Oscillations are repeating vibrations of a quantity around its equilibrium position.
The term originates from the Latin verb meaning "to swing."
A restoring force pushes or pulls an object back to its central point after displacement, causing it to oscillate around this equilibrium.
Periodic Motion
Periodic motion is motion repeated in equal time intervals.
Period (T): Time for one complete repetition or cycle.
Frequency (f): Number of periods per unit time.
Examples:
Rocking chair
Bouncing ball
Vibrating tuning fork
Swing in motion
Spring Oscillator
A spring oscillator (spring-mass system) is a mechanical system where a mass attached to a spring oscillates around an equilibrium point.
This oscillation is a form of simple harmonic motion.
The spring exerts a restoring force proportional to the displacement from equilibrium.
Simple Pendulum
A simple pendulum consists of a mass (pendulum bob) suspended from a fixed point by a string.
It exemplifies periodic motion with a regular back-and-forth swing.
Key Parameters:
T: Period (time for one complete swing, in seconds).
f: Frequency (number of complete swings per second, in Hertz).
L: Length (pendulum length from pivot to center of mass, in meters).
g: Acceleration due to gravity (approximately 9.8m/s2 on Earth).
Physical Pendulum
A physical pendulum is a rigid body oscillating about a fixed horizontal axis under gravity's influence.
It accounts for the object's size and mass distribution, unlike the simple pendulum.
Key Parameters:
T: Period (time for one complete swing, in seconds).
f: Frequency (number of complete swings per second, in Hertz).
I: Moment of inertia of the object about the pivot point (in kg⋅m2).
m: Mass of the object (in kg).
g: Acceleration due to gravity (approximately 9.8m/s2 on Earth).
d: Distance from the pivot point to the center of mass (in meters).
Difference Between Simple and Physical Pendulum
Simple Pendulum:
Mass concentrated at one point (the bob).
Motion is easily predictable.
Physical Pendulum:
A whole object swings on a pivot.
Mass is spread out, affecting the swing based on shape and weight distribution.
Frequency and Period of Objects in Periodic Motion
Period (T): Time to complete one full cycle (in seconds).
Frequency (f): Number of complete cycles per second (in Hertz).
Spring Oscillator Parameters
T: Period (time for one complete oscillation, in seconds).
f: Frequency (number of complete oscillations per second, in Hertz).
m: Mass of the object attached to the spring (in kg).
k: Spring constant (stiffness of the spring, in N/m).
Oscillation Explained
Oscillation is a repetitive motion around a central value or equilibrium point, typically occurring at regular intervals.
Examples:
Swinging pendulum (gravity restores equilibrium).
Vibrating guitar strings (producing sound through repeated motion).
Simple Harmonic Motion (SHM)
Simple Harmonic Motion (SHM) is a special oscillation where the restoring force is: Directly proportional to the displacement from the equilibrium position. Always directed toward the equilibrium position.
The farther the object moves from the center, the stronger the restoring force.
SHM Examples
Playground swing (gravity acts as the restoring force).
Metronome (gravity restores the center position).
Conditions Necessary for SHM
Restoring Force Proportional to Displacement: The force pulling back increases with distance from equilibrium.
Restoring Force Acts in the Opposite Direction: The force always points toward equilibrium.
Minimal Damping: Ideally, no energy loss, so the motion continues without fading.
Stable Equilibrium: The object returns to its original position when slightly disturbed.
SHM Graphs
Displacement, velocity, and acceleration graphs follow wave-like patterns, peaking at different times.
Displacement graph: distance from the center position.
Velocity graph: how fast it’s moving.
Acceleration graph: strength of the push or pull.
Equations of SHM
F=−kx
F=ma
−kx=mdt2d2x
x(t)=xmcos(ωt+ϕ)
v(t)=−ωxmsin(ωt+ϕ)
a(t)=−ω2xmcos(ωt+ϕ)
Hooke’s Law
Hooke's Law states that the strain of the material is proportional to the applied stress within the elastic limit of that material.
F=kx
F = Force
k = Spring Constant
x = Displacement from equilibrium
Force and Motion Relationship
F=ma=−kx
a=−mkx
Freeze-Frames
A freeze-frame is a snapshot of a moving system at one instant in time, showing positions, forces, and velocities as if motion is paused.
It helps analyze what's happening right at that moment without considering past or future motion.
Energy in SHM
Potential energy and velocity are zero at extreme points and greatest at x=0.
Kinetic energy and acceleration are zero at x = 0 and greatest at extreme points.
Displacement at Time T
x(t)=xmcos(ωt+ϕ)
x(t) = Displacement at time t
xm = Amplitude
ω = Angular frequency
t = Time
ϕ = Phase constant or phase angle
Angular Frequency
ω is the angular frequency of the motion.
The position x(t) returns to its initial value at the end of a period (T), i.e., at time T + T.
Velocity at Time T
The velocity varies in magnitude and direction.
It's momentarily zero at extreme points and maximum through the central point.
v(t)=dtdx(t)=−ωxmsin(ωt+ϕ)
Acceleration at Time X
The acceleration varies because the cosine function varies with time, between +1 and -1.
Equations for a Spring-Mass System Summary
Hooke's Law: F=−kx
Angular Frequency: ω=mk
Frequency: f=2πω=2π1mk
Period: T=f1=2πkm
Position: x=Acos(ωt+ϕ)
Velocity: v=−Aωsin(ωt+ϕ)
Acceleration: a=−Aω2cos(ωt+ϕ)
Damped and Forced Oscillation
Damped oscillations: Amplitude decreases over time due to energy loss.
Forced Oscillation: An oscillating system is driven by an external periodic force.
Types of Damping
Underdamped: Oscillations occur with gradually decreasing amplitude; the system oscillates multiple times before coming to rest.
Critically damped: The system returns to equilibrium as quickly as possible without oscillating.
Overdamped: The system returns to equilibrium slowly without oscillating; takes longer than critically damped systems.
Sample Problems
A block of mass m=680g is fastened to a spring with k=65N/m. The block is Pulled a distance x=11cm from its equilibrium position at x=0 on a frictionless surface and released from rest at t=0.
What is the angular frequency of the resulting motion?
What is the frequency of the motion?
What is the period of the motion?
A 2.00−kg block is placed on a frictionless surface. A spring with a force constant k=32.00N/m is attached to the block, and the opposite end of the spring is attached to a wall. The spring can be compressed or extended. The equilibrium position is marked as x=0.00m. Work is done on the block, pulling it out to x=+0.02m. The block is released from rest and oscillates between x=+0.02m and x=−0.02m. The period of the motion is 1.57s.
A 2kg mass is hung vertically from a spring, causing it to stretch by 0.1m. What is the spring constant (k) of the spring?
A 0.5kg mass is attached to a spring with a spring constant of 200N/m. Find the frequency and period of the resulting simple harmonic motion.
A mass-spring system oscillates with an amplitude of 0.3m and a spring constant of 50N/m. If the mass is 1kg, what is the maximum speed of the mass during oscillation?
A 0.25kg object is attached to a spring with a spring constant of 100N/m and displaced by 0.1m from equilibrium. What is the total mechanical energy of the system, assuming no damping?
A 1kg mass is hanging from a spring and set into vertical oscillation. The spring constant is 150N/m. How far does the mass move from the equilibrium position if its initial speed is 2m/s at equilibrium?
A particle undergoes simple harmonic motion with a maximum displacement (amplitude) of 0.2m and an angular velocity of 4rad/s. At time t=1.5s, calculate the following:
Instantaneous position
Instantaneous velocity
Instantaneous acceleration. Assume the motion starts from maximum displacement