The system is unbalanced
Bearing centre line coincides with the axis
The shafts are rotating at very high speeds
Resonance is caused due to the heavy mass of the rotor
D. Resonance is caused due to the heavy mass of the rotor
Toothed gearing
Belt and rope drive
Ball and roller bearing
All of these
Self-closed
Force-closed
Friction closed
None of these
Simple gear train
Reverted gear train
Sun and planet gear
Differential gear
Radial component only
Tangential component only
Coriolis component only
Radial and tangential components both
The tip of a tooth of a mating gear digs into the portion between base and root circles
Gears do not move smoothly in the absence of lubrication
Pitch of the gears is not same
Gear teeth are undercut
Static friction
Dynamic friction
Limiting friction
Coefficient of friction
Pitch circle
Base circle
Prime circle
Outer circle
Shoe brake
Band brake
Band and block brake
Internal expanding brake
Directly proportional to the distance from the points to the instantaneous centre and is parallel to the line joining the point to the instantaneous centre
Directly proportional to the distance from the points to the instantaneous centre and is perpendicular to the line joining the point to the instantaneous centre
Inversely proportional to the distance from the points to the instantaneous centre and is parallel to the line joining the point to the instantaneous centre
Inversely proportional to the distance from the points to the instantaneous centre and is perpendicular to the line joining the point to the instantaneous centre
Be zero
Act in upward direction
Act in downward direction
None of these
No node
One node
Two nodes
Three nodes
The system is critically damped
There is no critical speed in the system
The system is also statically balanced
There will absolutely no wear of bearings
Is based on acceleration diagram
Is a simplified form of instantaneous center method
Utilises a quadrilateral similar to the diagram of mechanism for reciprocating engine
Enables determination of Carioles component
Turning pair
Screw pair
Belt and pulley
None of the above
Zero
Less than one
Greater than one
Infinity
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
Zero
Minimum
Maximum
None of these
Oldham's coupling
Elliptical trammel
Scotch yoke mechanism
All of these
0° and 90°
180° and 360°
Both (A) and (B)
None of these
ω/2π
2π/ω
ω × 2π
π/ω
Sliding and turning pairs
Sliding and rotary pairs
Turning and rotary pairs
Sliding pairs only
(r₁ + r₂) (y/x)
(r₁ + r₂) (x/y)
(r₁ - r₂) (y/x)
(r₁ - r₂) (x/y)
Higher pair
Lower pair
Rolling pair
Sliding pair
Watt governor
Porter governor
Pickering governor
Hartnell governor
Perpendicular to the acceleration force
Along the direction of acceleration force
Opposite to the direction of acceleration force
None of the above
Rolling pair
Sliding pair
Screw pair
Turning pair
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
A triangle
A point
Two lines
A straight line
2 mm
2.22 mm
2.50 mm
3.0 mm
Single slider crank chain
Whitworth quick return motion mechanism
Crank and slotted lever quick return motion mechanism
All of the above