The elastic strain energy stored in a rod under uniaxial tensile load is given by the formula:
$U = \frac{F^2 L}{2 A E}$
Where:
We are given two rods, P and Q, made of the same material (\(E_P = E_Q = E\)) and subjected to identical tensile loads (\(F_P = F_Q = F\)). The relationships between their dimensions are:
The cross-sectional area (A) is related to the diameter (d) by \(A = \frac{\pi d^2}{4}\). Therefore, the relationship between the areas is:
$A_P = \frac{\pi d_P^2}{4} = \frac{\pi (2 d_Q)^2}{4} = \frac{\pi (4 d_Q^2)}{4} = 4 \left( \frac{\pi d_Q^2}{4} \right) = 4 A_Q$
So, \(A_P = 4 A_Q\).
We need to find the ratio \(\frac{U_P}{U_Q}\).
$\frac{U_P}{U_Q} = \frac{\frac{F_P^2 L_P}{2 A_P E_P}}{\frac{F_Q^2 L_Q}{2 A_Q E_Q}}$
Substitute the known relationships (\(F_P = F_Q\), \(E_P = E_Q\), \(L_P = 2 L_Q\), \(A_P = 4 A_Q\)):
$\frac{U_P}{U_Q} = \frac{\frac{F^2 (2 L_Q)}{2 (4 A_Q) E}}{\frac{F^2 L_Q}{2 A_Q E}}$
Simplify the expression:
$\frac{U_P}{U_Q} = \frac{2 L_Q / (8 A_Q E)}{L_Q / (2 A_Q E)} = \frac{2 L_Q}{8 A_Q E} \times \frac{2 A_Q E}{L_Q} = \frac{2 \times 2}{8} = \frac{4}{8} = \frac{1}{2}$
The ratio of elastic strain energy stored in rod P to that stored in rod Q is 1:2.
Both the numerator and the denominator of $\frac{3}{4}$ are increased by a positive integer, x, and those of $\frac{15}{17}$ are decreased by the same integer. This operation results in the same value for both the fractions.
What is the value of x?
| Metal | Pilling-Bedworth Ratio |
| Li | 0.57 |
| Ce | 1.16 |
| Ta | 2.33 |
| W | 3.40 |