Weight of the vehicle
(Velocity)2 of the vehicle
Nature of the road surface
Coefficient of friction between the road and vehicle contact point
B. (Velocity)2 of the vehicle
Perfect frame
Deficient frame
Redundant frame
None of the above
At distance from the plane base 3r
At distance from the plane base 3r
At distance from the plane base 3r
At distance from the plane base
ω
ωr
ω2r
ω/r
Same as
Twice
Thrice
Four times
Same
More
Less
May be less of more depending on nature of surfaces and velocity
If a system of coplanar forces is in equilibrium, then their algebraic sum is zero
If a system of coplanar forces is in equilibrium, then the algebraic sum of their moments about any point in their plane is zero
The algebraic sum of the moments of any two forces about any point is equal to moment of the resultant about the same point
Positive and negative couples can be balanced
Direction of the axis of rotation
Magnitude of angular displacement
Sense of angular displacement
All of these
ω.√(y² - r²)
ω.√(r² - y²)
ω².√(y² - r²)
ω².√(r² - y²)
Inward
Outward
Towards front
Towards back
5
10
20
40
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
Rolling friction
Dynamic friction
Limiting friction
Static friction
Same
Half
Double
None of these
Same
Half
Double
None of these
Potential energy only
Kinetic energy of translation only
Kinetic energy of rotation only
Kinetic energy of translation and rotation both
Coplanar concurrent forces
Coplanar non-concurrent forces
Like parallel forces
Unlike parallel forces
g. cos² β/2u². sin (α + β). cos α
2u². sin (α + β). cos α/g. cos² β
g. cos² β/2u². sin (α - β). cos α
2u². sin (α - β). cos α/g. cos² β
Equal to
Less than
Greater than
None of these
kcal
kg-m
kW-hr
h.p
Newton's first law of motion
Newton's second law of motion
Principle of conservation of energy
Principle of conservation of momentum
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
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
Principle of independence of forces
Principle of resolution of forces
Principle of transmissibility of forces
None of these
(2/3) Ml2
(1/3) Ml2
(3/4) Ml2
(1/12) Ml2
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
Change its motion
Balance the other forces acting on it
Retard its motion
All of the above
Newton's first law of motion
Newton's second law of motion
Newton's third law of motion
None of these
Bodies having relative motion
Two dry surfaces
Two lubricated surfaces
Solids and liquids
tan(α + φ)/tanα
tanα/tan (α + φ)
tan(α - φ)/tanα
None of these
A reversible machine
A non-reversible machine
An ideal machine
None of these