The following is the equation of motion for forced damped vibration of a mass-damper system: mx + cx + kx = F₁ sin wt The magnification factor variation with respect to the frequency ratio is given in Figure Q5 for various damping ratio values. If it is known that for the system examined the damping ratio is 0.3 and the magnification factor takes the value 0.8, then how the vibration amplitude can be further reduced by only altering the mass, damping coefficient and stiffness coefficient? Amplitude ratio: M = 2.8 2.4 2.0 1.6 1.2 1.0 0.8 0.4 0 = 0.1 = 0.3 = 0.4 <=0.5._. = 1.5 -= 2.0 5.0 0.4 0.8 1.2 1.6 2.0 1.0 Frequency ratio: r = 3.0 2.4 2.8 3.2 @ Wn

Elements Of Electromagnetics
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The following is the equation of motion for forced damped vibration of a
mass-damper system:
mx + cx + kx
Fo sin wt
The magnification factor variation with respect to the frequency ratio is
given in Figure Q5 for various damping ratio values. If it is known that for
the system examined the damping ratio is 0.3 and the magnification
factor takes the value 0.8, then how the vibration amplitude can be
further reduced by only altering the mass, damping coefficient and
stiffness coefficient?
4/1055
Amplitude ratio: M =
2.8
2.4
2.0
1.6
1.2
1.0
0.8
0.4
0
= 5.0
0.4
= 0.1
= 0.3
X = 0.4
-=0.5.--
= 1.5
= 2.0
0.8 1.2 1.6 2.0
1.0
Frequency ratio: r =
= 3.0
2.4 2.8 3.2
W
Wn
Transcribed Image Text:The following is the equation of motion for forced damped vibration of a mass-damper system: mx + cx + kx Fo sin wt The magnification factor variation with respect to the frequency ratio is given in Figure Q5 for various damping ratio values. If it is known that for the system examined the damping ratio is 0.3 and the magnification factor takes the value 0.8, then how the vibration amplitude can be further reduced by only altering the mass, damping coefficient and stiffness coefficient? 4/1055 Amplitude ratio: M = 2.8 2.4 2.0 1.6 1.2 1.0 0.8 0.4 0 = 5.0 0.4 = 0.1 = 0.3 X = 0.4 -=0.5.-- = 1.5 = 2.0 0.8 1.2 1.6 2.0 1.0 Frequency ratio: r = = 3.0 2.4 2.8 3.2 W Wn
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