3mr2/5
3mr2/10
2mr2/5
4mr2/5
B. 3mr2/10
N-m
m/s
m/s2
rad/s2
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
v
2v
4v
8v
kcal
kg-m
kW-hr
h.p
ω
ωr
ω2r
ω/r
50
100
200
400
Weight of the vehicle
(Velocity)2 of the vehicle
Nature of the road surface
Coefficient of friction between the road and vehicle contact point
Balance each other
Constitute a moment
Constitute a couple
Constitute a moment of couple
db³/12
bd³/12
db³/36
bd³/36
Weight
Velocity
Acceleration
Force
The kinetic energy of a body during impact remains constant.
The kinetic energy of a body before impact is equal to the kinetic energy of a body after impact.
The kinetic energy of a body before impact is less than the kinetic energy of a body after impact.
The kinetic energy of a body before impact is more than the kinetic energy of a body after impact.
Potential energy
Kinetic energy
Power
None of these
kilogram
Newton
Watt
Dyne
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
Along the plane
Horizontally
Vertically
At an angle equal to the angle of friction to the inclined plane
mr2/2
mr2/4
mr2/6
mr2/8
h/2
h/3
h/4
h/6
The centre of heavy portion
The bottom surface
The midpoint of its axis
All of the above
α = 45° + φ/2
α = 45° - φ/2
α = 90° + φ
α = 90° - φ
g (m1 - m2)/(m1 + m2)
2g (m1 - m2)/(m1 + m2)
g (m1 + m2)/(m1 - m2)
2g (m1 + m2)/(m1 - m2)
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
Will
Will not
Either A or B
None of these
Proportional to normal load between the surfaces
Dependent on the materials of contact surface
Proportional to velocity of sliding
Independent of the area of contact surfaces
kg-m²
m²/kg.
kg/m²
kg/m
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
Do not meet at one point but their lines of action lie on the same plane
None of the above
Change its motion
Balance the forces, already acting on it
Give rise to the internal stresses in it
All of these
a2/8
a3/12
a4/12
a4/16
T.ω (in watts)
T.ω/60 (in watts)
T.ω/75 (in kilowatts)
T.ω/4500 (in kilowatts)
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 = u² cos2α/g
R = u² sin2α/g
R = u² cosα/g
R = u² sinα/g