1. Oscillations By M.P.Chaphekar

2. Types Of Motion 1.Translational Motion 2. Rotational Motion 3. Oscillatory Motion

3. Linear simple harmonic Oscillator Example of spring mass oscillator.. Mass in equilibrium position Displacement of Mass towards right Restoring force directed towards left Displacement of Mass towards left Restoring force directed towards right Restoring force F=-kx Restoring force directed towards mean position

4. Linear S.H.M. Linear S.H.M. is defined as the linear periodic motion of a body, in which the restoring force (or acceleration ) is always directed towards the mean position and its magnitude is directly proportional to the displacement from the mean position.

5. Differential Equation of linear S.H.M. Restoring force = force constant

6. Acceleration,velocity and displacement in S.H.M 1. Acceleration

7. Acceleration,velocity and displacement in S.H.M 2. Velocity

8. Acceleration,velocity and displacement in S.H.M 2. Velocity C is constant of integration At Hence

9. Acceleration,velocity and displacement in S.H.M 3 Displacement

10. Acceleration,velocity and displacement in S.H.M 3. Displacement is called phase of S.H.M.

11. How to understand (starting phase or epoch)? TimeDisplacementOscillations starts at α t=0X=0Mean position and particle moves towards positive extreme position 0 t= 0X=ɑPositive extreme positionπ/2 t=0X=0Mean position and particle moves towards negative extreme position π t=0X=-ɑNegative extreme position3π/2 t=0X=0Mean position0

12. Kinetic energy and potential energy of a particle performing S.H.M 1. Kinetic energy OR

13. Kinetic energy and potential energy of a particle performing S.H.M 2 Potential energy Work done dw during the displacement dx is Work done to displace particle from 0 to x is stored as potential energy

14. Kinetic energy and potential energy of a particle performing S.H.M 3 Total energy Note– Total energy is independent of displacement x. Total energy depends upon mass,frequency of oscillation and amplitude of oscillation,

15. Kinetic energy and potential energy of a particle performing S.H.M 4.Variation of K.E. and P.E. in S.H.M. Note– Total energy is at any position in S.H.M. is constant i.e. conserved, Energy E Displacement x P. E K.E At mean position P.E.=0 K.E.=T.E At extreme position K.E.=0 P.E.=T.E

16. Graphical Representation of S.H.M 1 Particle performing S.H.M. Starting from mean position

17. Graphical Representation of S.H.M 1 Particle performing S.H.M. Starting from mean position

18. Graphical Representation of S.H.M 1 Particle performing S.H.M. Starting from mean position

19. Graphical Representation of S.H.M 1 Particle performing S.H.M. Starting from mean position

20. Simple pendulum Definition-An ideal simple pendulum is defined as a heavy particle suspended by weightless inextensible and twistless string from a rigid support.

21. , 2. Motion of simple pendulum as S.H.M L T m mg Fig shows a simple pendulum of length L with a bob of mass m. mgcos mgsin The restoring force is If the is small, (AS L m,g are consants) Thus simple pendulum performs S.H.M Note

22. , Motion of simple pendulum as S.H.M L T m mg mgcos mgsin Period of simple pendulum

23. Damped Oscillations This is differential equation of damped harmonic oscillator.

24. Damped Oscillations The solution of the differential equation gives Graph of displacement against time Note: 1)Amplitude decreases with time exponentially 2)Period of oscillation increases.