cdot 0 = 0 \] ### Conclusion The average power dissipated in the instrument is: \[ \boxed{0} \]
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