Coplanar
Meet at one point
Both (A) and (B) above
All be equal
C. Both (A) and (B) above
Less than
Equal to
More than
None of these
πd3/16
πd3/32
πd4/32
πd4/64
db³/12
bd³/12
db³/36
bd³/36
2mr2/3
2mr2/5
7mr2/3
7mr2/5
Reducing the problem of kinetics to equivalent statics problem
Determining stresses in the truss
Stability of floating bodies
Designing safe structures
kW (kilowatt)
hp (horse power)
kcal/sec
kcal/kg sec
Along the plane
Horizontally
Vertically
At an angle equal to the angle of friction to the inclined plane
Same
Half
Double
None of these
[m₁ m₂/2(m₁ + m₂)] (u₁ - u₂)²
[2(m₁ + m₂)/m₁ m₂] (u₁ - u₂)²
[m₁ m₂/2(m₁ + m₂)] (u₁² - u₂²)
[2(m₁ + m₂)/m₁ m₂] (u₁² - u₂²)
Concurrence of the medians
Intersection of its altitudes
Intersection of bisector of angles
Intersection of diagonals
(1/2π). √(l/g)
(1/2π). √(g/l)
2π. √(l/g)
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
mr2/2
mr2/4
mr2/6
mr2/8
Is the turning effect produced by a force, on the body, on which it acts
Is equal to the product of force acting on the body and the perpendicular distance of a point and the line of action of the force
Is equal to twice the area of the triangle, whose base is the line representing the force and whose vertex is the point, about which the moment is taken
All of the above
h/2
h/3
h/4
h/6
Their algebraic sum is zero
Their lines of action are at equal distances
The algebraic sum of their moments about any point in their plane is zero
The algebraic sum of their moments about any point is equal to the moment of their resultant force about the same point.
Not a replace them by a single force
To replace them by a single force
To replace them by a single force through C.G.
To replace them by a couple
9 cm4
12 cm4
16 cm4
20 cm4
R = u² cos2α/g
R = u² sin2α/g
R = u² cosα/g
R = u² sinα/g
Gravitational pull exerted by the earth
Forces experienced by body in atmosphere
Force of attraction experienced by particles
Gravitational force of attraction towards the centre of the earth
Coplanar concurrent forces
Coplanar non-concurrent forces
Like parallel forces
Unlike parallel forces
Same
Double
Half
Four times
P/sin β = Q/sin α = R/sin
P/sin α = Q/sin β = R/sin
P/sin = Q/sin α = R/sin β
P/sin α = Q/sin = R/sin β
Rotate about itself without moving
Move in any one direction rotating about itself
Be completely at rest
All of these
94.9 cm
99.4 cm
100 cm
101 cm
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
P = W tanα
P = W tan (α + φ)
P = W (sinα + μcosα)
P = W (cosα + μsinα)
A force acting in the opposite direction to the motion of the body is called force of friction
The ratio of the limiting friction to the normal reaction is called coefficient of friction
A machine whose efficiency is 100% is known as an ideal machine
The velocity ratio of a machine is the ratio of load lifted to the effort applied
Equal to
Less than
Greater than
None of these
ω.y
ω2.y
ω2/y
ω3.y