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
D. All of the above
Inner edge
Outer edge
Corners
None of these
cosθ = sinα
sinθ = ± tanα
tanθ = ± cosα
cotθ = cosα
Free vibration
Forced vibration
Damped vibration
Under damped vibration
Increasing the spring stiffness
Decreasing the spring stiffness
Increasing the ball mass
Decreasing the ball mass
Turning pair
Rolling pair
Screw pair
Spherical pair
l - 2
l - 1
l
l + 1
Wear is less
Power absorbed is less
Both wear and power absorbed are low
The pressure developed being high provides tight sealing
Grasshopper mechanism
Watt mechanism
Peaucellier's mechanism
Tchebicheff mechanism
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
n = 3(l - 1) - 2j - h
n = 2(l - 1) -2j - h
n = 3(l - 1) - 3j - h
n = 2(l - 1) - 3j - h
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
Be zero
Act in upward direction
Act in downward direction
None of these
Number of cycles per hour
Number of cycles per minute
Number of cycles per second
None of these
Bolt and nut
Lead screw of a lathe
Ball and socket joint
Ball bearing and roller bearing
Incompletely constrained motion
Partially constrained motion
Completely constrained motion
Successfully constrained motion
Higher pair
Lower pair
Rolling pair
Sliding pair
Fluctuation of energy
Maximum fluctuation of energy
Coefficient of fluctuation of energy
None of these
Remain in the same place for all configurations of the mechanism
Vary with the configuration of the mechanism
Moves as the mechanism moves, but joints are of permanent nature
None of the above
15
28
30
8
Spur gear
Spiral gear
Bevel gear
Worm gear
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
Spur gear
Helical gear
Bevel gear
None of the above
ω² × OQ
ω² × OQ sinθ
ω² × OQ cosθ
ω² × OQ tanθ
[(r² + R²) cosφ]/2
[(r² + R²) sinφ]/2
[(r + R) cosφ]/2
[(r + R) sinφ]/2
0° and 90°
0° and 180°
90° and 180°
180° and 360°
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
n₁ + n₂
n₁ + n₂ + 1
n₁ + n₂ - 1
n₁ + n₂ - 2
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
Tractive force
Swaying couple
Hammer blow
None of these
Theory of machines
Applied mechanics
Mechanisms
Kinetics