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A vector of magnitude a is turned throug...

A vector of magnitude a is turned through angle `theta` . The magnitude of change in the vector is given by:

A

`|2a sin theta|`

B

`|2a sin theta //2|`

C

`|(a)/(2) sin theta|`

D

`|(a)/(2) sin theta //2|`

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The correct Answer is:
To find the magnitude of change in a vector of magnitude \( A \) when it is turned through an angle \( \theta \), we can follow these steps: ### Step 1: Define the initial vector Let the initial vector \( \mathbf{A} \) be represented as: \[ \mathbf{A} = A \hat{i} \] This means it is directed along the x-axis with magnitude \( A \). ### Step 2: Define the new vector after rotation When the vector is turned through an angle \( \theta \), the new vector \( \mathbf{A'} \) can be expressed in terms of its components: \[ \mathbf{A'} = A \cos(\theta) \hat{i} + A \sin(\theta) \hat{j} \] Here, \( A \cos(\theta) \) is the x-component and \( A \sin(\theta) \) is the y-component of the new vector. ### Step 3: Calculate the change in the vector The change in the vector \( \Delta \mathbf{A} \) is given by: \[ \Delta \mathbf{A} = \mathbf{A'} - \mathbf{A} \] Substituting the expressions for \( \mathbf{A'} \) and \( \mathbf{A} \): \[ \Delta \mathbf{A} = (A \cos(\theta) \hat{i} + A \sin(\theta) \hat{j}) - (A \hat{i}) \] This simplifies to: \[ \Delta \mathbf{A} = (A \cos(\theta) - A) \hat{i} + A \sin(\theta) \hat{j} \] \[ \Delta \mathbf{A} = A (\cos(\theta) - 1) \hat{i} + A \sin(\theta) \hat{j} \] ### Step 4: Find the magnitude of the change in the vector To find the magnitude of \( \Delta \mathbf{A} \), we use the formula for the magnitude of a vector: \[ |\Delta \mathbf{A}| = \sqrt{(A (\cos(\theta) - 1))^2 + (A \sin(\theta))^2} \] Expanding this: \[ |\Delta \mathbf{A}| = \sqrt{A^2 (\cos(\theta) - 1)^2 + A^2 \sin^2(\theta)} \] Factoring out \( A^2 \): \[ |\Delta \mathbf{A}| = A \sqrt{(\cos(\theta) - 1)^2 + \sin^2(\theta)} \] ### Step 5: Simplify the expression Now we simplify the expression inside the square root: \[ |\Delta \mathbf{A}| = A \sqrt{\cos^2(\theta) - 2\cos(\theta) + 1 + \sin^2(\theta)} \] Using the Pythagorean identity \( \cos^2(\theta) + \sin^2(\theta) = 1 \): \[ |\Delta \mathbf{A}| = A \sqrt{1 - 2\cos(\theta) + 1} = A \sqrt{2 - 2\cos(\theta)} \] Factoring out the 2: \[ |\Delta \mathbf{A}| = A \sqrt{2(1 - \cos(\theta))} \] Using the trigonometric identity \( 1 - \cos(\theta) = 2 \sin^2(\frac{\theta}{2}) \): \[ |\Delta \mathbf{A}| = A \sqrt{2 \cdot 2 \sin^2\left(\frac{\theta}{2}\right)} = 2A \sin\left(\frac{\theta}{2}\right) \] ### Final Result Thus, the magnitude of the change in the vector is: \[ |\Delta \mathbf{A}| = 2A \sin\left(\frac{\theta}{2}\right) \]
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