0
1
2
-1
A. 0
The centre of the disc
The point of contact
An infinite distance on the plane surface
The point on the circumference situated vertically opposite to the contact point
The algebraic sum of the secondary forces must be equal to zero
The algebraic sum of the couples about any point in the plane of the secondary forces must be equal to zero
Both (A) and (B)
None of these
One direction only
Two directions only
More than one direction
None of these
Tension on tight side of belt
Tension on slack side of belt
Radius of pulley
All of the above
Pitch circle dia. × cosφ
Addendum circle dia. × cosφ
Clearance circle dia. × cosφ
Pitch circle dia. × sinφ
8.95/N²
89.5/N²
895/N²
8950/N²
Movement of a complete ship up and down in vertical plane about transverse axis
Turning of a complete ship in a curve towards right or left, while it moves forward
Rolling of a complete ship sideways
None of the above
Base circle
Pitch circle
Root circle
Prime circle
Intersecting and coplanar shafts
Nonintersecting and non-coplanar shafts
Parallel and coplanar shafts
Parallel and non-coplanar shafts
[c²/(1 + 2c)] (m + M) g.h
[2c²/(1 + 2c)] (m + M) g.h
[3c²/(1 + 2c)] (m + M) g.h
[4c²/(1 + 2c)] (m + M) g.h
Ellipse
Circle
Parabola
Hyperbola
A rigid link rotates instantaneously relative to another link at the instantaneous centre for the configuration of the mechanism considered.
The two rigid links have no linear velocity relative to each other at the instantaneous centre.
The velocity of the instantaneous centre relative to any third rigid link is same whether the instantaneous centre is regarded as a point on the first rigid link or on the second rigid link.
All of the above
Sliding pairs
Turning pairs
Rolling pairs
Higher pairs
Maximum
Minimum
Zero
None of these
(1/2) μ W R
(2/3) μ W R
(3/4) μ W R
μ W R
Lower pair
Higher pair
Spherical pair
Cylindrical pair
n = (l -1) - j
n = 2(l - 1) - 2j
n = 3(l - 1) - 2j
n = 4(l - 1) - 3j
Radial component
Tangential component
Coriolis component
None of these
Watt's mechanism
Grasshopper mechanism
Robert's mechanism
All of these
Completely constrained motion
Incompletely constrained motion
Successfully constrained motion
None of these
Parallel to each other
Perpendicular to each other
Inclined at 45°
Opposite to each other
Straight line path
Hyperbolic path
Parabolic path
Elliptical path
Circular
Tangent
Reciprocating
None of the above
T₁/T₂ = μ. θ. n
T₁/T₂ = [(1 - μ tanθ)/(1 + μ tanθ)]n
T₁/T₂ = (μ θ)n
T₁/T₂ = [(1 + μ tanθ)/(1 - μ tanθ)]n
In increasing velocity ratio
In decreasing the slip of the belt
For automatic adjustment of belt position so that belt runs centrally
Increase belt and pulley life
Completely constrained motion
Partially constrained motion
Incompletely constrained motion
Freely constrained motion
Cause withdrawing or throttling of steam
Reduce length of effective stroke of piston
Reduce maximum opening of port to steam
All of these
Pitch circle
Base circle
Prime circle
Outer circle
(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)]
Is in motion
Is at rest
Just begins to slide over the surface of the other body
None of the above