Have you ever swung on a playground? The swing begins to go forward and backward when we push it. The motion of the swing can be developed by giving it a series of pushes. If the person pushing the seat matches the timing of the swing as he applies the force, the swing's action has a greater amplitude and can therefore swing higher. This is the condition of resonance. Even a light push on the swing helps to sustain its amplitude due to the resonance. This happens as it has reached its natural frequency of oscillation. This coordinated motion is known as resonance. Let's understand the resonance in detail.
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Free oscillation occurs when a system oscillates at a frequency that is unique to its geometry and inertia, also referred to as its natural frequency. It is an ideal situation. In free oscillation, frequency, amplitude and the energy of oscillation remain constant. Motion of the spring block system in a non resisting medium is an example of free oscillation.
The forced oscillation is the oscillation that occurs when a body oscillates under the influence of an external periodic force. This external periodic force makes up for the energy which is lost because of the damping force. So the oscillation's amplitude remains constant. Oscillation of the swing when someone is pushing periodically is an example of forced oscillation.
In forced oscillation the external force is periodic in nature and has some periodic frequency. When the frequency of the external force is changed the amplitude of the oscillation also changes. When the frequency of the external force is equal to the natural frequency of the oscillator or the system, the amplitude of the oscillation increases. This condition is referred to as the resonance state and this frequency is referred to as the resonant frequency.
Now, let's see the resonance in a mathematical way.
Consider a spring-block system that performs free oscillation with a natural frequency and has a block of mass m and a spring of force constant k.
The block is moved away from its mean position. If the block's displacement at time t is x(t), then the spring's restoring force is,
A negative sign indicates that the force opposes displacement in the situation.
Now the system is placed in a damping medium of damping constant b as shown in figure.
If the velocity of the block at time t is v(t), then the damping force acting on the system is
An external periodic force is applied to a system whose frequency is and amplitude is which is given as
The net force on the block is
If the acceleration of the block at any time t is equal to a(t), then we can write
On Substitute and , we have
The above differential equation represents the motion of a block under the combined action of restoring force, damping force, and driving force. The motion of forced oscillation will be given by solving this differential equation.
Displacement of the particle of the forced oscillation motion is given by
Where, is the amplitude of motion and given as,
is the frequency of force, is the natural frequency of oscillation and t is time measured from the instant of force application and is the initial phase.
Now consider the following cases -
( ), then can be neglected. Hence the amplitude is given as ,
The amplitude will depend on the difference in square of frequencies.
Amplitude depends on the frequency of force.
Q. A block with a mass of is oscillating at a natural frequency of 20 rad/s. Driving force , is applied to it, where and . Find the amplitude of the oscillation.
As , so the amplitude of oscillation is given as
Q. A periodic force of maximum value 50 N is applied on a spring block system of mass 30 kg and spring constant 100 N/m. If the damping constant of the motion is 40 kg/s, find the amplitude of resonating oscillation.
A. Mass, m = 30 kg
Damping constant, b = 40 kg s−1
Spring constant, k = 100 N m−1
The natural frequency of the system
At resonance the frequency of external force will be equal to natural frequency
The amplitude of oscillation
Q. The amplitude of a forced oscillatory motion at resonance is 10 mm when it is placed in the medium of damping constant 0.5 kg/s. Find the amplitude of oscillation when it is placed in the medium of damping, constant 0.3 kg/s.
The amplitude of oscillation at resonance condition
Q.A spring of force constant 50 N m−1 is attached to the block of mass 500 gm. At what angular frequency of external force the system will start resonating?
A.GivenMass, m = 500 gm
Spring constant, k = 50 N m−1
At resonance the frequency of external force will be equal to the natural frequency of oscillation
Q1.How many types of resonance are there?
Answer: There are five types of resonance -they are Acoustic, Mechanical, Electrical, Optical, Orbital resonance.
Q2. What is a system's natural frequency?
Answer: The oscillation frequency of a system in the absence of any driving force or dampening is known as its natural frequency.
Q3.When the driving frequency is far from the natural frequency, what is the expression for the forced oscillator's amplitude?
Answer: When the driving frequency is far from the natural frequency the amplitude of the oscillation is given by
Where, force amplitude
mass of oscillator
Natural frequency of oscillator
frequency of external force
Q4.What happens to the oscillations' amplitude when the driving frequency approaches the oscillator's native frequency?
Answer: The oscillation's amplitude increases and the system is considered to be in resonance when the driving frequency approaches the oscillator's native frequency.
Q5.What is the effect of damping on amplitude of oscillation at resonance?
Answer: Amplitude is inversely proportional to the damping constant. So if damping increases, the amplitude of oscillation decreases, and if damping decreases, the amplitude of oscillation increases.