Simple Harmonic Motion(SHM)

Slides:



Advertisements
Similar presentations
Kinematics of simple harmonic motion (SHM)
Advertisements

Harmonic Motion and Waves
SHM -1.
Adapted from Holt book on physics
Introduction to Oscillations and Simple Harmonic Motion
Simple Harmonic Motion
Moza M. Al-Rabban Professor of Physics
Simple Harmonic Motion
Simple Harmonic Motion
Simple Harmonic Motion
Simple Harmonic Motion
Chapter 14 Oscillations Chapter Opener. Caption: An object attached to a coil spring can exhibit oscillatory motion. Many kinds of oscillatory motion are.
Oscillations and Simple Harmonic Motion:
Oscillation.
Oscillations and Simple Harmonic Motion : Mechanics C.
Simple Harmonic Motion
Harmonic Motion AP Physics C.
Physics 6B Oscillations Prepared by Vince Zaccone
Waves Physics H.
Oscillations Unit 7.
CHAPTER 10 Elasticity and Oscillations
Periodic Motion - 1.
A. Introduction 1. Oscillations: motions that repeat themselves a)Swinging chandeliers, boats bobbing at anchor, oscillating guitar strings, pistons in.
Objectives: 1)Describe how energy and speed vary in simple harmonic motion 2) Calculate sinusoidal wave properties in terms of amplitude, wavelength, frequency,
SIMPLE HARMOIC MOTION CCHS Physics.
Chapter 11 - Simple Harmonic Motion
Vibrations and Waves Hooke’s Law Elastic Potential Energy Comparing SHM with Uniform Circular Motion Position, Velocity and Acceleration.
Vibrations and Waves m Physics 2053 Lecture Notes Vibrations and Waves.
For this section we start with Hooke’s Law. But we already learned this. (partially)
Simple Harmonic Motion. l Vibrations è Vocal cords when singing/speaking è String/rubber band l Simple Harmonic Motion è Restoring force proportional.
Oscillations and Waves An oscillation is a repetitive motion back and forth around a central point which is usually an equilibrium position. A special.
Oscillations - SHM. Oscillations In general an oscillation is simply aback and forth motion Since the motion repeats itself, it is called periodic We.
Simple Harmonic Motion
Copyright © 2009 Pearson Education, Inc. Chapter 14 Oscillations.
Simple Harmonic Oscillator and SHM A Simple Harmonic Oscillator is a system in which the restorative force is proportional to the displacement according.
Chapter 15 Oscillatory Motion.
Copyright © 2009 Pearson Education, Inc. Oscillations of a Spring Simple Harmonic Motion Energy in the Simple Harmonic Oscillator The Simple Pendulum Lecture.
Physics 207: Lecture 19, Pg 1 Lecture 19Goals: Chapter 14 Chapter 14  Interrelate the physics and mathematics of oscillations.  Draw and interpret oscillatory.
4.1.1Describe examples of oscillation Define the terms displacement, amplitude, frequency, period, and phase difference Define simple harmonic.
Physics Vibrations and Waves 11.1 Simple Harmonic Motion 11.2 Energy in SHM 11.3 Period and sinusoidal nature of SHM 11.4 The Simple Pendulum.
Chapter 13: Vibrations and Waves
Periodic Motion What is periodic motion?
Simple Harmonic Motion This type of motion is the most pervasive motion in the universe. All atoms oscillate under harmonic motion. We can model this motion.
Physics 207, Lecture 18, Nov. 3 Goals: Chapter 14
Periodic Motions.
Chapter 11: Harmonic Motion
Physics 1501: Lecture 25, Pg 1 Physics 1501: Lecture 25 Today’s Agenda l Homework #9 (due Friday Nov. 4) l Midterm 2: Nov. 16 l Topics çReview of static.
Phys 250 Ch14 p1 Chapter 13: Periodic Motion What we already know: Elastic Potential Energy energy stored in a stretched/compressed spring Force: Hooke’s.
Simple Harmonic Motion
Oscillations. Periodic Motion Periodic motion is motion of an object that regularly returns to a given position after a fixed time interval A special.
What do these two systems have in common? Gravity is the driving force If it is frictionless, energy is conserved It would continue indefinitely.
Simple Harmonic Motion Periodic Motion Simple periodic motion is that motion in which a body moves back and forth over a fixed path, returning to each.
Simple Harmonic Motion AP Physics C. Simple Harmonic Motion What is it?  Any periodic motion that can be modeled with a sin or cosine wave function.
PHY 101: Lecture Ideal Spring and Simple Harmonic Motion 10.2 Simple Harmonic Motion and the Reference Circle 10.3 Energy and Simple Harmonic Motion.
Chapter 14 Springs A TRAMPOLINE exerts a restoring force on the jumper that is directly proportional to the average force required to displace the mat.
PHY 151: Lecture Motion of an Object attached to a Spring 12.2 Particle in Simple Harmonic Motion 12.3 Energy of the Simple Harmonic Oscillator.
S H M a n d W a v e s B a s i c s. T h e O s c i l l a t o r When displaced from its vertical equilibrium position, this plastic ruler oscillates back.
Assuming both these system are in frictionless environments, what do they have in common? Energy is conserved Speed is constantly changing Movement would.
Harmonic Motion AP Physics C.
Simple Harmonic Motion
Oscillations © 2014 Pearson Education, Inc..
Simple Harmonic Motion
Harmonic Motion AP Physics C.
Harmonic Motion AP Physics C.
Chapter 14: Simple harmonic motion
Harmonic Motion AP Physics C.
Harmonic Motion AP Physics C.
Harmonic Motion AP Physics C.
Simple Harmonic Motion and Wave Interactions
Presentation transcript:

