Remain horizontal
Slant up towards direction of pull
Slant down towards direction of pull
None of the above
C. Slant down towards direction of pull
Nature of surfaces
Area of contact
Shape of the surfaces
All of the above
Reversible machine
Non-reversible machine
Neither reversible nor non-reversible machine
Ideal machine
h/2
h/3
h/4
h/6
ml2/4
ml2/ 6
ml2/8
ml2/12
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
Halved
Doubled
Quadrupled
None of these
1 m
2 m
3 m
4 m
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
2.√(gh)
√(gh)
√(2gh)
2g.√h
Equal to 50 %
Less than 50 %
Greater than 50 %
100 %
P = W tanα
P = W tan (α + φ)
P = W (sinα + μcosα)
P = W (cosα + μsinα)
Coplanar concurrent forces
Coplanar non-concurrent forces
Non-coplanar concurrent forces
Non-coplanar non-concurrent forces
38 m
62.5 m
96 m
124 m
bh3/4
bh3/8
bh3/12
bh3/36
Rotate about itself without moving
Move in any one direction rotating about itself
Be completely at rest
All of these
L/2
L/3
3L/4
2L/3
Area of the triangle
Twice the area of the triangle
Half the area of the triangle
None of these
t = g cos β/2u sin (α - β)
t = 2u sin (α - β)/g cos β
t = g cos β/2u sin (α + β)
t = 2u sin (α + β)/g cos β
These forces are equal
The lines of action of these forces meet in a point
The lines of action of these forces are parallel
Both (B) and (C) above
The three forces must be equal
The three forces must be at 120° to each other
The three forces must be in equilibrium
If the three forces acting at a point are in equilibrium, then each force is proportional to the sine of the angle between the other two
Reversible machine
Non-reversible machine
Neither reversible nor non-reversible machine
Ideal machine
Compression or tension
Buckling or shear
Shear or tension
All of the above
Static friction
Dynamic friction
Limiting friction
Coefficient of friction
a = α/ r
a = α.r
a = r / α
None of these
P/sin β = Q/sin α = R/sin
P/sin α = Q/sin β = R/sin
P/sin = Q/sin α = R/sin β
P/sin α = Q/sin = R/sin β
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
The algebraic sum of the resolved parts of the forces in the given direction
The sum of the resolved parts of the forces in the given direction
The difference of the forces multiplied by the cosine of θ
The sum of the forces multiplied by the sine of θ
Coplanar concurrent forces
Coplanar non-concurrent forces
Non-coplanar concurrent forces
None of these
Directly proportional
Inversely proportional
Cube root
None of these
Two times
Same
Half
None of these