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Theory of Machine

Theory of Machine
Carnot cycle is

a quasi static cycle
an irreversible cycle
a reversible cycle
a semi-reversible cycle

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Theory of Machine
The Coriolis component of acceleration depends upon

Both (A) and (B)
Angular velocity of the link
Velocity of slider
None of these

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Theory of Machine
The velocity of a flat-faced follower when it has contact with the flank of a circular arc cam, is given by

ωR cosθ
ω(R - r₁) cosθ
ωr₁ sinθ
ω(R - r₁) sinθ

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Theory of Machine
If some links are connected such that motion between them can take place in more than one direction, it is called

Incompletely constrained motion
Successfully constrained motion
Partially constrained motion
Completely constrained motion

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Theory of Machine
In a Hartnell governor, the stiffness of the spring is given by (where S1 and S2 = Spring forces exerted on the sleeve at max. and min. radii of rotation, and h = Compression of the spring)

(S₁ - S₂) / h
(S₁ + S₂) / 2h
(S₁ - S₂) / 2h
(S₁ + S₂) / h

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Theory of Machine
The ratio of maximum fluctuation of energy to the work-done per cycle is called

Fluctuation of energy
Maximum fluctuation of energy
Coefficient of fluctuation of energy
None of these

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