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Published bySusanna Ferguson Modified over 9 years ago
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Simple Harmonic Motion
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l Vibrations è Vocal cords when singing/speaking è String/rubber band l Simple Harmonic Motion è Restoring force proportional to displacement è Springs F = -kx 11
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Question II A mass on a spring oscillates back & forth with simple harmonic motion of amplitude A. A plot of displacement (x) versus time (t) is shown below. At what points during its oscillation is the magnitude of the acceleration of the block biggest? 1. When x = +A or -A (i.e. maximum displacement) 2. When x = 0 (i.e. zero displacement) 3. The acceleration of the mass is constant +A t -A x 17
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Potential Energy in Spring l Force of spring is Conservative è F = -k x è W = -1/2 k x 2 è Work done only depends on initial and final position è Define Potential Energy PE spring = ½ k x 2 Force x work 20
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***Energy in SHM*** l A mass is attached to a spring and set to motion. The maximum displacement is x=A è Energy = PE + KE = constant! = ½ k x 2 + ½ m v 2 è At maximum displacement x=A, v = 0 Energy = ½ k A 2 + 0 è At zero displacement x = 0 Energy = 0 + ½ mv m 2 Since Total Energy is same ½ k A 2 = ½ m v m 2 v m = sqrt(k/m) A m x x=0 0 x PE S 25
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Question 3 A mass on a spring oscillates back & forth with simple harmonic motion of amplitude A. A plot of displacement (x) versus time (t) is shown below. At what points during its oscillation is the speed of the block biggest? 1. When x = +A or -A (i.e. maximum displacement) 2. When x = 0 (i.e. zero displacement) 3. The speed of the mass is constant +A t -A x 29
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Question 4 l A spring oscillates back and forth on a frictionless horizontal surface. A camera takes pictures of the position every 1/10 th of a second. Which plot best shows the positions of the mass. EndPoint Equilibrium EndPoint Equilibrium EndPoint Equilibrium 38 123123
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X=0 X=A X=-A X=A; v=0; a=-a max X=0; v=-v max ; a=0X=-A; v=0; a=a max X=0; v=v max ; a=0 X=A; v=0; a=-a max Springs and Simple Harmonic Motion 32
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What does moving in a circle have to do with moving back & forth in a straight line ?? y x -R R 0 1 1 22 33 4 4 55 66 R 8 7 8 7 x x = R cos = R cos ( t ) since = t 34
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SHM and Circles
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Simple Harmonic Motion: x(t) = [A]cos( t) v(t) = -[A ]sin( t) a(t) = -[A 2 ]cos( t) x(t) = [A]sin( t) v(t) = [A ]cos( t) a(t) = -[A 2 ]sin( t) x max = A v max = A a max = A 2 Period = T (seconds per cycle) Frequency = f = 1/T (cycles per second) Angular frequency = = 2 f = 2 /T For spring: 2 = k/m OR 36
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Example A 3 kg mass is attached to a spring (k=24 N/m). It is stretched 5 cm. At time t=0 it is released and oscillates. Which equation describes the position as a function of time x(t) = A) 5 sin( t)B) 5 cos( t)C) 24 sin( t) D) 24 cos( t)E) -24 cos( t) 39
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Example A 3 kg mass is attached to a spring (k=24 N/m). It is stretched 5 cm. At time t=0 it is released and oscillates. What is the total energy of the block spring system? 43
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Example A 3 kg mass is attached to a spring (k=24 N/m). It is stretched 5 cm. At time t=0 it is released and oscillates. What is the maximum speed of the block? 46
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Example A 3 kg mass is attached to a spring (k=24 N/m). It is stretched 5 cm. At time t=0 it is released and oscillates. How long does it take for the block to return to x=+5cm? 49
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Pendulum Motion l For small angles è T = mg è T x = -mg (x/L) Note: F proportional to x! F x = m a x -mg (x/L) = m a x a x = -(g/L) x Recall for SHO a = - 2 x = sqrt(g/L) T = 2 sqrt(L/g) Period does not depend on A, or m! m L x T mg 37
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Example: Clock l If we want to make a grandfather clock so that the pendulum makes one complete cycle each sec, how long should the pendulum be?
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Question 1 Suppose a grandfather clock (a simple pendulum) runs slow. In order to make it run on time you should: 1. Make the pendulum shorter 2. Make the pendulum longer 38
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Summary l Simple Harmonic Motion è Occurs when have linear restoring force F= -kx x(t) = [A] cos( t) v(t) = -[A ] sin( t) a(t) = -[A ] cos( t) l Springs è F = -kx è U = ½ k x 2 = sqrt(k/m) l Pendulum (Small oscillations) = sqrt(L/g) 50
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