Simple Harmonic Motion(SHM) Vibration (oscillation) Equilibrium position – position of the natural length of a spring Amplitude – maximum displacement

Period and Frequency Period (T) – Time for one complete cycle (back to starting point) Frequency (Hz) – Cycles per second Angular Velocity/Frequency (rad/s), w – FIND THIS FIRST f = 1 T = 1 w = 2pf T f

Period and Frequency A radio station has a frequency of 103.1 M Hz. What is the period of the wave? 103.1 M Hz 1X106 Hz = 1.031 X 108 Hz 1M Hz T = 1/f = 1/(1.031 X 108 Hz) = 9.700 X 10-9 s

Cosines and Sines Imagine placing a pen on a vibrating mass Draws a cosine wave

Starting at the Amplitude Used if spring is pulled out (or compressed) to full position x(t) = A cos2pt = A cos2pft = A coswt T v(t) = -vmaxsinwt vmax = wA A = Amplitude t = time T = period f = frequency

An air-track glider is attached to a spring. It is pulled 20 An air-track glider is attached to a spring. It is pulled 20.0 cm to the right and makes 15 oscillations in 10.0s Calculate the period Calculate the angular velocity (w) Calculate the maximum speed Calculate the speed and position at t = 0.800s

A mass starts at x=A. Using only variables, calculate at what time as a fraction of T that the object passes through ½ A. x(t) = A cos2pt T

x = A coswt v = -vosinwt a = -aocoswt Velocity is the derivative of position Acceleration is the derivative of velocity

A loudspeaker vibrates at 262 Hz (middle C) A loudspeaker vibrates at 262 Hz (middle C). The amplitude of the cone of the speaker is 1.5 X 10-4 m. Write the equation to describe the position of the cone over time. (x = (1.5 X 10-4 m) cos(1650 rad/s)t) Calculate the position at t = 1.00 ms. (-1.2 X 10-5 m) Calculate the maximum velocity and acceleration (0.25 m/s, 410 m/s2 )

F = ma kx = ma a = kx/m But we don’t know k or m a = k x Solve for k/m m T = 2p m k T2 = (2p)2m k = (2p)2 = (2p)2f2 m T2

a = k x m ao = (2pf)2x = (2pf)2A ao = [(2p)(262 Hz)]2(1.5 X 10-4 m) = 410 m/s2

Find the amplitude, frequency and period of motion for an object vibrating at the end of a spring that follows the equation: x = (0.25 m)cos p t 8.0 (0.25 m, 1/16 Hz, 16 s)

Find the position of the object after 2.0 seconds. x = (0.25 m)cos p t 8.0 x = (0.25 m)cos p 4.0 x = 0.18 m

