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
D. The C.G. of a semicircle is at a distance of r/2 from the centre
n
n²
2n
2n - 1
P = W tanα
P = W tan (α + φ)
P = W (sinα + μcosα)
P = W (cosα + μsinα)
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
15 N and 5 N
20 N and 5 N
15 N and 15 N
None of these
Nature of surfaces
Area of contact
Shape of the surfaces
All of the above
N-m
m/s
m/s2
rad/s2
Balance each other
Cannot balance each other
Produce moment of a couple
Are equivalent
Coplanar concurrent forces
Coplanar non-concurrent forces
Non-coplanar concurrent forces
Non-coplanar non-concurrent forces
Angle of projection
Angle of inclination of the plane
Both (A) and (B)
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
Meet at one point and their lines of action also lie on the same plane
Do not meet at one point, but their lines of action lie on the same plane
Straight line
Parabola
Hyperbola
Elliptical
h/2
J/3
h/6
h/4
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
0° and 180°
180° and 0°
90° and 180°
90° and 0°
94.9 cm
99.4 cm
100 cm
101 cm
Resultant couple
Moment of the forces
Resulting couple
Moment of the couple
0.5 cm
1.0 cm
1.5 cm
2.5 cm
Between 60 and 70 %
Between 70 and 80 %
Between 80 and 90 %
100 %
Impulsive force
Mass
Weight
Momentum
Equal to
Less than
Greater than
None of these
Newton's first law of motion
Newton's second law of motion
Principle of conservation of energy
Principle of conservation of momentum
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
Less than
More than
Equal to
None of These
Two times
Same
Half
None of these
W sinθ
W cosθ
W tanθ
None of these
Increase
Decrease
Remain the same
None of these
Algebraic sum of the horizontal components of all the forces should be zero
Algebraic sum of the vertical components of all the forces should be zero
Algebraic sum of moments of all the forces about any point should be zero
All of the above
Direction of the axis of rotation
Magnitude of angular displacement
Sense of angular displacement
All of these
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
Arm of man
Pair of scissors
Pair of clinical tongs
All of the above