Presentation is loading. Please wait.

Presentation is loading. Please wait.

Oscillatory Motion Serway & Jewett (Chapter 15).

Similar presentations


Presentation on theme: "Oscillatory Motion Serway & Jewett (Chapter 15)."— Presentation transcript:

1 Oscillatory Motion Serway & Jewett (Chapter 15)

2 M M M Equilibrium position: no net force
The spring force is always directed back towards equilibrium (hence called the ‘restoring force’). This leads to an oscillation of the block about the equilibrium position. M For an ideal spring, the force is proportional to displacement. For this particular force behaviour, the oscillation is simple harmonic motion. x F = -kx

3 SHM: x(t) A = amplitude t f = phase constant w = angular frequency
A is the maximum value of x (x ranges from +A to -A). f gives the initial position at t=0: x(0) = A cosf . w is related to the period T and the frequency f = 1/T T (period) is the time for one complete cycle (seconds). Frequency f (cycles per second or hertz, Hz) is the number of complete cycles per unit time.

4 units: radians/second or s-1
 (“omega”) is called the angular frequency of the oscillation.

5 Velocity and Acceleration
a(t) =- w 2 x(t)

6 Position, Velocity and Acceleration
x(t) t v(t) t a(t) t Question: Where in the motion is the velocity largest? Where in the motion is acceleration largest?

7 Example: SHM can produce very large accelerations if the frequency is high. Engine piston at 4000 rpm, amplitude 5 cm:

8 Simple Harmonic Motion
SHM: We can differentiate x(t): and find that acceleration is proportional to displacement: a(t) = - w 2 x(t) But, how do we know something will obey x=Acos(t) ???

9 Mass and Spring M Newton’s 2nd Law: F = -kx so x
This is a 2nd order differential equation for the function x(t). Recall that for SHM, a = -w 2 x : identical except for the proportionality constant. So the motion of the mass will be SHM: x(t) = A cos (wt + f), and to make the equations for acceleration match, we require that , or (and w = 2p f, etc.). Note: The frequency is independent of amplitude

10 Example: Elastic bands and a mass
Example: Elastic bands and a mass. A mass, m, is attached to two elastic bands. Each has tension T. The system is on a frictionless horizontal surface. Will this behave like a SHO?

11 Quiz The ball oscillates vertically on a single spring with period T0 . If two identical springs are used, the new period will be longer shorter by a factor of 2 4

12 Quiz The ball oscillates vertically on a single spring with period T0 . If two identical springs are used, the period will be longer shorter by a factor of 2 4 1

13 Quiz μs=0.5 B ω=10 s-1 The amplitude of the oscillation gradually increases till block B starts to slip. At what A does this happen? (there is no friction between the large block and the surface) Any A 5 cm 50 cm Not known without mB.

14 Solution

15 Look again at the block & spring
Energy in SHM M Look again at the block & spring We could also write E = K+U = ½ m(vmax )2

16 E U, K oscillate back and forth “out of phase” with each other; the total E is constant. n.b.! U, K go through two oscillations while the position x(t) goes through one. U K t T x t v

17 Suppose you double the amplitude of the motion:
1) What happens to the maximum speed? Doubles 4 x Larger Doesn’t change 2) What happens to the maximum acceleration? Doubles 4 x Larger Doesn’t change 3) What happens to the the total energy? Doubles 4 x Larger Doesn’t change

18 Summary SHM: (get v, a with calculus) Definitions: amplitude, period, frequency, angular frequency, phase, phase constant. The acceleration is proportional to displacement: a(t) = -w2 x(t) Practice problems, Chapter 15: 3, 5, 11, 19, 23 (6th ed – Chapter 13) 1, 3, 5, 9, 19, 23


Download ppt "Oscillatory Motion Serway & Jewett (Chapter 15)."

Similar presentations


Ads by Google