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.
C. The algebraic sum of their moments about any point in their plane is zero
ω
ωr
ω2r
ω/r
Equal to
Less than
Greater than
None of these
Impulsive force
Mass
Weight
Momentum
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
Coplanar concurrent forces
Coplanar non-concurrent forces
Non-coplanar concurrent forces
None of these
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
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
Stable
Unstable
Neutral
None of these
a = α/ r
a = α.r
a = r / α
None of these
kg-m2
kg-m-s2
kg/m2
m4
mv2
mgv2
0.5 mv2
0.5 mgv2
g (m1 - m2)/(m1 + m2)
2g (m1 - m2)/(m1 + m2)
g (m1 + m2)/(m1 - m2)
2g (m1 + m2)/(m1 - m2)
D/(D - d)
D/(D + d)
2D/(D - d)
2D/(D + d)
Zero
One
Between zero and one
More than one
Reversible
Non-reversible
Ideal
None of these
A path, traced by a projectile in the space, is known as trajectory.
The velocity, with which a projectile is projected, is known as the velocity of projection.
The angle, with the horizontal, at which a projectile is projected, is known as angle of projection.
All of the above
P = Q
Q = R
Q = 2R
None of these
kg-m²
m²/kg.
kg/m²
kg/m
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
Perfect frame
Deficient frame
Redundant frame
None of the above
The same as centre of gravity
The point of suspension
The point of application of the resultant of all the forces tending to cause a body to rotate about a certain axis
None of the above
Downward at its upper end
Upward at its upper end
Zero at its upper end
Perpendicular to the wall at its upper end
The point of C.G.
The point of metacenter
The point of application of the resultant of all the forces tending to cause a body to rotate about a certain axis
Point of suspension
Equal to
Less than
Greater than
None of these
2P sinθ/2
2P cosθ/2
2P tanθ/2
2P cotθ/2
3r/ 8
4r/ 3π
8r/3
3r/4π
Towards the wall at its upper end
Away from the wall at its upper end
Downward at its upper end
Upward at its upper end
y = (gx²/2u² cos²α) + x. tanα
y = (gx²/2u² cos²α) - x. tanα
y = x. tanα - (gx²/2u² cos²α)
y = x. tanα + (gx²/2u² cos²α)
1 + m
1 - m
1 / m
m