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Mechanical Properties Of Fluids

Question
CBSEENPH11019354

What is damped oscillation. Write the differential equation for damped oscillations. Obtain an expression for the displacement in the case of damped oscillatory motion. Discuss how the amplitude of oscillation changes with time?

Solution
When an oscillator is oscillating in a resistive medium, the energy of oscillation is consequently decreasing. For such an oscillator, the amplitude decreases with time and ultimately the oscillations die out.
This type of oscillator is known as a damped oscillator.
                         

Consider a loaded spring oscillating in the vertical direction in a resistive media.
Let m be the mass of load and k be the spring constant.
The load is displaced from the equilibrium position. Let at any instant, y be the displacement from equilibrium position and v is the velocity of the load.
The different forces acting on load are:

(i) Restoring force which is proportional to displacement and directed towards equilibrium position.
i.e.,    F1= – ky

(ii) Resistive force of medium which is proportional to velocity and opposite to the direction of velocity.
i.e.,     F2 = –bv
The net force acting on the load is,

F = Fx1 + F
   = – ky –bv
Therefore the equation of motion of load is, 
space space space space space space space space space space space space space space space space space straight m fraction numerator straight d squared straight y over denominator dt squared space end fraction equals negative ky minus straight b dy over dt

space rightwards double arrow space space space space space space space space space space straight m fraction numerator straight d squared straight y over denominator dt squared space end fraction plus straight b dy over dt plus ky equals 0
rightwards double arrow space space space space space space fraction numerator straight d squared straight y over denominator dt squared end fraction plus straight b over straight m dy over dt plus straight k over straight m straight y equals 0
This is the required differential equation of motion of damped oscillations.
The solution of the equation is,
straight y equals straight A subscript 0 straight e to the power of fraction numerator straight b over denominator 2 straight m end fraction straight i end exponent cos open square brackets open parentheses square root of straight k over straight m minus fraction numerator straight b squared over denominator 4 straight m squared end fraction end root close parentheses straight r plus straight ϕ close square brackets 
Comparing it with space space straight y equals Acos left parenthesis ωt plus straight ϕ right parenthesis, we get,
straight A equals straight A subscript 0 straight e to the power of fraction numerator straight h over denominator 2 straight m end fraction straight i end exponent                                      .....(1)
space space space space straight omega equals square root of straight k over straight m minus fraction numerator straight b squared over denominator 4 straight m squared end fraction end root equals square root of straight omega subscript 0 squared minus fraction numerator straight b squared over denominator 4 straight m squared end fraction end root space space space...... left parenthesis 2 right parenthesis
Equation (1) gives the amplitude of oscillation, which decreases exponentially with time.

Equation (2) gives the frequency of oscillation which is less than the natural frequency of oscillation ω0