Turning pairs
Sliding pairs
Spherical pairs
Self-closed pairs
A. Turning pairs
Directly proportional to the distance from the points to the instantaneous centre and is parallel to the line joining the point to the instantaneous centre
Directly proportional to the distance from the points to the instantaneous centre and is perpendicular to the line joining the point to the instantaneous centre
Inversely proportional to the distance from the points to the instantaneous centre and is parallel to the line joining the point to the instantaneous centre
Inversely proportional to the distance from the points to the instantaneous centre and is perpendicular to the line joining the point to the instantaneous centre
Fc = ar + b
Fc = ar - b
Fc = ar
Fc = a/r + b
Zero
One
π/2
π
Shaft tends to vibrate in longitudinal direction
Torsional vibrations occur
Shaft tends to vibrate vigorously in transverse direction
Combination of transverse and longitudinal vibration occurs
Motion of a piston in the cylinder of a steam engine
Motion of a square bar in a square hole
Motion of a shaft with collars at each end in a circular hole
All of the above
[(r² + R²) cosφ]/2
[(r² + R²) sinφ]/2
[(r + R) cosφ]/2
[(r + R) sinφ]/2
Universal joint
Knuckle joint
Oldham's coupling
Flexible coupling
Transverse vibrations
Torsional vibrations
Longitudinal vibrations
All of these
To raise the bow and stern
To lower the bow and stern
To raise the bow and lower the stern
To raise the stern and lower the bow
Watts mechanism
Grasshopper mechanism
Roberts mechanism
Peaucelliers mechanism
Is the maximum horizontal unbalanced force caused by the mass provided to balance the reciprocating masses.
Is the maximum vertical unbalanced force caused by the mass added to balance the reciprocating masses
Varies as the square root of the speed
Varies inversely with the square of the speed
fn/2
2 fn
4 fn
8 fn
Halved
Doubled
Quadrupled
None of these
Angular acceleration of the body
Moment of inertia of the body
Periodic time of the body
Frequency of vibration of the body
ωx
ω²x
ω²/x
ω³/x
The tip of a tooth of a mating gear digs into the portion between base and root circles
Gears do not move smoothly in the absence of lubrication
Pitch of the gears is not same
Gear teeth are undercut
45° to each other
90° to each other
120° to each other
180° to each other
Bulky
Wears rapidly
Difficult to manufacture
Both (A) and (B) above
Be zero
Act in upward direction
Act in downward direction
None of the above
Leads by 90°
Lags by 90°
Leads by 180°
Are in phase
Each of the four pairs is a turning pair
One is a turning pair and three are sliding pairs
Two are turning pairs and two are sliding pairs
Three are turning pairs and one is a sliding pair
Simple gear train
Compound gear train
Reverted gear train
Epicyclic gear train
Slider crank mechanism
Four bar chain mechanism
Quick return motion mechanism
All of these
Gyroscope
Pantograph
Valve and valve gears
All of the above
The power absorbed in operating the piston valve is less than D-slide valve
The wear of the piston valve is less than the wear of the D-slide valve
The D-slide valve is also called outside admission valve.
All of the above
Double helical gears having opposite teeth
Double helical gears having identical teeth
Single helical gear in which one of the teeth of helix angle a is more
Mutter gears
Parallel to OA
Perpendicular to OA
At 45° to OA
Along AO
Inertia
Momentum
Moment of momentum
Torque
The sum of the two masses is equal to the total mass of body
The centre of gravity of the two masses coincides with that of the body
The sum of mass moment of inertia of the masses about their centre of gravity is equal to the mass moment of inertia of the body
All of the above
Free vibration
Forced vibration
Damped vibration
Under damped vibration