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Theory of Machine

Theory of Machine
Carnot cycle is

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

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Theory of Machine
A disturbing mass m₁ attached to the rotating shaft may be balanced by a single mass m₂ attached in the same plane of rotation as that of m₁, such that (where r₁ and r₂ are the radii of rotation of m₁ and m₂ respectively)

None of these
m₁ r₂ = m₂ r₁
m₁ m₂ = r₁ r₂
m₁ r₁ = m₂ r₂

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Theory of Machine
The relation between number of links (l) and number of joints (j) in a kinematic chain is

l = (3/4).(j + 3)
l = (1/2).(j + 2)
l = (2/3).(j + 2)
l = j + 4

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Theory of Machine
In a multiple V-belt drive, if one of the belts is broken, then we should replace

The broken belt and the belts on either side of it
The broken belt only
All the belts
None of these

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Theory of Machine
The Coriolis component of acceleration exists whenever a point moves along a path that has

Rotational motion
Tangential acceleration
Linear displacement
Gravitational acceleration

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Theory of Machine
Coriolis component acts

Somewhere in between above two
Perpendicular to sliding surfaces
None of these
Along sliding surfaces

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