The tension \( T \) in the wire, due to the masses, is given by:
\[ T = \left( \frac{2m_1m_2}{m_1 + m_2} \right) g = \frac{80}{3} \, \text{N}. \]The cross-sectional area \( A \) of the wire is:
\[ A = \pi r^2 = 16\pi \times 10^{-10} \, \text{m}^2. \]The strain \( \frac{\Delta \ell}{\ell} \) in the wire is given by:
\[ \text{Strain} = \frac{F}{AY} = \frac{T}{AY}. \]Substitute the values:
\[ \text{Strain} = \frac{\frac{80}{3}}{16\pi \times 10^{-10} \times 2 \times 10^{11}} = \frac{1}{12\pi}. \]Thus, \(\alpha = 12\).
The Young's modulus of a steel wire of length \(6 m\) and cross-sectional area \(3 \,mm ^2\), is \(2 \times 10^{11}\) \(N / m ^2\). The wire is suspended from its support on a given planet A block of mass \(4 kg\) is attached to the free end of the wire. The acceleration due to gravity on the planet is \(\frac{1}{4}\) of its value on the earth The elongation of wire is (Take \(g\) on the earth \(=10\, m / s ^2\)) :
A steel wire of length 3.2 m (Ys = 2.0 × 1011 Nm-2) and a copper wire of length 4.4 m (Yc = 1.1 × 1011 Nm-2), both of radius 1.4 mm are connected end to end. When stretched by a load, the net elongation is found to be 1.4 mm. The load applied, in Newton, will be:
\((Given: π = \frac{22}{7})\)