To determine how the potential energy of a spring changes when the stretching is increased, we can use Hooke's Law and the formula for the potential energy of the spring. The potential energy \(U\) stored in a spring is given by:
\(U = \frac{1}{2}kz^2\)
where:
Given that initially the spring is stretched by a distance \(z\) and the potential energy is \(U\):
\(U = \frac{1}{2}kz^2\)
If the stretching is increased to \(n\) times, then the new stretching distance will be \(nz\). The new potential energy \(U'\) is given by:
\(U' = \frac{1}{2}k(nz)^2\)
Which simplifies to:
\(U' = \frac{1}{2}k \cdot n^2 \cdot z^2\)
Comparing the original and new potential energies:
\(U' = \frac{1}{2}k \cdot n^2 \cdot z^2 = n^2 \cdot \frac{1}{2}kz^2 = n^2 \cdot U\)
Thus, the potential energy of the spring when stretched to \(n\) times the original distance is \(n^2U\).
Therefore, the correct answer is: \( n^2U \)
Two springs of force constants \( k_1 \) and \( k_2 \) are connected to a mass \( m \) as shown. The angular frequency of this configuration is:
A solid cylinder of mass 2 kg and radius 0.2 m is rotating about its own axis without friction with angular velocity 5 rad/s. A particle of mass 1 kg moving with a velocity of 5 m/s strikes the cylinder and sticks to it as shown in figure.
The angular velocity of the system after the particle sticks to it will be: