Coefficient of friction
Angle of friction
Angle of repose
Sliding friction
A. Coefficient of friction
The centre of heavy portion
The bottom surface
The midpoint of its axis
All of the above
πN/60
πN/180
2πN/60
2πN/180
a = α/ r
a = α.r
a = r / α
None of these
The point of C.G.
The point of metacenter
The point of application of the resultant of all the forces tending to cause a body to rotate about a certain axis
Point of suspension
Equal to
Less than
Greater than
None of these
0°
30°
45°
60°
One point
Two points
Plane
Perpendicular planes
Rolling friction
Dynamic friction
Limiting friction
Static friction
A reversible machine
A non-reversible machine
An ideal machine
None of these
Angle between normal reaction and the resultant of normal reaction and the limiting friction
Ratio of limiting friction and normal reaction
The friction force acting when the body is just about to move
The friction force acting when the body is in motion
r/2
2r/3
r/A
3r/2
Algebraic sum of the horizontal components of all the forces should be zero
Algebraic sum of the vertical components of all the forces should be zero
Algebraic sum of moments of all the forces about any point should be zero
All of the above
Coplanar non-concurrent forces
Non-coplanar concurrent forces
Non-coplanar non-concurrent forces
Intersecting forces
Meet in a point
Be all parallel
At least two of them must meet
All the above are correct
Magnitude
Direction
Position or line of action
All of the above
√(P² + Q² + 2PQ sinθ)
√(P² + Q² + 2PQ cosθ)
√(P² + Q² - 2PQ cosθ)
√(P² + Q² - 2PQ tanθ)
Meet at one point, but their lines of action do not lie on the same plane
Do not meet at one point and their lines of action do not lie on the same plane
Meet at one point and their lines of action also lie on the same plane
Do not meet at one point, but their lines of action lie on the same plane
50 mm
75 mm
87.5 mm
125 mm
Reversible
Non-reversible
Ideal
None of these
Equal to
Less than
Greater than
None of these
Three forces acting at a point will be in equilibrium
Three forces acting at a point can be represented by a triangle, each side being proportional to force
If three forces acting upon a particle are represented in magnitude and direction by the sides of a triangle, taken in order, they will be in equilibrium
If three forces acting at a point are in equilibrium, each force is proportional to the sine of the angle between the other two
Zero
One
Between zero and one
More than one
mr2/2
mr2/4
mr2/6
mr2/8
Limiting friction
Sliding friction
Rolling friction
Kinematic friction
a4/4
a4/8
a4/12
a4/36
Static friction
Dynamic friction
Limiting friction
Coefficient of friction
Dyne
Kilogram
Newton
Watt
3r/ 8
4r/ 3π
8r/3
3r/4π
Same
Half
Double
None of these
4
8
16
20