The Phase Constant Do not always start at the Amplitude Can start your observations at any time o is the starting angle using the circle model x(t) = A cos(wt + o) v(t) = -vmaxsin(wt + o) vmax = wA w = 2pf = 2p/T

An object on a spring oscillates with a period of 0 An object on a spring oscillates with a period of 0.800 s and an amplitude of 10.0 cm. At t=0, it is 5.0 cm to the left of equilibrium and moving to the left. Calculate the phase constant (in radians) from the initial conditions. (2/3p rad) Calculate the position at t = 2.0 s (5.0 cm) Calculate the velocity at t = 2.0 s (68 cm/s) What direction is the object moving at 2 s? (right)

A mass of 4. 00 kg is attached to a horizontal spring with k = 100 N/m A mass of 4.00 kg is attached to a horizontal spring with k = 100 N/m. It is displaced 10.0 cm from equilibrium and released. Calculate the period. (1.25 s) Calculate the angular velocity w. (5.00 rad/s) Calculate the phase angle (in radians) from the initial conditions. (p/2 rad) Calculate the maximum velocity (0.500 m/s) Calculate the velocity when x = 5.0 cm (0.433 m/s)

The initial position and velocity of a block moving in SHM with period T=0.25 s are x(0) = 5.0 cm and v(0) = 218 cm/s. Calculate the angular velocity w. (25.1 rad/s) Calculate the amplitude (10.0 cm) Calculate the phase constant (in radians) from the initial conditions. (p/6 rad)

Forces on a Spring Extreme Position (Amplitude) Equilibrium position Force at maximum Velocity = 0 Equilibrium position Force = 0 Velocity at maximum

The Equation of Motion F = ma F = -kx ma = -kx a = -kx also a = dv = d2x m dt dt2 d2x = -kx dt2 m

d2x + kx = 0 Equation of Motion dt2 m x(t) = A cos(wt + j) dx/dt = -wA sin(wt + j) d2x/dt2 = -w2A cos(wt + j) -w2A cos(wt + j) + k A cos(wt + j) = 0 m

Energy and Springs KE = ½ mv2 PE = ½ kx2 Maximum PE = ½ kA2 Law of conservation of Energy ½ kA2 = ½ mv2+ ½ kx2 Also w = (k/m)½

All PE All KE Some KE and Some PE

A 0.50 kg mass is connected to a light spring with a spring constant of 20 N/m. Calculate the total energy if the amplitude is 3.0 cm. (9 X 10-3 J) Calculate the maximum speed of the mass (0.19 m/s) Calculate the potential energy and kinetic energy at x = 2.0 cm (U = 4 X 10-3 J, K = 5 X 10-3 J) At what position is the speed 0.10 m/s? (+ 2.6 cm)

A spring stretches 0.150 m when a 0.300 kg mass is suspended from it. Find the spring constant. (19.6 N/m) The spring is now stretched an additional 0.100 m and allowed to oscillate (diagram c). What is the maximum velocity? (0.808 m/s) Calculate the velocity at x = 0.0500 m (0.700 m/s) What is the maximum acceleration? (6.53 m/s2)

A 500 g block is pulled 20 cm on a spring and released A 500 g block is pulled 20 cm on a spring and released. It has a period of 0.800 s . At what positions is the block’s speed 1.0 m/s? (Hint: use w = \/k/m )

Trigonometry and SHM Ball rotates on a table Looks like a spring from the side One rev(diameter) = 2pA T = 2p m w = \/k/m k f = 1 T

Period depends only on mass and spring constant Amplitude does not affect period vmax = 2pAf or vmax = 2pA T w = \/k/m

What is the period and frequency of a 1400 kg car whose shocks have a k of 6.5 X 104 N/m after it hits a bump? w = k = 6.81 rad/s m w = 2pf ANS: 1.09 Hz

An insect (m=0.30 g) is caught in a spiderweb that vibrates at 15 Hz. What is the spring constant of the web? (2.7 N/m) What would be the frequency for a lighter insect, 0.10 g? Would it be higher or lower? (26 Hz)

At t = 0, a 5000 g block is moving to the right and is at 15 cm At t = 0, a 5000 g block is moving to the right and is at 15 cm. Its maximum displacement is 25 cm at 0.30 s. Calculate the phase constant Calculate the angular velocity Calculate the time and velocity when the mass is at x = 20 cm Sketch a graph of the motion, including the phase constant and period

