Given that wires \( P \) and \( Q \) have equal volumes and are composed of the same material, their volume \( V \) can be defined as \( V = A \times l \), where \( A \) denotes the cross-sectional area and \( l \) represents the length.
Let \( A_P \) and \( A_Q \) be the cross-sectional areas of \( P \) and \( Q \), respectively, and \( l_P \) and \( l_Q \) be their corresponding lengths. With the given ratio \( \frac{A_P}{A_Q} = 4 \), it follows that:
\( A_P = 4A_Q \)
Since the volumes are equal:
\( A_P \cdot l_P = A_Q \cdot l_Q \)
Upon substituting \( A_P = 4A_Q \):
\( 4A_Q \cdot l_P = A_Q \cdot l_Q \)
This leads to the relationship \( l_Q = 4l_P \).
Considering the formula for Young's modulus:
\( \text{Stress} = \frac{F}{A} \) and \( \text{Strain} = \frac{\Delta l}{l} \)
Young's modulus is \( Y = \frac{\text{Stress}}{\text{Strain}} = \frac{F/l}{A/\Delta l} \), which can be rearranged to \( F = \frac{YA\Delta l}{l} \).
For wire \( P \): \( F_1 = \frac{YA_P \Delta l}{l_P} \)
For wire \( Q \) to exhibit the same extension \( \Delta l \): \( F_2 = \frac{YA_Q \Delta l}{l_Q} \)
Substituting \( A_Q = \frac{A_P}{4} \) and \( l_Q = 4l_P \):
\( F_2 = \frac{Y(A_P/4)\Delta l}{4l_P} = \frac{YA_P \Delta l}{16l_P} \)
Therefore, the ratio \( \frac{F_1}{F_2} = \frac{\frac{YA_P \Delta l}{l_P}}{\frac{YA_P \Delta l}{16l_P}} = 16 \).
The calculated value is \( 16 \).
A 2 $\text{kg}$ mass is attached to a spring with spring constant $ k = 200, \text{N/m} $. If the mass is displaced by $ 0.1, \text{m} $, what is the potential energy stored in the spring?
