Magnitude of the forces on journal
Angular velocity of journal
Clearance between journal and bearing
Radius of journal
D. Radius of journal
Perpendicular to sliding surfaces
Along sliding surfaces
Somewhere in between above two
None of the above
45 mm
Slightly less than 45 mm
Slightly more than 45 mm
95 mm
Transverse vibrations
Torsional vibrations
Longitudinal vibrations
All of these
1
1/π
π
2 π
Sum
Difference
Product
Ratio
9/8
9/82
9/16
9/128
No node
One node
Two nodes
Three nodes
Higher pair
Lower pair
Rolling pair
Sliding pair
A rigid link rotates instantaneously relative to another link at the instantaneous centre for the configuration of the mechanism considered.
The two rigid links have no linear velocity relative to each other at the instantaneous centre.
The velocity of the instantaneous centre relative to any third rigid link is same whether the instantaneous centre is regarded as a point on the first rigid link or on the second rigid link.
All of the above
Theory of machines
Applied mechanics
Mechanisms
Kinetics
Turning pair
Rolling pair
Screw pair
Spherical pair
Free vibration with damping
Free vibration without damping
Forced vibration with damping
Forced vibration without damping
Rack and pinion
Worm and wheel
Spiral gears
None of the above
Below the critical speed
Near the critical speed
Above the critical speed
None of these
Line or point contact
Surface contact
Body contact
None of these
10° to 20°
20° to 30°
30° to 40°
60° to 80°
(1/2). μ W cosec α (r₁ + r₂)
(2/3).μ W cosec α (r₁ + r₂)
(1/2). μ W cosec α [(r₁³ - r₂³)/(r₁² - r₂²)]
(2/3). μ W cosec α [(r₁³ - r₂³)/(r₁² - r₂²)]
Over damped
Under damped
Critically damped
Without vibrations
Turning pairs
Sliding pairs
Spherical pairs
Self-closed pairs
Remains constant
Decreases
Increases
None of these
(Length of the path of approach)/(Circular pitch)
(Length of path of recess)/(Circular pitch)
(Length of the arc of contact)/(Circular pitch)
(Length of the arc of approach)/cosφ
One-half
Two-third
Three-fourth
Whole
Structure
Mechanism
Kinematic chain
Inversion
ω² × OQ
ω² × OQ sinθ
ω² × OQ cosθ
ω² × OQ tanθ
Changing of a higher pair to a lower pair
Turning its upside down
Obtained by fixing different links in a kinematic chain
Obtained by reversing the input and output motion
Longitudinal vibrations
Transverse vibrations
Torsional vibrations
None of these
No acceleration
Only linear acceleration
Only angular acceleration
Both linear and angular acceleration
Hammer blow
Swaying couple
Variation in tractive force along the line of stroke
All of the above
Double slider crank chain
Elliptical trammel
Scotch yoke mechanism
All of these
Vertically and parallel
Vertically and perpendicular
Horizontally and parallel
Horizontally and perpendicular