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Theory of Machine

Theory of Machine
The periodic time of one oscillation for a simple pendulum is

(1/2π). √(g/l)
2π. √(l/g)
2π. √(g/l)
(1/2π). √(l/g)

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Theory of Machine
Balancing of rotating and reciprocating parts of an engine is necessary when it runs at

Any one of these
Highs peed
Moderate speed
Slow speed

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Theory of Machine
Oldham’s coupling is an inversion of the kinematic chain used in

Universal joint
Whitworth quick return mechanism
Rotary engine
Elliptical trammels

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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

Critically damped
Over-damped
Without vibrations
Under damped

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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

Forced vibration
Free vibration
Damped vibration
Under damped vibration

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Theory of Machine
In locomotives, the ratio of the connecting rod length to me crank radius is kept very large in order to

Have perfect balancing
Minimize the effect of secondary forces
To start the locomotive quickly
Minimize the effect of primary forces

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