A wire of negligible mass having uniform area of cross section \( A \) and Young modulus \( Y \) is used to suspend a point mass \( m \). The point mass executes simple harmonic motion in a vertical plane with a period \( T \), then the length of the wire is:
Show Hint
For oscillations of a mass suspended from an elastic wire, the effective spring constant is \( k=\frac{YA}{L} \).
Step 1: Relate wire extension with restoring force.
For a wire of length \(L\), area \(A\), and Young's modulus \(Y\):
\[
Y=\frac{\text{stress}}{\text{strain}}
\]
\[
Y=\frac{F/A}{x/L}
\] Step 2: Rearrange the formula.
\[
Y=\frac{FL}{Ax}
\]
So:
\[
F=\frac{YA}{L}x
\] Step 3: Compare with Hooke's law.
For SHM:
\[
F=kx
\]
Thus, effective force constant is:
\[
k=\frac{YA}{L}
\] Step 4: Use time period formula of SHM.
\[
T=2\pi\sqrt{\frac{m}{k}}
\] Step 5: Substitute value of \(k\).
\[
T=2\pi\sqrt{\frac{m}{YA/L}}
\]
\[
T=2\pi\sqrt{\frac{mL}{YA}}
\] Step 6: Square both sides.
\[
T^2=4\pi^2\frac{mL}{YA}
\] Step 7: Solve for \(L\).
\[
L=\frac{T^2YA}{4\pi^2m}
\]
\[
\boxed{\frac{T^2YA}{4\pi^2m}}
\]