Balanced completely
Balanced partially
Balanced by secondary forces
Not balanced
B. Balanced partially
Hammer blow
Swaying couple
Variation in tractive force along the line of stroke
All of the above
(1/2) μ W (r₁ + r₂)
(2/3) μ W (r₁ + r₂)
(1/2) μ W [(r₁³ - r₂³)/(r₁² - r₂²)]
(2/3) μ W [(r₁³ - r₂³)/(r₁² - r₂²)]
No node
One node
Two nodes
Three nodes
Quick return mechanism of shaper
Four bar chain mechanism
Slider crank mechanism
Both (A) and (C) above
Self-closed
Force-closed
Friction closed
None of these
sinφ + sinα = b/c
cosφ - sinα = c/b
cotφ - cotα = c/b
tanφ + cotα = b/c
L + 1
L - 1
L
L + 2
Varies in magnitude but constant in direction
Varies in direction but constant in magnitude
Varies in magnitude and direction both
Constant in magnitude and direction both
Bolt and nut
Lead screw of a lathe
Ball and socket joint
Ball bearing and roller bearing
The difference between the maximum and minimum energies is called maximum fluctuation of energy
The coefficient of fluctuation of speed is the ratio of maximum fluctuation of speed to the mean speed
The variations of energy above and below the mean resisting torque line is known as fluctuation of energy
None of the above
Over-damped
Under damped
Critically damped
Without vibrations
Vector sum of radial component and coriolis component
Vector sum of tangential component and coriolis component
Vector sum of radial component and tangential component
Vector difference of radial component and tangential component
For constant velocity ratio transmission between two gears, the common normal at the point of contact must always pass through a fixed point on the line joining the centres of rotation of gears.
For involute gears, the pressure angle changes with the change in centre distance between gears.
The epicyclic gear trains involve rotation of atleast one gear axis about some other gear axis.
All of the above
Universal joint
Knuckle joint
Oldham's coupling
Flexible coupling
v
(2/3). v
(3/2). v
(9/4). v
Uniform velocity
Simple harmonic motion
Uniform acceleration and retardation
Cycloidal motion
(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)]
(1/2). μ W cosecα (r₁ + r₂)
(2/3). μ W cosecα (r₁ + r₂)
(1/2). μ W cosecα [(r₁³ - r₂³)/(r₁² - r₂²)]
(2/3). μ W cosecα [(r₁³ - r₂³)/(r₁² - r₂²)]
Along PO
Perpendicular to PO
At 45° to PO
None of the above
Right side pivot of this link
Left side pivot of this link
A point obtained by intersection on extending adjoining links
Cant occur
x₁/x₂
log(x₁/x₂)
loge(x₁/x₂)
log(x₁.x₂)
(1/2) μ W R cosecα
(2/3) μ W R cosecα
(3/4) μ W R cosecα
μ W R cosecα
Pendulum type governor
Dead weight governor
Spring loaded governor
Inertia governor
Inner dead centre
Outer dead centre
Right angles to the link of the stroke
All of the above
Compound gears
Worm and wheel method
Hooke's joint
Crown gear
9/8
9/82
9/16
9/128
Cause withdrawing or throttling of steam
Reduce length of effective stroke of piston
Reduce maximum opening of port to steam
All of these
Of rotation of the cam for a definite displacement of the follower
Through which the cam rotates during the period in which the follower remains in the highest position
Moved by the cam from the instant the follower begins to rise, till it reaches its highest position
Moved by the cam from beginning of ascent to the termination of descent
Screw pair
Spherical pair
Turning pair
Sliding pair
Four times the first one
Same as the first one
One fourth of the first one
One and a half times the first one