Parallel to OA
Perpendicular to OA
At 45° to OA
Along AO
B. Perpendicular to OA
Upward
Downward
Forward
Backward
Lower pair
Higher pair
Open pair
Close pair
ω²r. (n + 1)/n
ω²r. (n - 1)/n
ω²r. n/(n + 1)
ω²r. n/(n - 1)
Pitch circle to the bottom of a tooth
Pitch circle to the top of a tooth
Top of a tooth to the bottom of a tooth
Addendum circle to the clearance circle
Less
More
Equal
May be less or more depending on efficiency
Diameter of disc
Span of shaft
Eccentricity
All of these
Point or line contact between the two elements when in motion
Surface contact between the two elements when in motion
Elements of pairs not held together mechanically
Two elements that permit relative motion
Permanent instantaneous centres
Fixed instantaneous centres
Neither fixed nor permanent instantaneous centres
None of the above
Universal joint
Knuckle joint
Oldham's coupling
Flexible coupling
0
2
4
6
The system is critically damped
There is no critical speed in the system
The system is also statically balanced
There will absolutely no wear of bearings
Turning pairs
Sliding pairs
Spherical pairs
Self-closed pairs
Equal to 1
Less than 2
Equal to 2
Greater than 2
For changing the direction of motion of the belt
For applying tension
For increasing velocity ratio
All of the above
1
2
3
4
Radius of rotation of balls increases as the equilibrium speed decreases
Radius of rotation of balls decreases as the equilibrium speed decreases
Radius of rotation of balls increases as the equilibrium speed increases
Radius of rotation of balls decreases as the equilibrium speed increases
Point or line contact between the two elements when in motion
Surface contact between the two elements when in motion
Elements of pairs not held together mechanically
Two elements that permit relative motion
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
Bolt and nut
Lead screw of a lathe
Ball and socket joint
Ball bearing and roller bearing
Natural frequency of vibration
Position of balancing weights
Moment of inertia
Centripetal acceleration
(1 - sinφ)/(1 + sinφ)
(1 + sinφ)/(1 - sinφ)
(1 - tanφ)/(1 + tanφ)
(1 + tanφ)/(1 - tanφ)
Minimise the effect of primary forces
Minimise the effect of secondary forces
Have perfect balancing
To start the locomotive quickly
Angle of friction
Angle of repose
Angle of projection
None of these
Circular
Tangent
Reciprocating
None of the above
Tractive force
Swaying couple
Hammer blow
None of these
Inside admission valve
Outside admission valve
Piston slide valve
None of these
(1/2) μ W R
(2/3) μ W R
(3/4) μ W R
μ W R
2
4
3
None of the above
90° and 180°
45° and 225°
180° and 270°
270° and 360°
Remains constant
Decreases
Increases
None of these