8.95/N²
89.5/N²
895/N²
8950/N²
C. 895/N²
On their point of contact
At the centre of curvature
At the centre of circle
At the pin joint
2
3
4
5
Fluctuation of energy
Maximum fluctuation of energy
Coefficient of fluctuation of energy
None of these
Governor A is more sensitive than governor B
Governor B is more sensitive than governor A
Both governors A and B are equally sensitive
None of the above
Balanced completely
Balanced partially
Balanced by secondary forces
Not balanced
sinφ + sinα = b/c
cosφ - sinα = c/b
cotφ - cotα = c/b
tanφ + cotα = b/c
In plane rotation with variable velocity
In plane translation with variable velocity
In plane motion which is a resultant of plane translation and rotation
Restrained to rotate while sliding over another body
kG + l₁
kG² + l₁
(kG² + l₁²)/ l₁
(kG + l₁²)/ l₁
45° to each other
90° to each other
120° to each other
180° to each other
Minimum
Maximum
Zero
Infinity
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
Two links should be fixed
One link should be fixed
None of the links should be fixed
There is no such criterion
Primary unbalanced force
Secondary unbalanced force
Two cylinders of locomotive
Partial balancing
Toothed gearing
Belt and rope drive
Ball and roller bearing
All of these
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
Offset between centre lines of cam and follower
Lift of follower
Angle of ascent
All 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
Line or point contact
Surface contact
Body contact
None of these
ω² × NO
ω² × CO
ω² × CN
ω² × QN
Between I₁, and I₂ but nearer I₁
Between I₁, and I₂ but nearer to I₂
Exactly in the middle of the shaft
Nearer to I₁ but outside
l = (1/2).(j + 2)
l = (2/3).(j + 2)
l = (3/4).(j + 3)
l = j + 4
Incompletely constrained motion
Partially constrained motion
Completely constrained motion
Successfully constrained motion
Belt, rope and chain drives
Gears, cams
Ball and roller bearings
All of the above
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
0.4985/√δ
0.5615/√δ
0.571/√δ
0.6253/√δ
Perpendicular to the acceleration force
Along the direction of acceleration force
Opposite to the direction of acceleration force
None of the above
Open pair
Kinematic pair
Sliding pair
None of these
Will remain same
Will change
Could change or remain unaltered depending on which link is fixed
Will not occur
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
Ball bearing
Roller bearing
Needle roller bearing
Thrust bearing