Vertical Motion of a Spring Gravity is ALWAYS acting on the spring and mass consistently Only need to use it to calculate the spring constant F = -ky (using y for vertical rather than x)

An 83 kg student hangs from a bungee cord with spring constant 270 N/m An 83 kg student hangs from a bungee cord with spring constant 270 N/m. He is pulled down to a position 5.0 m below the unstretched length of the bungee, then released. Calculate the equilibrium length of the bungee/student (3 m) Calculate the Amplitude (2 m) Calculate the position and velocity 2.0 s later. (1.8 m, -1.6 m/s)

The Pendulum Pendulums follow SHM only for small angles (<15o) The restoring force is at a maximum at the top of the swing. q Fr = restoring Force

Remember the circle (360o = 2p rad) q = x L Fr = mgsinq at small angles sinq = q Fr = mgq q L x q mg s

Fr = mgq Fr = mg s (Look’s like Hook’s Law F = -kx) L k = mg T = 2p m k T = 2p mL mg

T = 2p L g f = 1 = 1 g T 2p L The Period and Frequency of a pendulum depends only on its length

The Pendulum and the Equation of motion F = -mgsinq ma = -mgsinq a = -gsinq d2s = -gsinq dt2 d2s = -gq (small angle approximation)

d2s = -gs (q = s/L) dt2 L s = Acos(wt + f) d2s = -w2Acos(wt + f) dt2 -w2Acos(wt + f) = -g Acos(wt + f) L

Swings and the Pendulum To go fast, you need a high frequency Short length (tucking and extending your legs) f = 1 g 2p L decrease the denominator

Consider a grandfather clock with a 1.0 m long pendulum Calculate the period of? (2.0 s) Estimate the length of the pendulum of a grandfather clock that ticks once per second (T = 1.0 s). (0.25 m)

A 300 g mass on a 30 cm long string swings at a speed of 0 A 300 g mass on a 30 cm long string swings at a speed of 0.25 m/s at its lowest point. Calculate the period Calculate the angular velocity Calculate the maximum angle that the pendulum reaches (HINT: Use the triangle and the small angle approximation).

Physical Pendulum Center of mass is in the middle (sinq q) t = -Mglsinq t = -Mglq (small angle approximation)

= Ia a = d2q dt2 = I d2q = -Mglq I d2q = -Mglq d2q + Mglq = 0 dt2 I

d2q + Mglq = 0 dt2 I d2x + k x = 0 dt2 m

A student swings his leg which is 0. 90 m long A student swings his leg which is 0.90 m long. Assume the center of mass is halfway down the leg. Write the equation for the moment of inertia of the leg (I = ML2/3) Substitute this into the period formula to calculate the period (1.6 s) Calculate the frequency (0.64 Hz)

A nonuniform 1.0 kg physical pendulum has a center of mass 42 cm from the pivot. It oscillates with a period of 1.6 s. Calculate the moment of inertia (0.27 kg m2) Using the parallel axis theorem, calculate the period if the pendulum were swung at the center of mass. (0.09 kg m2) I = Icm + Md2

A Christmas ball has a radius R and a moment of inertia of 5/3MR2 when hung by a hook. The ball is given a slight tap and rocks back and forth. Derive the formula for the period of oscillation. Assume the center of mass is at the center of the ball. Insert a reasonable radius into your equation to estimate the period.

Damped Harmonic Motion Most SHM systems slowly stop For car shocks, a fluid “dampens” the motion

Resonance: Forced Vibrations Can manually move a spring (sitting on a car and bouncing it) Natural or Resonant frequency (fo) When the driving frequency f = fo, maximum amplitude results Tacoma Narrows Bridge 1989 freeway collapse Shattering a glass by singing

Wave Medium Mechanical Waves Electromagnetic Waves Require a medium Water waves Sound waves Medium moves up and down but wave moves sideways Electromagnetic Waves Do not require a medium EM waves can travel through the vacuum of space

Parts of a wave Crest Trough Amplitude Wavelength Frequency (cycles/s or Hertz (Hz)) Velocity v = lf

How many complete waves are shown above? What is the wavelength of light shown above?