91Ó°ÊÓ

Diameter of the sphere:\(d = 35\;{\rm{cm}}\)

Length of steel cable:\(L = 10.5\;{\rm{m}}\)

The temperature at which measurements are made:\(T = 20.0\;^\circ {\rm{C}} = 293\;{\rm{K}}\)

The expansion in length:\(\Delta L = 2.0\;{\rm{mm}}\)

The coefficient of expansion of steel is: \(1.2 \times {10^{ - 5}}\;{{\rm{K}}^{{\rm{ - 1}}}}\)

It is a common observation that matter changes its shape, size, volume, or density in response to variation in temperature. This phenomenon is known as thermal expansion. If the length of any object changes in response to the variation in temperature, it is called Linear Expansion. The increase in length \(\left( {{\bf{\Delta L}}} \right)\) can be calculated as-

\({\bf{\Delta L = \alpha L\Delta T}}\;\; \cdot \cdot \cdot \cdot \cdot \cdot \cdot \cdot \cdot \cdot \cdot \cdot \cdot \cdot \cdot \cdot \cdot \cdot \cdot \cdot \cdot \cdot \cdot \cdot \cdot \cdot \cdot \cdot \cdot \cdot \cdot \cdot \cdot \cdot \cdot \cdot \cdot \cdot \left( 1 \right)\)

Here, \({\bf{\alpha }}\) is the coefficient of expansion and \({\bf{\Delta T}}\) is the variation in temperature.

Using equation (1), the increase in length is given as-

\(\begin{array}{c}\Delta L = \alpha L\Delta T\\ = \alpha L\left( {{T_o} - T} \right)\end{array}\)

Here\({T_o}\)is the final temperature at which sphere will brush the floor.

For the given values the equation becomes-

\(\begin{array}{l}2 \times {10^{ - 3}}\;{\rm{m}}\; = \left( {1.2 \times {{10}^{ - 5}}\;{{\rm{K}}^{{\rm{ - 1}}}}} \right)\left( {10.5\;{\rm{m}}} \right)\left( {{T_o} - 293\;{\rm{K}}} \right)\\\left( {{T_o} - 293\;{\rm{K}}} \right) = 15.9\;{\rm{K}}\end{array}\)

Solving further,

\(\begin{array}{c}{T_o} = \left( {293 + 15.9} \right)\;{\rm{K}}\\ = 308.9\;{\rm{K}}\\ = 35.9\;^\circ {\rm{C}}\end{array}\)

The temperature at which the sphere will brush the surface is \(35.9\;^\circ {\rm{C}}\).