We are given the following:
Length of the rod, \( L = 1 \, {m} \),
Cross-sectional area before deformation: \( A_0 = 1 \, {cm} \times 1 \, {cm} = 1 \, {cm}^2 \),
Axial tensile force, \( F = 35 \, {kN} = 35000 \, {N} \),
Young’s modulus, \( E = 70 \, {GPa} = 70 \times 10^9 \, {Pa} \),
The cross-sectional area after deformation: \( A_f = 0.998 \, {cm} \times 0.998 \, {cm} = 0.996004 \, {cm}^2 \),
Poisson's ratio, \( \nu \), is the quantity we need to find.
Step 1:
Calculate the axial strain \( \epsilon \).
The axial strain \( \epsilon \) is given by the formula:
\[
\epsilon = \frac{\Delta L}{L} = \frac{F}{A_0 E}
\]
Substitute the given values:
\[
\epsilon = \frac{35000}{1 \times 10^{-4} \times 70 \times 10^9} = \frac{35000}{7 \times 10^6} = 5 \times 10^{-3}
\]
So, the axial strain \( \epsilon = 0.005 \).
Step 2:
Calculate the lateral strain \( \epsilon_{{lateral}} \).
The lateral strain is related to the axial strain by Poisson’s ratio \( \nu \):
\[
\epsilon_{{lateral}} = - \nu \epsilon
\]
The change in the cross-sectional dimension is:
\[
\Delta A = A_0 - A_f = 1 - 0.996004 = 0.003996 \, {cm}^2
\]
Thus, the lateral strain is:
\[
\epsilon_{{lateral}} = \frac{\Delta A}{A_0} = \frac{0.003996}{1} = 0.003996
\]
Step 3:
Relate lateral strain and Poisson’s ratio.
From the relationship:
\[
\epsilon_{{lateral}} = - \nu \epsilon
\]
Substitute the values:
\[
0.003996 = - \nu \times 0.005
\]
Solve for \( \nu \):
\[
\nu = \frac{- 0.003996}{-0.005} = 0.7992
\]
Thus, the Poisson’s ratio is approximately:
\[
\boxed{0.3}
\]