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The rms value of the emf given by E = 8...

The rms value of the emf given by ` E = 8 sin omegat + 6 sin 2omegat` .

A

`5sqrt2 V`

B

`7sqrt2 V`

C

`10V`

D

`10sqrt2V`

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The correct Answer is:
To find the RMS (Root Mean Square) value of the given EMF \( E = 8 \sin(\omega t) + 6 \sin(2\omega t) \), we will follow these steps: ### Step 1: Understanding the RMS Value The RMS value of a function over one complete cycle is given by the formula: \[ E_{\text{rms}} = \sqrt{\frac{1}{T} \int_0^T E^2 \, dt} \] where \( T \) is the period of the function. ### Step 2: Calculate \( E^2 \) First, we need to square the expression for \( E \): \[ E^2 = (8 \sin(\omega t) + 6 \sin(2\omega t))^2 \] Expanding this: \[ E^2 = 64 \sin^2(\omega t) + 36 \sin^2(2\omega t) + 96 \sin(\omega t) \sin(2\omega t) \] ### Step 3: Simplifying the Terms Now, we will evaluate the average of each term over one complete cycle: 1. The average of \( \sin^2(\omega t) \) over one complete cycle is \( \frac{1}{2} \). 2. The average of \( \sin^2(2\omega t) \) over one complete cycle is also \( \frac{1}{2} \). 3. The average of \( \sin(\omega t) \sin(2\omega t) \) over one complete cycle is \( 0 \) (since it is a product of sine functions with different frequencies). ### Step 4: Calculate the Mean Square Value Using the averages calculated: \[ \langle E^2 \rangle = 64 \cdot \frac{1}{2} + 36 \cdot \frac{1}{2} + 96 \cdot 0 \] \[ \langle E^2 \rangle = 32 + 18 + 0 = 50 \] ### Step 5: Calculate the RMS Value Now, we can find the RMS value: \[ E_{\text{rms}} = \sqrt{\langle E^2 \rangle} = \sqrt{50} = 5\sqrt{2} \] ### Final Answer Thus, the RMS value of the EMF is: \[ E_{\text{rms}} = 5\sqrt{2} \text{ volts} \] ---

To find the RMS (Root Mean Square) value of the given EMF \( E = 8 \sin(\omega t) + 6 \sin(2\omega t) \), we will follow these steps: ### Step 1: Understanding the RMS Value The RMS value of a function over one complete cycle is given by the formula: \[ E_{\text{rms}} = \sqrt{\frac{1}{T} \int_0^T E^2 \, dt} \] where \( T \) is the period of the function. ...
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