Chapter 13 SHM? WOD are underlined. Remember Hooke’s Law F = - k Δx New Symbol: “k” Spring constant. “Stiffness” of the spring. Depends on each spring’s.

Slides:



Advertisements
Similar presentations
Physics January
Advertisements

Kinematics of simple harmonic motion (SHM)
Chapter 5 Kinetic Energy
SHM -1.
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.
Copyright © 2009 Pearson Education, Inc. Lecture 1 – Waves & Sound a) Simple Harmonic Motion (SHM)
Simple Harmonic Motion & Elasticity
Chapter 15 Oscillatory Motion.
Simple Harmonic Motion
Physics 6B Oscillations Prepared by Vince Zaccone
Chapter 13 Vibrations and Waves.
Chapter 13 Vibrations and Waves. Hooke’s Law F s = - k x F s is the spring force k is the spring constant It is a measure of the stiffness of the spring.
Springs and Pendulums.
Simple Harmonic Motion
Simple Harmonic Motion
Vibrations and Waves AP Physics Lecture Notes m Vibrations and Waves.
Simple Harmonic Motion
Simple Harmonic Motion Chapter 12 Section 1. Periodic Motion A repeated motion is what describes Periodic Motion Examples:  Swinging on a playground.
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 m Physics 2053 Lecture Notes Vibrations and Waves.
Periodic Motion. Definition of Terms Periodic Motion: Motion that repeats itself in a regular pattern. Periodic Motion: Motion that repeats itself in.
Oscillations - SHM. Oscillations In general an oscillation is simply aback and forth motion Since the motion repeats itself, it is called periodic We.
Oscillatory Motion Serway & Jewett (Chapter 15).
Copyright © 2009 Pearson Education, Inc. Chapter 14 Oscillations.
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.
Hooke’s Law F s = - k x F s is the spring force k is the spring constant It is a measure of the stiffness of the spring A large k indicates a stiff spring.
Introduction to Simple Harmonic Motion Unit 12, Presentation 1.
Chapter 15: Oscillations
L 20 – Vibration, Waves and Sound -1 Resonance Tacoma Narrows Bridge Collapse The pendulum springs harmonic motion mechanical waves sound waves musical.
Physics 1B03summer - Lecture 7 HOMEWORK QUESTION Please do this question and hand it by Tuesday after the reading week, in class: A 50kg child slides down.
Periodic Motion What is periodic motion?
Simple Harmonic Motion
SIMPLE HARMONIC MOTION. STARTER MAKE A LIST OF OBJECTS THAT EXPERIENCE VIBRATIONS:
Periodic Motions.
Chapter 11: Harmonic Motion
Chapter 12 Vibrations and Waves. Periodic Motion Any repeated motion Examples?
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.
Vibrations and Waves Chapter 11. Most object oscillate (vibrate) because solids are elastic and they will vibrate when given an impulse Tuning forks,
Chapter 5.2 Hooke’s Law WOD are underlined. Question What is the net force on this mass?
VibrationsandWaves. Ch. 14 examines wave motion and the oscillating, vibrating motion that creates them. This oscillating motion is known as periodic.
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.
Chapter 16 Vibrations Motion. Vibrations/Oscillations Object at the end of a spring Object at the end of a spring Tuning fork Tuning fork Pendulum Pendulum.
Physics 201: Lecture 28, Pg 1 Lecture 28 Goals Goals  Describe oscillatory motion  Use oscillatory graphs  Define the phase constant  Employ energy.
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.
Any regular vibrations or oscillations that repeat the same movement on either side of the equilibrium position and are a result of a restoring force Simple.
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.
Simple Harmonic Motion (SHM). Simple Harmonic Motion – Vibration about an equilibrium position in which a restoring force is proportional to displacement.
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.
Simple Harmonic Motion Wenny Maulina Simple harmonic motion  Simple harmonic motion (SHM) Solution: What is SHM? A simple harmonic motion is the motion.
Chapter 10 Waves and Vibrations Simple Harmonic Motion SHM.
Simple Harmonic Motion (SHM)
Chapter 14 – Vibrations and Waves. Every swing follows the same path This action is an example of vibrational motion vibrational motion - mechanical oscillations.
Simple Harmonic Motion
Harmonic Motion AP Physics C.
Unit D: Oscillatory Motion & Mechanical Waves
Simple Harmonic Motion
Simple Harmonic Motion
Oscillations An Introduction.
Unit 4: Oscillatory Motion and Mechanical Waves
PHYS 1441 – Section 004 Lecture #22
Simple Harmonic Motion
Simple Harmonic Motion (SHM)
Vibrations and Waves.
Simple Harmonic Motion and Wave Interactions
Presentation transcript:

Chapter 13 SHM? WOD are underlined

Remember Hooke’s Law F = - k Δx New Symbol: “k” Spring constant. “Stiffness” of the spring. Depends on each spring’s dimensions and material. In N/m

Question If I let go, what will happen to the mass? Then what? Then what?

