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Theory of Machine

Theory of Machine
In automobiles the power is transmitted from gear box to differential through

Bevel gear
Knuckle joint
Hooke's joint
Universal joint

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Theory of Machine
The equation of motion for a vibrating system with viscous damping is (d²x/dt²) + (c/m). (dx/dt) + (s/m). x = 0. If the roots of this equation are real, then the system will be

Without vibrations
Critically damped
Over-damped
Under damped

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Theory of Machine
When a ship travels in a sea, which of the effect is more dangerous

Pitching
All of these
Rolling
Steering

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Theory of Machine
A body of weight W is required to move up the rough inclined plane whose angle of inclination with the horizontal is α. The effort applied parallel to the plane is given by (where μ = tan φ = Coefficient of friction between the plane and the body)

P = W tan (α + φ)
P = W tan α
P = W (sin α + μ cos α)
P = W (cos α + μ sin α)

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Theory of Machine
When there is a reduction in amplitude over every cycle of vibration, then the body is said to have

Damped vibration
Forced vibration
Under damped vibration
Free vibration

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Theory of Machine
In railway axle boxes, the bearing used is

Double row self aligning ball bearing
Cylindrical roller bearing
Deep groove ball bearing
Double row spherical roller bearing

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