Reducing the problem of kinetics to equivalent statics problem
Determining stresses in the truss
Stability of floating bodies
Designing safe structures
A. Reducing the problem of kinetics to equivalent statics problem
First
Second
Third
None of these
Bodies having relative motion
Two dry surfaces
Two lubricated surfaces
Solids and liquids
Principle of independence of forces
Principle of resolution of forces
Principle of transmissibility of forces
None of these
mr2/3
2mr2/3
2mr2/5
3mr2/5
Downward at its upper end
Upward at its upper end
Zero at its upper end
Perpendicular to the wall at its upper end
Reducing the problem of kinetics to equivalent statics problem
Determining stresses in the truss
Stability of floating bodies
Designing safe structures
Some force acts on a body, but displacement is zero
No force acts on a body but some displacement takes place
Either (A) or (B)
None of the above
Two times
Same
Half
None of these
Coplanar concurrent forces
Coplanar non-concurrent forces
Non-coplanar concurrent forces
Non-coplanar non-concurrent forces
Change its motion
Balance the forces, already acting on it
Give rise to the internal stresses in it
All of these
Dyne
Kilogram
Newton
Watt
Balance each other
Cannot balance each other
Produce moment of a couple
Are equivalent
Arm of man
Pair of scissors
Pair of clinical tongs
All of the above
Coefficient of friction
Angle of friction
Angle of repose
Sliding friction
v
2v
4v
8v
mr2/2
mr2/4
mr2/6
mr2/8
Equal to
Less than
Greater than
None of these
7.8 N
8.9 N
9.8 N
12 N
MS/3
MS/4
MS/5
None of these
Limiting friction
Sliding friction
Rolling friction
Kinematic friction
The tangent of the angle of friction is equal to coefficient of friction
The angle of repose is equal to angle of friction
The tangent of the angle of repose is equal to coefficient of friction
The sine of the angle of repose is equal to coefficient to friction
Work is said to be done
Power is being transmitted
Body has kinetic energy of translation
None of these
Perfect
Imperfect
Deficient
None of these
Tangent of angle between normal reaction and the resultant of normal reaction and limiting friction
Ratio of limiting friction and normal reaction
The friction force acting when the body is just about to move
The friction force acting when the body is in motion
(v1 - v2)/(u1 - u2)
(v₂ - v₁)/(u1 - u2)
(u1 - u2)/(v1 - v2)
(u₂ + u₁)/(v₂ + v₁)
N-m
m/s
m/s2
rad/s2
(ΣV)2 + (ΣH)2
√[(ΣV)2 + (ΣH)2]
(ΣV)2 +(ΣH)2 +2(ΣV)(ΣH)
√[(ΣV)2 +(ΣH)2 +2(ΣV)(ΣH)]
kW (kilowatt)
hp (horse power)
kcal/sec
kcal/kg sec
P = W tan (α - φ)
P = W tan (α + φ)
P = W tan (φ - α)
P = W cos (α + φ)
Static friction
Dynamic friction
Limiting friction
Coefficient of friction