mr2/2
mr2/4
mr2/6
mr2/8
A. mr2/2
Coplanar
Meet at one point
Both (A) and (B) above
All be equal
g. cos² β/2u². sin (α + β). cos α
2u². sin (α + β). cos α/g. cos² β
g. cos² β/2u². sin (α - β). cos α
2u². sin (α - β). cos α/g. cos² β
kg/cm
Bar
Atmosphere
Newton
Tangent of angle between normal reaction and the resultant of normal reaction and 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
Area of the triangle
Twice the area of the triangle
Half the area of the triangle
None of these
Curved surface
Convex surface
Horizontal surface
None of these
Angular displacement
Angular velocity
Angular acceleration
All of these
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
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
Weight of the vehicle
(Velocity)2 of the vehicle
Nature of the road surface
Coefficient of friction between the road and vehicle contact point
Dyne
Kilogram
Newton
Watt
Coplanar concurrent forces
Coplanar non-concurrent forces
Non-coplanar concurrent forces
Non-coplanar non-concurrent forces
Coefficient of friction
Angle of friction
Angle of repose
Sliding friction
y = (gx²/2u² cos²α) + x. tanα
y = (gx²/2u² cos²α) - x. tanα
y = x. tanα - (gx²/2u² cos²α)
y = x. tanα + (gx²/2u² cos²α)
A path, traced by a projectile in the space, is known as trajectory.
The velocity, with which a projectile is projected, is known as the velocity of projection.
The angle, with the horizontal, at which a projectile is projected, is known as angle of projection.
All of the above
1 + m
1 - m
1 / m
m
2π. √(gh/kG² + h²)
2π. √(kG² + h²/gh)
1/2π. √(gh/kG² + h²)
1/2π. √(kG² + h²/gh)
h [(2a + b)/(a + b)]
(h/2) [(2a + b)/(a + b)]
(h/3) [(2a + b)/(a + b)]
(h/3) [(a + b)/(2a + b)]
kcal
kg-m
kW-hr
h.p
Kinetic friction
Limiting friction
Angle of repose
Coefficient of friction
Equal to
Less than
Greater than
None of these
ω
ωr
ω2r
ω/r
Limiting friction
Kinematic friction
Frictional resistance
Dynamic friction
Purely translation
Purely rotational
Combined translation and rotational
None of these
2π. √(g/δ)
1/2π. √(g/δ)
2π. √(δ/g)
1/2π. √(δ/g)
25
50
100
250
2P sinθ/2
2P cosθ/2
2P tanθ/2
2P cotθ/2
P = mW - C
P = m/W + C
P = mW + C
P = C - mW
Right angled triangle
Equilateral triangle
Square
Circle
P = Q
Q = R
Q = 2R
None of these