Theory of Machines Miscellaneous
- A rod of length 1 m is sliding in a corner as shown in figure. At an instant when the rod makes an angle of 60 degrees with the horizontal plane., the velocity of point A on the rod is 1m/ s. The angular velocity of the rod at this instant is
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VA = O'A × ω
1 = 1 cos 60° × ω
ω = 2 rad/sCorrect Option: A
VA = O'A × ω
1 = 1 cos 60° × ω
ω = 2 rad/s
- Figure shows a quick return mechanism. The cranks OA rotates clockwise uniformly. OA = 2 cm, OO' = 4 cm. The ratio of time for forward motion to that for return motion is
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Ratio of time of forward motion to return motion
= 180 + 2α = 180 + 60 = 240 = 2 180 − 2α 180 − 60 120
(Given OD = 2 cm, OO ' = 4 cm, sin α = 2/4 = 0.5 ⇒ α = 30°)Correct Option: B
Ratio of time of forward motion to return motion
= 180 + 2α = 180 + 60 = 240 = 2 180 − 2α 180 − 60 120
(Given OD = 2 cm, OO ' = 4 cm, sin α = 2/4 = 0.5 ⇒ α = 30°)
- A slender uniform rigid bar of mass m is hinged at O and supported by two spr i ngs, wit h stiffnesses 3k and k, and a damper with damping coefficient c, as shown in the figure. For the system to be critically damped, t he ratio c / √km should be
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I0 = m
L2+ m L 2 12 4 = mL2 + mL2 = 7 mL2 12 16 48
Torque about hinge ‘O’= 7mL2 θ̇̇ + 3k. L2 θ + k. 9L2 θ + C. L2 θ̇ = 0 48 16 16 16 ⇒ 7mL2 θ̇̇ + 12kL2 θ + CL2 θ̇ = 0 48 16 16 2ξωn = C × 48 = 3C 16 × 7 m 7m ⇒ 2√km = 3 × √7 × C 7 6 C = 4√7 √km Correct Option: D
I0 = m
L2+ m L 2 12 4 = mL2 + mL2 = 7 mL2 12 16 48
Torque about hinge ‘O’= 7mL2 θ̇̇ + 3k. L2 θ + k. 9L2 θ + C. L2 θ̇ = 0 48 16 16 16 ⇒ 7mL2 θ̇̇ + 12kL2 θ + CL2 θ̇ = 0 48 16 16 2ξωn = C × 48 = 3C 16 × 7 m 7m ⇒ 2√km = 3 × √7 × C 7 6 C = 4√7 √km
- A uniform thin disk of mass 1 kg and radius 0.1 m is kept on a surface as shown in the figure. The spring of stiffness k1 = 400 N/m is connected to the disk center A and another spring of stiffness k2 = 100 N/m is connected at point B just above point A on the circumference of the disk. Initially, both the springs are unstretched. A assume pure rolling of the disk. For small disturbance from the equilibrium, the natural frequency of vibration of the system is _____rad/ s (round off to one decimal place).
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Given, Disc mass m = 1 kg, R = 0.1 m
K1 = 400 N/m, K2 = 100 N/m
By assuming pure rolling of the disc, Mc = 0 at I.C. at point (C)
Icθ̇̇ + K2(2R)θ × 2R + K1Rθ × R = 0Ic = Idisc + mR2 = mR2 + mR2 2 = 3 mR2 = 3 × 0.12 = 1.5 × 10-2 2 2
⇒ ωn = √533.3rad / sec
ωn = 23.094 rad / sec
ωn = 23.1 rad / secCorrect Option: A
Given, Disc mass m = 1 kg, R = 0.1 m
K1 = 400 N/m, K2 = 100 N/m
By assuming pure rolling of the disc, Mc = 0 at I.C. at point (C)
Icθ̇̇ + K2(2R)θ × 2R + K1Rθ × R = 0Ic = Idisc + mR2 = mR2 + mR2 2 = 3 mR2 = 3 × 0.12 = 1.5 × 10-2 2 2
⇒ ωn = √533.3rad / sec
ωn = 23.094 rad / sec
ωn = 23.1 rad / sec
- The natural frequencies corresponding t o the spring-mass system I and II are ωI and ωII, respectively.
The ratio ωⅠ is ωⅡ
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Now , 1 = 1 + 1 (For series connection) {Keq} K1 K2 ⇒ Keq1 = K1K2 = K K1 + K2 2
(Keq)2 = K1 + K2 = K (For parallel connection)
Correct Option: D
Now , 1 = 1 + 1 (For series connection) {Keq} K1 K2 ⇒ Keq1 = K1K2 = K K1 + K2 2
(Keq)2 = K1 + K2 = K (For parallel connection)