Weight
Velocity
Acceleration
Force
A. Weight
Strain energy
Kinetic energy
Heat energy
Electrical energy
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
u² sin²α/2g
u² cos²α/2g
u² sin²α/g
u² cos²α/g
g/2
g
√2.g
2g
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
m1/m2
m1. g. sin α
m1.m2/m1 + m2
m1. m2.g (1 + sin α)/(m1 + m2)
πd3/16
πd3/32
πd4/32
πd4/64
No
Minimum
Maximum
None of these
ω
ωr
ω2r
ω/r
Coplanar non-concurrent forces
Non-coplanar concurrent forces
Non-coplanar non-concurrent forces
Intersecting forces
Angle of projection
Angle of inclination of the plane
Both (A) and (B)
None of these
√(P² + Q² + 2PQ sinθ)
√(P² + Q² + 2PQ cosθ)
√(P² + Q² - 2PQ cosθ)
√(P² + Q² - 2PQ tanθ)
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
50
100
200
400
Halved
Doubled
Quadrupled
None of these
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
Less than
Greater than
Equal to
None of these
Rolling friction
Dynamic friction
Limiting friction
Static friction
Balance each other
Cannot balance each other
Produce moment of a couple
Are equivalent
Zero
Minimum
Maximum
None of these
Directly
Inversely
Square root
None of these
20 kg, -ve sense
20 kg, + ve sense
10 kg, + ve sense
10 kg, -ve sense
2n³
2n
n²
3n² Where n = number of joints in a frame
Zeroth order
First order
Second order
Third order
m/min
rad/s
Revolutions/min
Both (B) and (C)
The point of C.G.
The point of metacenter
The point of application of the resultant of all the forces tending to cause a body to rotate about a certain axis
Point of suspension
kg/cm
Bar
Atmosphere
Newton
Less than
Greater than
Equal to
None of these
Change its motion
Balance the forces, already acting on it
Give rise to the internal stresses in it
All of these
Moment of inertia
Centre of gravity
Centre of percussion
Centre of mass