12
14
18
24
C. 18
(m.g + S₁)/(m.g + S₂) = r₁/r₂
(m.g - S₁)/(m.g - S₂) = r₂/r₁
S₁/S₂ = r₁/r₂
S₂/S₁ = r₁/r₂
P = W tan α
P = W tan (α + φ)
P = W (sin α + μ cos α)
P = W (cos α + μ sin α)
Slow speed
Moderate speed
Highs peed
Any one of these
Longitudinal vibration
Transverse vibration
Torsional vibration
None of these
D-slide valve
Governor
Flywheel
Meyer's expansion valve
θ/2
θ
2θ
4θ
One-half
Two-third
n times
1/n times
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
Have a surface contact when in motion
Have a line or point contact when in motion
Are kept in contact by the action of external forces, when in motion
Permit relative motion
For changing the direction of motion of the belt
For applying tension
For increasing velocity ratio
All of the above
During which the follower returns to its initial position
Of rotation of the cam for 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
Yes
No
Unpredictable
None of these
Perpendicular to its axis
Parallel to its axis
In a circle about its axis
None of these
Compound gears
Worm and wheel method
Hooke's joint
Crown gear
Radial component
Tangential component
Coriolis component
None of these
Upward
Downward
Forward
Backward
Simple pendulum
Compound pendulum
Torsional pendulum
Second's pendulum
Completely constrained motion
Incompletely constrained motion
Successfully constrained motion
None of these
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
Weak material of the belt
Weak material of the pulley
Uneven extensions and contractions of the belt when it passes from tight side to slack side
Expansion of the belt
Mean speed to the maximum equilibrium speed
Mean speed to the minimum equilibrium speed
Difference of the maximum and minimum equilibrium speeds to the mean speed
Sum of the maximum and minimum equilibrium speeds to the mean speed
π (r₁ + r₂) + (r₁ + r₂)²/x + 2x
π (r₁ + r₂) + (r₁ - r₂)²/x + 2x
π (r₁ - r₂) + (r₁ - r₂)²/x + 2x
π (r₁ - r₂) + (r₁ + r₂)²/x + 2x
The control of speed fluctuations
Balancing of forces and couples
Kinematic analysis
Vibration analysis
Machines transmit mechanical work, whereas structures transmit forces
In machines, relative motion exists between its members, whereas same does not exist in case of structures
Machines modify movement and work, whereas structures modify forces
Efficiency of machines as well as structures is below 100%
Remains constant
Decreases
Increases
None of these
Radial component only
Tangential component only
Coriolis component only
Radial and tangential components both
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
2ECS
ECS/2
2ECS²
2E²CS
(r₁ - r₂) (1 - cosθ)
(r₁ + r₂) (1 + cosθ)
(r₁ - r₂) [(1 - cosθ)/cos θ]
(r₁ + r₂) [(1 - cosθ)/cos θ]
0.25
0.5
1
2