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Question: A mass of 5 kg is suspended on a spring of stiffness 4000 N/m. The system is fitted with a damper wi...

A mass of 5 kg is suspended on a spring of stiffness 4000 N/m. The system is fitted with a damper with a damping ratio of 0.2. The mass is pulled down 50 mm and released. Calculate the displacement after 0.3 sec:
A.)4.07mm
B.)4.70mm
C.)7.40mm
D.)7.04mm

Explanation

Solution

Hint: We have to find the natural frequency fn{f_n} and angular velocity ωn{\omega _n} of the Simple harmonic motion. We also have to calculate the frequency ff and angular velocity ω\omega considering damping. We have to use the damping ratio given δ\delta .Substituting this general form of the equation of an under damped simple harmonic wave we find the displacement.

Formula used:
ω=2πf\omega = 2\pi f ω\omega is the angular velocity ff and is the frequency.
fn=12πkM{f_n} = \dfrac{1}{{2\pi }}\sqrt {\dfrac{k}{M}} , here fn{f_n} denotes the natural frequency kk denotes the spring constant /stiffness of the spring and MM denotes the mass.
f=fn1δ2f = {f_n}\sqrt {1 - {\delta ^2}} Where ff is the frequency, fn{f_n} denotes the natural frequency and δ\delta denotes the damping ratio.
ω=ωn1δ2\omega = {\omega _n}\sqrt {1 - {\delta ^2}} Here ω\omega is the angular velocity, ωn{\omega _n} denotes the natural angular velocity and δ\delta denotes the damping ratio.
x=Ceδωntcosωtx = C{e^{ - \delta {\omega _n}t}}\cos \omega t, here xx shows the displacement, CC denotes the initial /maximum displacement, δ\delta denotes the damping ratio,ω\omega is the angular velocity, ωn{\omega _n} denotes the natural angular velocity and tt shows the time.

Complete step by step answer:
In order to calculate the frequency of the wave we use the equation fn=12πkM{f_n} = \dfrac{1}{{2\pi }}\sqrt {\dfrac{k}{M}}

It is given that k=4000N/mk = 4000N/m and M=5KgM = 5Kg.We get
fn=12π40005{f_n} = \dfrac{1}{{2\pi }}\sqrt {\dfrac{{4000}}{5}}
fn=12π800{f_n} = \dfrac{1}{{2\pi }}\sqrt {800}
fn=4.5Hz{f_n} = 4.5Hz

Using ω=2πf\omega = 2\pi f we get ωn=9π{\omega _n} = 9\pi
ωn=28.28rad/s{\omega _n} = 28.28rad/s
The frequency and angular velocity can be found out by using f=fn1δ2f = {f_n}\sqrt {1 - {\delta ^2}} and ω=ωn1δ2\omega = {\omega _n}\sqrt {1 - {\delta ^2}}

Given that δ=0.2\delta = 0.2.Substituting

f=4.51(0.2)2f = 4.5\sqrt {1 - {{(0.2)}^2}}
f=4.41Hzf = 4.41Hz
ω=28.281(0.2)2\omega = 28.28\sqrt {1 - {{(0.2)}^2}}
ω=27.71rad/s\omega = 27.71rad/s

The initial / maximum displacement of this wave is 50mm{50mm} downwards .Therefore C=50mmC = - 50mm
The time for which we have to find the displacement is given t=0.3st = 0.3s
Using all the found values in h\the general form x=Ceδωntcosωtx = C{e^{ - \delta {\omega _n}t}}\cos \omega t we get,

x=50e0.2×28.28×0.3cos(27.71×0.3)x = - 50{e^{ - 0.2 \times 28.28 \times 0.3}}\cos (27.71 \times 0.3)
x=50e1.6968cos(8.313)x = - 50{e^{ - 1.6968}}\cos (8.313)
x=50×0.183×0.443x = - 50 \times 0.183 \times - 0.443
x4.07mmx \approx 4.07mm

Note: The angle taken here is in the units of radians. Based on the value of damping ratio and the natural angular velocity of the wave damping can be of basically three types. If γ2>4ω02{\gamma ^2} > 4{\omega _0}^2 it is said to be over damped. If γ2=4ω02{\gamma ^2} = 4{\omega _0}^2it is called critically damped and when γ2<4ω02{\gamma ^2} < 4{\omega _0}^2 it is under damped. (Here γ\gamma is the damping ratio).