What is the effect of damping in an oscillatory system? Differentiate between heavy and critical damping. Show that the displacement of a weakly damped oscillator is given by
x(t ) = a0 exp(−bt ) cos(ωd t − φ)
where symbols have their usual meanings.
Let us take a spring mass system with a natural frequency ω0.
m = mass of the body oscillating
Spring restoration force F = - k x , k = spring constant.
Damping force F_d = - b v , where b = damping factor.
x = displacement.
v = velocity of mass.
ωâ‚€ is the frequency of the spring mass when there is no damping. Only force is spring force.
so, m d² x / d t² = - k x has the solution:
x = A0 Sin (ωâ‚€ + Ф₀) --- (0)
and ωâ‚€ = √(k/m) or ω0² = k/m ---- (12)
===========================
net force acting on mass m is: F = - k x - b v --- (1)
The minus sign is because spring restoration force is opposite to displacement direction and the damping force is in the direction opposite to velocity.
m a = m d² x / d t² = - k x - b v
d² x /d t² = -k/m * x - b/m * dx/dt --- (2)
This is the equation of motion in the form of differential equation.
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