Test Index

Work, Power and Energy

© examsnet.com
Question : 4 of 30
Marks: +1, -0
The potential energy function for a particle executing linear simple harmonic motion is given by V(x)=kx22V(x) = \frac{kx^2}{2}, where kk is the force constant of the oscillator. For k=0.5 N m1k = 0.5 \text{ N m}^{-1}, the graph of V(x)V(x) versus xx is shown in figure. Show thata particle of total energy 1 J moving under this potential must ‘turn back’ when it reaches x=±2x = \pm 2 m.
Solution:  
The total energy of an oscillator is the sum of kinetic energy and potential energy at any instant.
Total energy = Kinetic energy + Potential energy
E=12mu2+12kx2E = \frac{1}{2} m u^{2} + \frac{1}{2} k x^{2}
The particle turn back at the instant, when its velocity becomes zero, u=0u = 0,
Therefore E=12mu2+12kx2=0+12kx2E = \frac{1}{2} m u^{2} + \frac{1}{2} k x^{2} = 0 + \frac{1}{2} k x^{2}
1=12×12x21 = \frac{1}{2} \times \frac{1}{2} x^{2} (E=1 J,k=1/2 N/m)(\because E = 1 \text{ J}, k = 1/2 \text{ N/m})
1=14x21 = \frac{1}{4} x^{2}
x2=4,x=±2x^{2} = 4, x = \pm 2
Thus, the particle of total energy 1 J moving under this potential, must turn back at x=±2x = \pm 2 m.
© examsnet.com
Go to Question: