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A string of length L is stretched along ...

A string of length L is stretched along the x-axis and is rigidly clamped at its two ends. It undergoes transverse vibration. If n an integer, which of the following relations may represent the shape of the string at any time :-

A

`y=A sin ((n pi x)/(L)) cos omega t`

B

`y=A sin((n pi x)/(L))sin omega t`

C

`y=A cos ((n pi x)/(L)) cos omega t`

D

`y=A cos ((n pi x)/(L))sin omega t`

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The correct Answer is:
To solve the problem, we need to determine which of the given equations can represent the shape of a string undergoing transverse vibrations while being clamped at both ends. The boundary conditions are that the displacement \( y \) of the string must be zero at both ends, \( x = 0 \) and \( x = L \). ### Step-by-Step Solution: 1. **Understanding the Boundary Conditions**: - The string is clamped at both ends, which means that at \( x = 0 \) and \( x = L \), the displacement \( y \) must be zero: \[ y(0, t) = 0 \quad \text{and} \quad y(L, t) = 0 \] 2. **Analyzing the First Equation**: - Let's consider the first equation: \[ y = A \sin\left(\frac{n \pi x}{L}\right) \cos(\omega t) \] - Check the boundary conditions: - At \( x = 0 \): \[ y(0, t) = A \sin(0) \cos(\omega t) = 0 \] - At \( x = L \): \[ y(L, t) = A \sin(n \pi) \cos(\omega t) = 0 \] - Both conditions are satisfied, so this equation is valid. 3. **Analyzing the Second Equation**: - Now consider the second equation: \[ y = A \sin\left(\frac{n \pi x}{L}\right) \sin(\omega t) \] - Check the boundary conditions: - At \( x = 0 \): \[ y(0, t) = A \sin(0) \sin(\omega t) = 0 \] - At \( x = L \): \[ y(L, t) = A \sin(n \pi) \sin(\omega t) = 0 \] - Both conditions are satisfied, so this equation is also valid. 4. **Analyzing the Third Equation**: - Now consider the third equation: \[ y = A \cos\left(\frac{n \pi x}{L}\right) \cos(\omega t) \] - Check the boundary conditions: - At \( x = 0 \): \[ y(0, t) = A \cos(0) \cos(\omega t) = A \cos(\omega t) \quad (\text{not } 0) \] - This does not satisfy the boundary condition at \( x = 0 \), so this equation is invalid. 5. **Analyzing the Fourth Equation**: - Finally, consider the fourth equation: \[ y = A \cos\left(\frac{n \pi x}{L}\right) \sin(\omega t) \] - Check the boundary conditions: - At \( x = 0 \): \[ y(0, t) = A \cos(0) \sin(\omega t) = A \sin(\omega t) \quad (\text{not } 0) \] - This does not satisfy the boundary condition at \( x = 0 \), so this equation is also invalid. ### Conclusion: The valid equations that represent the shape of the string at any time are: - \( y = A \sin\left(\frac{n \pi x}{L}\right) \cos(\omega t) \) - \( y = A \sin\left(\frac{n \pi x}{L}\right) \sin(\omega t) \) ### Final Answer: The correct options are the first and second equations.

To solve the problem, we need to determine which of the given equations can represent the shape of a string undergoing transverse vibrations while being clamped at both ends. The boundary conditions are that the displacement \( y \) of the string must be zero at both ends, \( x = 0 \) and \( x = L \). ### Step-by-Step Solution: 1. **Understanding the Boundary Conditions**: - The string is clamped at both ends, which means that at \( x = 0 \) and \( x = L \), the displacement \( y \) must be zero: \[ y(0, t) = 0 \quad \text{and} \quad y(L, t) = 0 ...
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