Incompletely constrained motion
Partially constrained motion
Completely constrained motion
Successfully constrained motion
A. Incompletely constrained motion
Resultant force is equal to zero
Resultant couple is equal to zero
Resultant force and resultant couple are both equal to zero
Resultant force is numerically equal to the resultant couple, but neither of them need necessarily be zero
sin (θ + φ) + 1/ cos (θ - φ) + 1
cos (θ - φ) + 1/ sin (θ + φ) + 1
cos (θ + φ) + 1/ cos (θ - φ) + 1
cos (θ - φ) + 1/ cos (θ + φ) + 1
The former is mathematically accurate
The former is having turning pair
The former is most economical
The former is most rigid
P = W tan α
P = W tan (α + φ)
P = W (sin α + μ cos α)
P = W (cos α + μ sin α)
Simple gear train
Compound gear train
Reverted gear train
None of the above
Angle of friction
Angle of repose
Angle of projection
None of these
Watts mechanism
Grasshopper mechanism
Roberts mechanism
Peaucelliers mechanism
cosθ = sinα
sinθ = ± tanα
tanθ = ± cosα
cotθ = cosα
The periodic time of a particle moving with simple harmonic motion is the time taken by a particle for one complete oscillation.
The periodic time of a particle moving with simple harmonic motion is directly proportional to its angular velocity.
The velocity of a particle moving with simple harmonic motion is zero at the mean position.
The acceleration of the particle moving with simple harmonic motion is maximum at the mean position.
There is a reduction in amplitude after every cycle of vibration
No external force acts on a body, after giving it an initial displacement
A body vibrates under the influence of external force
None of the above
Parallel to AB
Perpendicular to AB
Along AB
At 45° to AB
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
2ECS
ECS/2
2ECS²
2E²CS
Free vibration with damping
Free vibration without damping
Forced vibration with damping
Forced vibration without damping
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
Simple
Compound
Binary
None of these
Turning pair
Rolling pair
Screw pair
Spherical pair
Reduce vibration
Reduce slip
Ensure uniform loading
Ensure proper alignment
Quick return mechanism of shaper
Four bar chain mechanism
Slider crank mechanism
Both (A) and (C) above
To dip the nose and tail
To raise the nose and tail
To raise the nose and dip the tail
To dip the nose and raise the tail
Hammer blow
Swaying couple
Variation in tractive force along the line of stroke
All of the above
Beam engine
Rotary engine
Oldhams coupling
Elliptical trammel
Bulky
Wears rapidly
Difficult to manufacture
Both (A) and (B) above
1 link with pin joints
2 links with pin joints
3 links with pin joints
4 links with pin joints
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
Tip of the gear tooth and flank of pinion
Tip of the pinion and flank of gear
Flanks of both gear and pinion
Tip of both gear and pinion
Knife edge follower
Flat faced follower
Spherical faced follower
Roller follower
(S₁ + S₂)/h
(S₁ - S₂)/h
(S₁ + S₂)/2h
(S₁ - S₂)/2h
Each of the four pairs is a turning pair
One is a turning pair and three are sliding pairs
Two are turning pairs and two are sliding pairs
Three are turning pairs and one is a sliding pair
Over damped
Under damped
Critically damped
Without vibrations