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A block of mass m, when attached to a un...

A block of mass `m`, when attached to a uniform ideal apring with force constant `k` and free length `L` executes SHM. The spring is then cut in two pieces, one with free length n `L` and other with free length `(1 - n)L`. The block is also divided in the same fraction. The smaller part of the block attached to longer part of the spring executes SHM with frequency `f_(1)` . The bigger part of the block attached to smaller part of the spring executes SHM with frequency `f_(2)`. The ratio `f_(1)//f_(2)` is

A

`1`

B

`(n)/(1 - n)`

C

`(1 + n)/(n)`

D

`(n)/(1 + n)`

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The correct Answer is:
To solve the problem, we need to find the ratio of the frequencies \( f_1 \) and \( f_2 \) of two blocks attached to different parts of a spring after it has been cut. Here’s a step-by-step breakdown of the solution: ### Step 1: Understanding the Spring Constant The spring constant \( k \) is inversely proportional to the length of the spring. If the original spring has a length \( L \) and spring constant \( k \), then when the spring is cut into two parts: - The longer part with length \( nL \) will have a spring constant: \[ k_1 = \frac{k}{n} \] - The shorter part with length \( (1-n)L \) will have a spring constant: \[ k_2 = \frac{k}{1-n} \] ### Step 2: Dividing the Mass The mass \( m \) is also divided in the same ratio: - The smaller part of the mass (attached to the longer spring) is: \[ m_1 = n \cdot m \] - The larger part of the mass (attached to the shorter spring) is: \[ m_2 = (1-n) \cdot m \] ### Step 3: Finding the Frequencies The frequency of a mass-spring system executing simple harmonic motion (SHM) is given by: \[ f = \frac{1}{2\pi} \sqrt{\frac{k}{m}} \] Using this formula, we can find the frequencies \( f_1 \) and \( f_2 \): - For the smaller mass \( m_1 \) attached to the longer spring: \[ f_1 = \frac{1}{2\pi} \sqrt{\frac{k_1}{m_1}} = \frac{1}{2\pi} \sqrt{\frac{\frac{k}{n}}{n \cdot m}} = \frac{1}{2\pi} \sqrt{\frac{k}{n^2 m}} \] - For the larger mass \( m_2 \) attached to the shorter spring: \[ f_2 = \frac{1}{2\pi} \sqrt{\frac{k_2}{m_2}} = \frac{1}{2\pi} \sqrt{\frac{\frac{k}{1-n}}{(1-n) \cdot m}} = \frac{1}{2\pi} \sqrt{\frac{k}{(1-n)^2 m}} \] ### Step 4: Finding the Ratio of Frequencies Now we can find the ratio \( \frac{f_1}{f_2} \): \[ \frac{f_1}{f_2} = \frac{\sqrt{\frac{k}{n^2 m}}}{\sqrt{\frac{k}{(1-n)^2 m}}} = \frac{\sqrt{(1-n)^2}}{\sqrt{n^2}} = \frac{1-n}{n} \] Thus, the ratio of the frequencies is: \[ \frac{f_1}{f_2} = \frac{1-n}{n} \] ### Final Answer The ratio \( \frac{f_1}{f_2} \) is \( \frac{1-n}{n} \). ---

To solve the problem, we need to find the ratio of the frequencies \( f_1 \) and \( f_2 \) of two blocks attached to different parts of a spring after it has been cut. Here’s a step-by-step breakdown of the solution: ### Step 1: Understanding the Spring Constant The spring constant \( k \) is inversely proportional to the length of the spring. If the original spring has a length \( L \) and spring constant \( k \), then when the spring is cut into two parts: - The longer part with length \( nL \) will have a spring constant: \[ k_1 = \frac{k}{n} \] ...
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