Both the balls undergo an equal change in momentum
The change in momentum suffered by rubber ball is more than the lead ball
The change in momentum suffered by rubber ball is less than the lead ball
None of the above
B. The change in momentum suffered by rubber ball is more than the lead ball
Equal to
Less than
Greater than
None of these
Increase
Decrease
Not be effected
None of these
P = Q
Q = R
Q = 2R
None of these
Limiting friction
Sliding friction
Rolling friction
Kinematic friction
Angle of friction
Angle of repose
Angle of projection
None of these
Equal to
Less than
Greater than
None of these
ω/r
ω.r
ω2/r
ω2.r
Balance each other
Produce a couple and an unbalanced force
Are equivalent
Cannot balance each other
Change its motion
Balance the other forces acting on it
Retard its motion
All of the above
a = α/ r
a = α.r
a = r / α
None of these
Circular arc
Parabola
Hyperbola
Elliptical
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 same as centre of gravity
The point of suspension
The point of application of the resultant of all the forces tending to cause a body to rotate about a certain axis
None of the above
Inelastic bodies
Elastic bodies
Neither elastic nor inelastic bodies
None of these
Reversible
Non-reversible
Ideal
None of these
The algebraic sum of the forces, constituting the couple is zero
The algebraic sum of the forces, constituting the couple, about any point is the same
A couple cannot be balanced by a single force but can be balanced only by a couple of opposite sense
All of the above
P + Q
P - Q
P / Q
Q / P
1 m
2 m
3 m
4 m
ω.y
ω2.y
ω2/y
ω3.y
Momentum and impulse
Torque and energy
Torque and work
Moment of a force and angular momentum.
v
2v
4v
8v
Newton's first law of motion
Newton's second law of motion
Principle of conservation of energy
Principle of conservation of momentum
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
Translatory motion
Rotational motion
Combined translatory and rotational motion
None of the above
Equal to
Less than
Greater than
None of these
g sinθ
g cosθ
g tanθ
None of these
If any number of forces acting at a point can be represented by the sides of a polygon taken in order, then the forces are in equilibrium
If any number of forces acting at a point can be represented in direction and magnitude by the sides of a polygon, then the forces are in equilibrium
If a polygon representing forces acting at a point is closed then forces are in equilibrium
If any number of forces acting at a point can be represented in direction and magnitude by the sides of a polygon taken in order, then the forces are in equilibrium
Equal to
Less than
Greater than
None of these
N-m
m/s
m/s2
rad/s2
0.5r
0.6 r
0.7 r
0.8 r