A massless spring of length \( l \) and spring constant \( k \) oscillates with a time period \( T \) when loaded with a mass \( m \). The spring is now cut into three equal parts and connected in parallel. The frequency of oscillation of the combination when it is loaded with a mass \( 4m \) is:
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Show Hint
For a spring cut into \( n \) equal parts, the new spring constant is \( k' = nk \), and when connected in parallel, the effective spring constant is \( k_{\text{eff}} = n^2 k \).
Step 1: Understanding the Effect of Cutting the Spring
The time period for a mass-spring system is given by:
\[
T = 2\pi \sqrt{\frac{m}{k}}
\]
When the spring is cut into three equal parts, each segment will have a new spring constant:
\[
k' = 3k
\]
Since they are connected in parallel, the effective spring constant becomes:
\[
k_{\text{eff}} = 3k + 3k + 3k = 9k
\]
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Step 2: Finding the New Time Period
The new time period when a mass \( 4m \) is attached:
\[
T' = 2\pi \sqrt{\frac{4m}{9k}}
\]
\[
T' = 2\pi \times \frac{2}{3} \sqrt{\frac{m}{k}}
\]
\[
T' = \frac{2}{3} T
\]
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Step 3: Finding the Frequency
Frequency is the reciprocal of the time period:
\[
f' = \frac{1}{T'} = \frac{1}{\frac{2}{3} T} = \frac{3}{2T}
\]
Thus, the frequency of oscillation of the combination is:
\[
\mathbf{\frac{3}{2T}}
\]
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