Simple Harmonic Motion Repeating up and down motion, (like cos wave.) (Draw a picture.) Motion that occurs when the net force obeys Hooke’s Law The force is proportional to the displacement and always directed toward the equilibrium position Show Example with Spring The motion of a spring mass system is an example of Simple Harmonic Motion Are springs the only type of SHM?

Simple Harmonic Motion The motion of a spring mass system is an example of Simple Harmonic Motion Are springs the only type of SHM: No, Jump Rope, Sound Waves, Pendulum, Swing, up and down motion of an engine piston

Motion of the Spring-Mass System Initially, Δx is negative and the spring pulls it up. The object’s inertia causes it to overshoot the equilibrium position. Δx is positive now and the spring pushes it down. Again it will over shoot equilibrium.

Δx, v and a versus t graphs What type of curve is this? For Calculus, Derivative of sin is what? What happens if you bump the spring?

Δx, v and a

All three look like sinusoidal curves. V is shifted backwards from Δx a is shifted backwardwards from v.

Acceleration of an Object in Simple Harmonic Motion Remember F = - k x & F = ma Set them equal to each other: - k x = ma Solve for a: a = -kΔx / m The acceleration is a function of position Acceleration is not constant. So non-inertial frame of reference. So, the kinematic equations are not valid here.

Amplitude: New Symbol “A” Amplitude, A The amplitude is the maximum position of the object relative to the equilibrium position: (Max Height) In the absence of friction, an object in simple harmonic motion will oscillate between the positions x = ±A What friction is there?

Amplitude: New Symbol “A” Amplitude, A The amplitude is the maximum position of the object relative to the equilibrium position: (Max Height) In the absence of friction, an object in simple harmonic motion will oscillate between the positions x = ±A What friction is there? Air Resistance, Molecular Motion in Spring

Period: New Symbol “T” Period: T uppercase T stands for “period.” Amount of time for the oscillator to go through 1 complete cycle. (Time for 1 up and 1 down.) Often measured from Max to Max, But can be measured from start to start, etc. Measured in seconds.

Frequency: Another new symbol “ƒ” “ƒ” is for frequency. It is the number of cycles an oscillator goes through in one second. It is measured in 1/seconds 1/seconds => New unit “Hertz” or Hz. What is the frequency of revolutions of a new M16 bullet?

Frequency: Another new symbol “ƒ” “ƒ” is for frequency. It is the number of cycles an oscillator goes through in one second. It is measured in 1/seconds 1/seconds => New unit “Hertz” What is the frequency of revolutions of a new M16 bullet? Ans:5100 Hz or Rev per Second.

Period and Frequency The period, T, is the time per cycle. The frequency, ƒ, is cycles per time. Frequency is the reciprocal of the period ƒ = 1 / T

Quick Recap(Pic for WOD) A – maximum distance from rest postion. T – time for one complete cycle ƒ = 1 / T

In the table, label each +, -, or 0.

Question When you compress (or stretch) a spring, you have to do work on it. You apply a force over some distance. Can you get that energy back?

Elastic Potential Energy (Energy stored in a spring. Ability of a spring to do work.) Work done on a spring is stored as potential energy. The potential energy of the spring can be transformed into kinetic energy of the mass on the end.

Energy Transformations Suppose a block is moving on a frictionless surface. Before it hits the spring, the total mechanical energy of the system is the kinetic energy of the block. What happens next?

Energy Transformations, 2 The spring is partially compressed. The mass has slowed down. Σ ME = K.E. + P.E.

Energy Transformations, 3 The spring is now fully compressed The block momentarily stops The total mechanical energy is stored as elastic potential energy of the spring

At all times, total Mechanical Energy is constant = KE + PE (Put into notes) Equations for SHM Energy: KE = ½ mv 2 PE = ½ kx 2

Keep in mind. It takes the same energy to stretch a spring as compress it. PE = ½ kx 2 Is the same as = ½ k(-x) 2 So PE is same at Max or Min A.

Back to Period and Frequency Period Frequency What variable is not in these equations?

Back to Period and Frequency Period Frequency What variable is not in these equations? A. T and f do not depend on Amplitude.

Problem A 1 kg block is dropped from a height of 1 m onto a spring with k = 55 N/m. How far will the spring compress?

Problem (revisited) A 1 kg block is dropped from a height of 1 m onto a spring with k = 55 N/m. What will it’s frequency and period of oscillation be?

Problem A 1 kg block is dropped from a height of 1 m onto a spring with k = 55 N/m. Q1. How far will the spring compress? Q2. What will it’s frequency and period of oscillation be?