Bodies having relative motion
Two dry surfaces
Two lubricated surfaces
Solids and liquids
A. Bodies having relative motion
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
(BD³/12) - (bd³/12)
(DB³/12) - (db³/12)
(BD³/36) - (bd³/36)
(DB³/36) - (db³/36)
6t² - 8t
3t² + 2t
6f - 8
6f - 4
t = 2u. sinα/g
t = 2u. cosα/g
t = 2u. tanα/g
t = 2u/g.sinα
Composition
Resolution
Decomposition
None of these
W between P and F
F between W and P
P between W and F
W, P and F all on one side
Stable
Unstable
Neutral
None of these
Meet at one point, but their lines of action do not lie on the same plane
Do not meet at one point and their lines of action do not lie on the same plane
Do not meet at one point but their lines of action lie on the same plane
None of the above
W/√3 (compression)
W/√3 (tension)
2W/√3 (compression)
2W/√3 (tension)
D/(d₁ + d₂)
D/(d₁ - d₂)
2D/(d₁ + d₂)
2D/(d₁ - d₂)
W sinθ
W cosθ
W tanθ
W cotθ
bh3/4
bh3/8
bh3/12
bh3/36
Same at every point on its line of action
Different at different points on its line of action
Minimum, if it acts at the centre of gravity of the body
Maximum, if it acts at the centre of gravity of the body
kW (kilowatt)
hp (horse power)
kcal/sec
kcal/kg sec
Towards the wall at its upper end
Away from the wall at its upper end
Upwards at its upper end
Downwards at its upper end
Simple pendulum
Compound pendulum
Torsional pendulum
Second's pendulum
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
Potential energy
Kinetic energy
Electrical energy
Chemical energy
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
No
Minimum
Maximum
None of these
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
Reversible machine
Non-reversible machine
Neither reversible nor non-reversible machine
Ideal machine
These forces are equal
The lines of action of these forces meet in a point
The lines of action of these forces are parallel
Both (B) and (C) above
g sinθ
g cosθ
g tanθ
None of these
Kinetic friction
Limiting friction
Angle of repose
Coefficient of friction
Two times
Same
Half
None of these
2π. √(g/δ)
1/2π. √(g/δ)
2π. √(δ/g)
1/2π. √(δ/g)
Static friction
Dynamic friction
Limiting friction
Coefficient of friction
Reducing the problem of kinetics to equivalent statics problem
Determining stresses in the truss
Stability of floating bodies
Designing safe structures
Angle between normal reaction and the resultant of normal reaction and the limiting friction
Ratio of limiting friction and normal reaction
The ratio of minimum friction force to the friction force acting when the body is just about to move
The ratio of minimum friction force to friction force acting when the body is in motion