u² sin²α/2g
u² cos²α/2g
u² sin²α/g
u² cos²α/g
A. u² sin²α/2g
1/m
V.R./m
m/V.R.
1/(m × V.R.)
2mr2/3
2mr2/5
7mr2/3
7mr2/5
2n³
2n
n²
3n² Where n = number of joints in a frame
Is constant at every instant
Varies from point to point
Is maximum in the start and minimum at the end
Is minimum in the start and maximum at the end
(v1 - v2)/(u1 - u2)
(v₂ - v₁)/(u1 - u2)
(u1 - u2)/(v1 - v2)
(u₂ + u₁)/(v₂ + v₁)
Equal to
Less than
Greater than
None of these
Equal to one
Less than one
Greater than one
None of these
0.1 joule/s
1 joule/s
10 joules/s
100 joules/s
g sinθ
g cosθ
g tanθ
None of these
One point
Two points
Plane
Perpendicular planes
Impulsive force
Mass
Weight
Momentum
20 N
40 N
120 N
None of these
(1/2π). √(l/g)
(1/2π). √(g/l)
2π. √(l/g)
None of these
t = 2u. sinα/g
t = 2u. cosα/g
t = 2u. tanα/g
t = 2u/g.sinα
W sinθ
W cosθ
W secθ
W cosecθ
Weight
Velocity
Acceleration
Force
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
Rotate about itself without moving
Move in any one direction rotating about itself
Be completely at rest
All of these
Potential energy only
Kinetic energy of translation only
Kinetic energy of rotation only
Kinetic energy of translation and rotation both
a = α/ r
a = α.r
a = r / α
None of these
Tangent of 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
v
2v
4v
8v
9 cm4
12 cm4
16 cm4
20 cm4
Output to the input
Work done by the machine to the work done on the machine
Mechanical advantage to the velocity ratio
All of the above
Work is said to be done
Power is being transmitted
Body has kinetic energy of translation
None of these
db3/12
bd³/12
db³/36
bd³/36
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
1/2
2/3
3/2
2/4
Velocity
Acceleration
Momentum
None of these
Newton's first law of motion
Newton's second law of motion
Newton's third law of motion
None of these