m1/m2
m1. g. sin α
m1.m2/m1 + m2
m1. m2.g (1 + sin α)/(m1 + m2)
D. m1. m2.g (1 + sin α)/(m1 + m2)
Energy
Mass
Momentum
Angle
Less than
More than
Equal to
None of These
mr2/2
mr2/4
mr2/6
mr2/8
Arm of man
Pair of scissors
Pair of clinical tongs
All of the above
Mechanical advantage is greater than velocity ratio
Mechanical advantage is equal to velocity ratio
Mechanical advantage is less than velocity ratio
Mechanical advantage is unity
Gravitational pull exerted by the earth
Forces experienced by body in atmosphere
Force of attraction experienced by particles
Gravitational force of attraction towards the centre of the earth
Magnitude
Direction
Position or line of action
All of the above
W sinθ
W cosθ
W secθ
W cosecθ
+8.9 m/s2
-8.9 m/s2
+9.8 m/s2
-9.8 m/s2
At distance from the plane base 3r
At distance from the plane base 3r
At distance from the plane base 3r
At distance from the plane base
Magnitude of the force
Line of action of the force
Nature of the force i.e. whether the force is push or pull
All of the above
P = mW - C
P = m/W + C
P = mW + C
P = C - mW
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
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
The tangent of the angle of friction is equal to coefficient of friction
The angle of repose is equal to angle of friction
The tangent of the angle of repose is equal to coefficient of friction
The sine of the angle of repose is equal to coefficient to friction
mr2/2
mr2/4
mr2/6
mr2/8
Kinetic friction
Limiting friction
Angle of repose
Coefficient of friction
Mass
Volume
Density
Acceleration
Inelastic bodies
Elastic bodies
Neither elastic nor inelastic bodies
None of these
m/min
rad/s
Revolutions/min
Both (B) and (C)
Along the plane
Horizontally
Vertically
At an angle equal to the angle of friction to the inclined plane
Concurrence of the medians
Intersection of its altitudes
Intersection of bisector of angles
Intersection of diagonals
db3/12
bd³/12
db³/36
bd³/36
Principle of independence of forces
Principle of resolution of forces
Principle of transmissibility of forces
None of these
Limiting friction
Sliding friction
Rolling friction
Kinematic friction
db³/12
bd³/12
db³/36
bd³/36
D + d
D - d
D × d
D / d
W between P and F
F between W and P
P between W and F
W, P and F all on one side
Equal to
Less than
Greater than
None of these
Reversible machine
Non-reversible machine
Neither reversible nor non-reversible machine
Ideal machine