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Question: A steel rail of length \(5\,m\) and area of cross section \(40\,c{m^2}\) is prevented from expanding...

A steel rail of length 5m5\,m and area of cross section 40cm240\,c{m^2} is prevented from expanding along its length while the temperature rises by 10C10\,{}^ \circ C. If coefficient of linear expansion and young’s modulus of steel are 1.2×105K11.2 \times {10^{ - 5}}\,{K^{ - 1}} and 2×1011Nm22 \times {10^{11}}\,N{m^{ - 2}} respectively, the force developed in the rail is approximately:
A) 2×107N2 \times {10^7}\,N
B) 3×105N3 \times {10^{ - 5}}\,N
C) 1×105N1 \times {10^5}\,N
D) 2×109N2 \times {10^9}\,N

Explanation

Solution

The force developed in the rail can be determined by using the young’s modulus formula, the young’s modulus is the ratio of the stress and the strain. By using the stress and the strain formula in the young’s modulus formula, the force can be determined.

Formula used:
The young’s modulus is given by,
Y=σεY = \dfrac{\sigma }{\varepsilon }
Where, YY is the young’s modulus of the material, σ\sigma is the stress in the material and ε\varepsilon is the strain in the material.
The stress of the material is given by,
σ=FA\sigma = \dfrac{F}{A}
Where, σ\sigma is the stress, FF is the force and AA is the area.
The strain of the material is given by,
ε=Δll\varepsilon = \dfrac{{\Delta l}}{l}
Where, ε\varepsilon is the strain, Δl\Delta l is the change in the length and ll is the original length.

Complete step by step solution:
Given that,
The length of the rail is, l=5ml = 5\,m,
The Area of the cross section is, A=40cm2=40×104m2A = 40\,c{m^2} = 40 \times {10^{ - 4}}\,{m^2},
The change in temperature is, ΔT=10C\Delta T = 10\,{}^ \circ C,
The coefficient of the linear expansion is, α=1.2×105K1\alpha = 1.2 \times {10^{ - 5}}\,{K^{ - 1}},
The young’s modulus of the material is, Y=2×1011Nm2Y = 2 \times {10^{11}}\,N{m^{ - 2}}.
The relation between the change in length and the change in the temperature is given by,
Δl=l×α×ΔT\Delta l = l \times \alpha \times \Delta T
By rearranging the terms in the above equation, then
Δll=α×ΔT...............(1)\dfrac{{\Delta l}}{l} = \alpha \times \Delta T\,...............\left( 1 \right)
Now,
The young’s modulus is given by,
Y=σεY = \dfrac{\sigma }{\varepsilon }
By substituting the stress and strain formula in the above equation, then the above equation is written as,
Y=(FA)(Δll)Y = \dfrac{{\left( {\dfrac{F}{A}} \right)}}{{\left( {\dfrac{{\Delta l}}{l}} \right)}}
By substituting the equation (1) in the above equation, then
Y=(FA)α×ΔTY = \dfrac{{\left( {\dfrac{F}{A}} \right)}}{{\alpha \times \Delta T}}
By rearranging the terms in the above equation, then the above equation is written as,
Y=FA×α×ΔTY = \dfrac{F}{{A \times \alpha \times \Delta T}}
By rearranging the terms in the above equation, then the above equation is written as,
F=Y×A×α×ΔTF = Y \times A \times \alpha \times \Delta T
By substituting the young’s modulus, cross sectional area, coefficient of the linear expansion and change in temperature in the above equation, then
F=2×1011×40×104×1.2×105×10F = 2 \times {10^{11}} \times 40 \times {10^{ - 4}} \times 1.2 \times {10^{ - 5}} \times 10
By multiplying the terms in the above equation, then
F=9600NF = 9600\,N
The above equation is also written as,
F=0.96×104NF = 0.96 \times {10^4}\,N
Then the force is approximately equal to,
F1×105NF \simeq 1 \times {10^5}\,N

Hence, the option (C) is the correct answer.

Note: The force of the object is directly proportional to the young’s modulus of the material, cross sectional area of the material, coefficient of the linear expansion and the change in temperature. As the young’s modulus of the material, cross sectional area of the material, coefficient of the linear expansion and the change in temperature increases, then the force also increases.