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Theory of Machine

Theory of Machine
The behaviour of gases can be fully determined by

1 law
3 laws
4 laws
2 laws

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Theory of Machine
In order to facilitate starting of locomotive in any position, the cranks of a locomotive with two cylinders, are placed at

120° to each other
45° to each other
180° to each other
90° to each other

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Theory of Machine
With usual notations for different parameters involved, the maximum fluctuations of energy for a flywheel is given by

EC S/2
2E²CS
2ECS
2ECS²

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Theory of Machine
To obviate axial thrust, following gear drive is used

Double helical gears having opposite teeth
Single helical gear in which one of the teeth of helix angle a is more
Double helical gears having identical teeth
Mutter gears

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

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

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

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