Energy
Mass
Momentum
Angle
C. Momentum
Equal to
Less than
Greater than
None of these
In the shaded area
In the hole
At O
None of these
Directly proportional
Inversely proportional
Cube root
None of these
Impulsive force
Mass
Weight
Momentum
Limiting friction
Sliding friction
Rolling friction
Kinematic friction
m₁. m₂. g/(m₁ + m₂)
2m₁. m₂. g/(m₁ + m₂)
(m₁ + m₂)/ m₁. m₂. g
(m₁ + m₂)/2m₁. m₂. g
Less than
Greater than
Equal to
None of these
Coplanar non-concurrent forces
Non-coplanar concurrent forces
Non-coplanar non-concurrent forces
Intersecting forces
More inclined when moving
Less inclined when moving
More inclined when standing
Less inclined when standing
The algebraic sum of the resolved parts of the forces in the given direction
The sum of the resolved parts of the forces in the given direction
The difference of the forces multiplied by the cosine of θ
The sum of the forces multiplied by the sine of θ
N-m
m/s
m/s2
rad/s2
0°
30°
45°
60°
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.
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
0° and 180°
180° and 0°
90° and 180°
90° and 0°
Potential energy
Kinetic energy
Electrical energy
Chemical energy
Potential energy
Kinetic energy
Power
None of these
Coplanar force
Non-coplanar forces
Moment
Couple
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
D + d
D - d
D × d
D / d
Same
More
Less
May be less of more depending on nature of surfaces and velocity
[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)
g/2
g
√2.g
2g
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
The C.G. of a circle is at its centre
The C.G. of a triangle is at the intersection of its medians
The C.G. of a rectangle is at the intersection of its diagonals
The C.G. of a semicircle is at a distance of r/2 from the centre
Simple pendulum
Compound pendulum
Torsional pendulum
Second's pendulum
Along the plane
Horizontally
Vertically
At an angle equal to the angle of friction to the inclined plane
Perfect frame
Deficient frame
Redundant frame
None of the above
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
ω
ωr
ω2r
ω/r