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Question: The radius of a metal sphere at room temperature \[T\] is \[\;R\], and the coefficient of linear exp...

The radius of a metal sphere at room temperature TT is   R\;R, and the coefficient of linear expansion of the metal is α\alpha . The sphere is heated a little by a temperature ΔT\Delta T so that its new temperature is (T+ΔT).  \left( {T + \Delta T} \right).\; the increase in the volume of the sphere is approximate:

A. 2πRαT2\pi R\alpha T
B. π2RαT{\pi ^2}R\alpha T
C. 4πR3αΔT/34\pi {R^3}\alpha \Delta T/3
D. 4πR3αΔT4\pi {R^3}\alpha \Delta T

Explanation

Solution

Thermal expansion is defined as the tendency of matter to change its shape, area, or volume in response to a change in temperature. This expansion occurs when the substance is heated up. When we heat the substance the particles inside it vibrate faster which creates more space in between the particles. This results in the expansion of the substance.

Complete step by step solution:
Given a three-dimensional body. Let the body be the metal sphere. The body has room temperature TT and volume VV. Its radius at the room temperature TT is RR.
When we heat a three-dimensional body its volume increases. This is caused by thermal expansion as we already said.
Given that we have increased the temperature by T+ΔTT + \Delta T. Also given that the coefficient of linear expansion of the metal is α\alpha .
The volumetric thermal expansion is given as,
αV=1VdVdT{\alpha _{\text{V}}} = \dfrac{1}{{\text{V}}}\dfrac{{{\text{dV}}}}{{{\text{dT}}}}
Here, α\alpha is the coefficient of thermal expansion with respect to volume.
V{\text{V}} is the volume of the material
dVdT\dfrac{{{\text{dV}}}}{{{\text{dT}}}} is the rate of change of volume with respect to temperature.
Similar to volume expansion we also have a linear expansion that applies to one dimension bodies.
Coefficient of Linear expansion= α\alpha
Coefficient of Volume expansion= 3α3\alpha
We can substitute the formula for the coefficient of thermal expansion with respect to volume from above. So we get,
1VdVdT=3α\dfrac{1}{{\text{V}}}\dfrac{{{\text{dV}}}}{{{\text{dT}}}} = 3\alpha
We need to find only the volume changedV{\text{dV}}. Therefore rearranging the above equation,
dV = 3VαdT{\text{dV = }}3{\text{V}}\alpha {\text{dT}}
We know the volume of the sphere, V{\text{V}}=43πR3αdT\dfrac{4}{3}\pi {R^3}\alpha {\text{dT}}
Also change in the temperature is given as dT{\text{dT}}=ΔT\Delta T
Therefore,
dV=4πR3αΔT{\text{dV}} = 4\pi {R^3}\alpha \Delta T
Hence the correct option is D.

Note:
Generally, the coefficient of volume expansion is givens as,
αV=1V(VT)p{\alpha _{\text{V}}} = \dfrac{1}{{\text{V}}}{(\dfrac{{\partial {\text{V}}}}{{\partial {\text{T}}}})_{\text{p}}}
The subscript pp indicates that the pressure is held constant during the expansion. In the case of a gas, keeping pressure constant is important, as the volume of a gas will vary appreciably with pressure as well as with temperature. But in the above case, we didn’t consider pressure. Because in solids we can ignore the effects of the pressure of the material.