5,367 r.p.m.
6,000 r.p.m.
9,360 r.p.m.
12,000 r.p.m.
A. 5,367 r.p.m.
Zero
One
π/2
π
Completely constrained motion
Incompletely constrained motion
Successfully constrained motion
None of these
Magnitude of the forces on journal
Angular velocity of journal
Clearance between journal and bearing
Radius of journal
Less
More
Equal
May be less or more depending on efficiency
All points of the disc have the same velocity
The centre of the disc has zero acceleration
The centre of the disc has centrifugal acceleration
The point on the disc making contact with the plane surface has zero acceleration
Simple gear train
Compound gear train
Reverted gear train
Epicyclic gear train
Pitch circle dia. × cosφ
Addendum circle dia. × cosφ
Clearance circle dia. × cosφ
Pitch circle dia. × sinφ
95 mm
Slightly less than 95 mm
Slightly more than 95 mm
45 mm
All four pairs are turning
Three pairs turning and one pair sliding
Two pairs turning and two pairs sliding
One pair turning and three pairs sliding
Radial component
Tangential component
Coriolis component
None of these
Journal bearing
Ball and Socket joint
Leave screw and nut
None of the above
Second inversion of double slider crank chain
Third inversion of double slider crank chain
Second inversion of single slider crank chain
Third inversion of slider crank chain
The interference is inherently absent.
The variation in centre distance of shafts increases radial force.
A convex flank is always in contact with concave flank.
The pressure angle is constant throughout the teeth engagement.
Eight links
Six links
Four links
Twelve links
Less
More
Same
Data are insufficient to determine same
Primary unbalanced force
Secondary unbalanced force
Two cylinders of locomotive
Partial balancing
Flexible coupling
Universal coupling
Chain coupling
Oldham's coupling
(r₁² - r₂²)/(r₁ - r₂)
(r₁² - r₂²)/(r₁ + r₂)
(r₁³ - r₂³)/(r₁² - r₂²)
(r₁³ - r₂³)/(r₁ - r₂)
Turning pair
Rolling pair
Sliding pair
Spherical pair
Linear displacement
Rotational motion
Gravitational acceleration
Tangential acceleration
(r₁ + r₂) (y/x)
(r₁ + r₂) (x/y)
(r₁ - r₂) (y/x)
(r₁ - r₂) (x/y)
90° and 180°
45° and 225°
180° and 270°
270° and 360°
1/2π × √(s/m)
1/2π × √(g/δ)
0.4985/√δ
Any one of these
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
Difference of minimum fluctuation of speed and the mean speed
Difference of the maximum and minimum speeds
Sum of maximum and minimum speeds
Variations of speed above and below the mean resisting torque line
Shaft revolving in a bearing
Straight line motion mechanisms
Automobile steering gear
All of the above
0°
90°
180°
360°
9/8
9/82
9/16
9/128
Is a simplified version of instantaneous centre method
Utilises a quadrilateral similar to the diagram of mechanism for reciprocating engine
Enables determination of coriolis component
Is based on the acceleration diagram
45° in the direction of rotation of the link containing the path
45° in the direction opposite to the rotation of the link containing the path
90° in the direction of rotation of the link containing the path
180° in the direction opposite to the rotation of the link containing the path