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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)`

Text Solution

AI Generated Solution

The correct Answer is:
To solve the problem, we need to analyze the situation step by step, focusing on the properties of the spring and the masses involved in the Simple Harmonic Motion (SHM). ### Step-by-Step Solution: 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 \( k \), when the spring is cut into two parts, the spring constants of the new springs can be calculated. - For the longer part of the spring with length \( nL \), the spring constant \( k_1 \) is given by: \[ k_1 = \frac{k}{n} \] - For the shorter part of the spring with length \( (1-n)L \), the spring constant \( k_2 \) is given by: \[ k_2 = \frac{k}{1-n} \] 2. **Dividing the Mass**: - The mass \( m \) is also divided in the same ratio. The smaller part of the mass \( m_1 \) (attached to the longer spring) is: \[ m_1 = (1-n)m \] - The bigger part of the mass \( m_2 \) (attached to the shorter spring) is: \[ m_2 = n m \] 3. **Calculating Frequencies**: - The frequency of SHM is given by the formula: \[ f = \frac{1}{2\pi} \sqrt{\frac{k}{m}} \] - For the smaller mass \( m_1 \) attached to the longer spring (with spring constant \( k_1 \)): \[ f_1 = \frac{1}{2\pi} \sqrt{\frac{k_1}{m_1}} = \frac{1}{2\pi} \sqrt{\frac{\frac{k}{n}}{(1-n)m}} = \frac{1}{2\pi} \sqrt{\frac{k}{n(1-n)m}} \] - For the bigger mass \( m_2 \) attached to the shorter spring (with spring constant \( k_2 \)): \[ f_2 = \frac{1}{2\pi} \sqrt{\frac{k_2}{m_2}} = \frac{1}{2\pi} \sqrt{\frac{\frac{k}{1-n}}{n m}} = \frac{1}{2\pi} \sqrt{\frac{k}{n(1-n)m}} \] 4. **Finding the Ratio of Frequencies**: - Now, we can find the ratio \( \frac{f_1}{f_2} \): \[ \frac{f_1}{f_2} = \frac{\sqrt{\frac{k}{n(1-n)m}}}{\sqrt{\frac{k}{n(1-n)m}}} = 1 \] ### Final Answer: The ratio \( \frac{f_1}{f_2} \) is \( 1 \).

To solve the problem, we need to analyze the situation step by step, focusing on the properties of the spring and the masses involved in the Simple Harmonic Motion (SHM). ### Step-by-Step Solution: 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 \( k \), when the spring is cut into two parts, the spring constants of the new springs can be calculated. - For the longer part of the spring with length \( nL \), the spring constant \( k_1 \) is given by: \[ ...
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