To solve this problem, we must understand how elongation is affected by the dimensions of the wire. The elongation (\( \Delta L \)) of a wire when a force \( F \) is applied can be described by Hooke's Law:
\( \Delta L = \frac{FL}{AE} \)
where \( L \) is the original length, \( A \) is the cross-sectional area, and \( E \) is the Young's modulus of the material.
Original Wire:
The elongation given is 0.04 m with force \( F \). Let's analyze:
Modified Wire:
The new elongation \( \Delta L' \) is:
\( \Delta L' = \frac{F(2L)}{4A_1E} = \frac{2FL}{4A_1E} = \frac{FL}{2A_1E} \)
Substituting the known elongation for the original wire:
\( \Delta L' = \frac{1}{2} \Delta L_1 = \frac{1}{2} \times 0.04 \, \text{m} = 0.02 \, \text{m} \)
Convert 0.02 m to centimeters:
\( 0.02 \, \text{m} = 2 \, \text{cm} \)
This result is within the expected range [2, 2].
Conclusion: The elongation of the wire when both length and diameter are doubled, keeping the force constant, is 2 cm.
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?
