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As we know that the equation of motion of damped oscillation is
given by the second order
differential equation is
( d ² x / dt ² ) + 2 β ( d x / dt ) + ω₀ ² x = 0
where -
β = b / ( 2m ) [ b = damping constant, m = mass]
ω₀ = √ [ k / m ]
k = spring constant
Now assume small damping => underdamped oscillation -
The corresponding solution of the differential equation is given by -
x ( t ) = A₀ exp [ - β t ] cos ( ω₁ t – δ ) = A cos ( ω₁ t – δ )
Where -
A = A₀ exp [ - β t ]
ω₁ = √ [ ω₀ ² - β ² ]
δ = phase constant
Since the exponential function gives numbers only, the unit of β
must be 1 / s
β = b / ( 2 m )
=> b = 2 m β
(Therefore, unit of the damping constant (coefficient) b should be ( kg / s ), not N/m = unit for spring constant)
Given that,
b = 2 kg / s, A₀ = 20 cm, A = 15 cm and t = 10 s
So,
A / A₀ = 15 cm / 20 cm = 0.75 = exp [ - β ( 10 s ) ]
Take the logarithmic function -
ln ( 0.75 ) = - 0.287682 = - β ( 10 s )
=> β = 0.287682 / ( 10 s ) = 0.0287682 s ⁻ ¹
Now, β = b / ( 2 m )
=> m = b / [ 2 β ] = [ 2 kg / s ] / [ 2 ( 0.0287682 s ⁻ ¹ ) ] = 34.8 kg
Hence the oscillating mass = 34.8 kg.
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