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
C. The friction force acting when the body is just about to move
Equal to
Less than
Greater than
None of these
Coplanar concurrent forces
Coplanar non-concurrent forces
Non-coplanar concurrent forces
Non-coplanar non-concurrent forces
πd3/16
πd3/32
πd4/32
πd4/64
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
If any number of forces acting at a point can be represented by the sides of a polygon taken in order, then the forces are in equilibrium
If any number of forces acting at a point can be represented in direction and magnitude by the sides of a polygon, then the forces are in equilibrium
If a polygon representing forces acting at a point is closed then forces are in equilibrium
If any number of forces acting at a point can be represented in direction and magnitude by the sides of a polygon taken in order, then the forces are in equilibrium
Work is done by a force of 1 N when it displaces a body through 1 m
Work is done by a force of 1 kg when it displaces a body through 1 m
Work is done by a force of 1 dyne when it displaces a body through 1 cm
Work is done by a force of 1 g when it displaces a body through 1 cm
1/2
2/3
3/2
2/4
Strain energy
Kinetic energy
Heat energy
Electrical energy
Limiting friction
Kinematic friction
Frictional resistance
Dynamic friction
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
h [(2a + b)/(a + b)]
(h/2) [(2a + b)/(a + b)]
(h/3) [(2a + b)/(a + b)]
(h/3) [(a + b)/(2a + b)]
Translatory
Rotary
Circular
Translatory as well as rotary
P + m.a = 0
P - m.a = 0
P × m.a = 0
P/m.a = 0
y = (gx²/2u² cos²α) + x. tanα
y = (gx²/2u² cos²α) - x. tanα
y = x. tanα - (gx²/2u² cos²α)
y = x. tanα + (gx²/2u² cos²α)
√3. W (tensile) and 2W (compressive)
2W (tensile) and √3. W (compressive)
2√3. W (tensile) and 2√3. W (compressive)
None of the above
Ellipse
Hyperbola
Parabola
Circle
Two times
Same
Half
None of these
Directly
Inversely
Square root
None of these
2n³
2n
n²
3n² Where n = number of joints in a frame
ω
ωr
ω2r
ω/r
The algebraic sum of the forces, constituting the couple is zero
The algebraic sum of the forces, constituting the couple, about any point is the same
A couple cannot be balanced by a single force but can be balanced only by a couple of opposite sense
All of the above
Moment of inertia
Centre of gravity
Centre of percussion
Centre of mass
No
Minimum
Maximum
None of these
Increasing the length of the handle
Increasing the radius of the load drum
Increasing the number of teeth of the pinion
All of the above
ω/2π
2π/ω
2π × ω
π/ω
Between 60 and 70 %
Between 70 and 80 %
Between 80 and 90 %
100 %
a = α/ r
a = α.r
a = r / α
None of these
W sinθ
W cosθ
W secθ
W cosecθ
Angular displacement
Angular velocity
Angular acceleration
All of these
L/2
L/3
3L/4
2L/3