√3. W (tensile) and 2W (compressive)
2W (tensile) and √3. W (compressive)
2√3. W (tensile) and 2√3. W (compressive)
None of the above
A. √3. W (tensile) and 2W (compressive)
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
Newton
Pascal
Watt
Joule
mv2
mgv2
0.5 mv2
0.5 mgv2
A reversible machine
A non-reversible machine
An ideal machine
None of these
Translatory
Rotary
Circular
Translatory as well as rotary
ω.√(y² - r²)
ω.√(r² - y²)
ω².√(y² - r²)
ω².√(r² - y²)
Everybody continues in its state of rest or of uniform motion, in a straight line, unless it is acted upon by some external force
The rate of change of momentum is directly proportional to the impressed force, and takes place in the same direction, in which the force acts
To every action, there is always an equal and opposite reaction
None of the above
Second moment of force
Second moment of area
Second moment of mass
All of these
Direction of the axis of rotation
Magnitude of angular displacement
Sense of angular displacement
All of these
Will
Will not
Either A or B
None of these
Arm of man
Pair of scissors
Pair of clinical tongs
All of the above
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
Maximum
Minimum
Zero
Infinity
The periodic time of a particle moving with simple harmonic motion is the time taken by a particle for one complete oscillation.
The periodic time of a particle moving with simple harmonic motion is directly proportional to its angular velocity.
The velocity of the particle moving with simple harmonic motion is zero at the mean position.
The acceleration of the particle moving with simple harmonic motion is maximum at the mean position.
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
a = α/ r
a = α.r
a = r / α
None of these
Mass
Volume
Density
Acceleration
94.9 cm
99.4 cm
100 cm
101 cm
Directly
Inversely
Square root
None of these
Work is said to be done
Power is being transmitted
Body has kinetic energy of translation
None of these
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
ω
ωr
ω2r
ω/r
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
6t² - 8t
3t² + 2t
6f - 8
6f - 4
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
0.5r
0.6 r
0.7 r
0.8 r
Equal to
Equal and opposite to
Less than
Greater than
Equal to
Less than
Greater than
None of these
Curved surface
Convex surface
Horizontal surface
None of these
20 N
100 N
500 N
None of these