Grade 11

Grade 11Waves and oscillationsSimple Harmonic Motion


Damped and forced oscillations


Introduction

Oscillations are an integral part of our daily lives and nature. From the way a clock pendulum swings to the vibration of our vocal cords while speaking. Understanding oscillations can provide us with information about various natural phenomena and technological applications. Simple Harmonic Motion (SHM) has two types of oscillations, damped oscillations and forced oscillations. In this lesson, we will explain these concepts in a simple and easy to understand manner.

Understanding Simple Harmonic Motion (SHM)

Before diving into damped and forced oscillations, let us refresh our understanding about simple harmonic motion (SHM). SHM is a type of oscillatory motion where the restoring force is directly proportional to the displacement from the mean position and acts in the opposite direction to the displacement. It can be mathematically expressed as:

F = -kx

Here, F is the restoring force, k is the spring constant, and x is the displacement from the mean position. The negative sign indicates that the force is in the opposite direction of the displacement.

Let's look at an example of a simple harmonic oscillator:


    
    
    
    Average position
    ↔ F
    ↔ X

    

In the visualization, the blue circle represents an oscillating object that moves back and forth about a mean position. The arrows represent vector quantities: displacement x in green and force F in red.

Damped oscillation

In the ideal world, the oscillations would continue forever. However, in real life, oscillating systems are subject to forces such as friction and air resistance, which cause them to lose energy over time. This type of motion is called damped oscillation.

Types of damping

There are different degrees of damping depending on the medium and forces:

  • Hypodamped: The system oscillates with a gradually decreasing amplitude.
  • Critically damped: The system returns to the equilibrium position quickly without oscillation.
  • Overdamped: The system returns to equilibrium slowly, without oscillation.

The mathematical expression for damped oscillations is:

x(t) = A e^(-bt/2m) cos(ωt + φ)

Here, A is the initial amplitude, b is the damping coefficient, m is the mass, t is the time, ω is the angular frequency, and φ is the phase angle.

Let us imagine a slightly damped oscillation:


    
    
    
    Time
    Dimensions

    

In the visualization above, the red curve shows how the amplitude decreases with time in an underdamped system.

Practical example of damped oscillations

Consider the car's suspension system. The springs and shock absorbers in the suspension are designed to reduce vibrations caused by bumps and potholes in the road, making the ride more comfortable.

Forced oscillation

In forced oscillation, an external force continuously acts on the system, giving it energy. The system oscillates under the influence of an external periodic force.

F(t) = F_0 cos(ω_d t)

Here, F(t) is the external periodic force, F_0 is the amplitude of the force, and ω_d is the driving angular frequency.

Resonance in forced oscillation

Resonance is an important concept related to forced oscillation, which occurs when the frequency of the external force matches the natural frequency of the system. This can cause a significant increase in amplitude, which can sometimes lead to structural failures such as bridges collapsing due to marching soldiers or when a singer breaks a glass by singing at its natural frequency.

Practical example of forced oscillation

A simple example of forced oscillation is pushing a swing at regular intervals. The external force applied by the person pushing keeps the swing moving.

Let us imagine the resonance phenomenon:


    
    
    
    Time
    Dimensions

    

The blue curve shows the increase in amplitude due to resonance.

Conclusion

Understanding damped and forced oscillations opens the door to exploring complex physical systems. This knowledge helps in designing technological devices and understanding natural systems. By understanding these fundamental concepts, you have taken the first step towards further exploration in physics.


Grade 11 → 5.1.3


U
username
0%
completed in Grade 11


Comments