A wheel in uniform motion about an axis passing through its centre and perpendicular to its plane is considered to be in mechanical (translational plus rotational) equilibrium because no net external force or torque is required to sustain its motion. However, the particles that constitute the wheel do experience a centripetal acceleration directed towards the centre. How do you reconcile this fact with the wheel being in equilibrium? How would you set a half-wheel into uniform motion about an axis passing through the centre of mass of the wheel and perpendicular to its plane? Will you require external forces to sustain the motion?
A wheel in uniform motion about an axis passing through its centre and perpendicular to its plane is considered to be in mechanical (translational plus rotational) equilibrium because no net external force or torque is required to sustain its motion. However, the particles that constitute the wheel do experience a centripetal acceleration directed towards the centre. How do you reconcile this fact with the wheel being in equilibrium? How would you set a half-wheel into uniform motion about an axis passing through the centre of mass of the wheel and perpendicular to its plane? Will you require external forces to sustain the motion?
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1 Answer
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This is a short answer type question as classified in NCERT Exemplar
Wheel is a rigid body. The particles that constitute the wheel do experience a centripetal acceleration directed towards the centre. This acceleration arises due to internal elastic forces which cancel out in pairs.
In a half wheel the distribution of mass about its centre of mass is not symmetrical, therefore the direction of angular momentum of the wheel does not coincide with the direction of its angular velocity. Hence an external torque is required to maintain the motion of the wheel.
Similar Questions for you
Case – I : When disk slides down
Case – II : When disk rolls down
This is a multiple choice type question as classified in NCERT Exemplar
a, b, d
a) according to the perpendicular axes theorem statement 1 is wrong
b) As z’|z so distance between them = a
So according to parallel axes theorem Iz’=Iz+m (a/ )2= Iz+ma2/2
Hence b is true
c) z’ is not parallel to z hence Parallel axes does not applied so statement is false
d) as x and y axes are symmetrical . hence Ix=Iy so d is true
d) as x and y axes are symmetrical . hence Ix=Iy so d is true
This is a multiple choice type question as classified in NCERT Exemplar
b, c
a) When r>r’

Torque about z-axis t=r F
b) t’=r’ which is along negative z axis
c) tz=Fr = magnitude of torque about z axis where r is perpendicular between F and z axis so torque along positive z axis is greater than negative z axis.
d) We are always calculating resultant torque about common axis. Hence total torque not equal to combination of torque along both axis of z, because they are not on common axis.
This is a multiple choice type question as classified in NCERT Exemplar
a, b, c, d
As we know torque = r F = rFsin
a) when forces act radially angle =0 hence torque =0
b) when forces are acting on the axis of rotation r=0 torque=0
c) when forces acting parallel to the axis of rotation angle =0 so torque =0
d) when torque by forces are equal and opposite torque net = t1-t2=0
This is a multiple choice type question as classified in NCERT Exemplar
(a), (b)As we know L= r p where r is position vector and p is the linear momentum . the direction of L is perpendicular to both r and p by right hand rule.
For particle 1
I1=r1 mv is out of the plane of the paper and perpendicular to r1 and p . similarly I2=r2 m (-v) is into the plane of the paper and perpendicular to r2 and -p.
Hence total angular momentum
L= L1+L2= I1=r1 mv+ (r2 m (-v)
L= mvd1-mvd2 as d2>d1
So total angular momentum will be inwards so I = l = mv (d2-d1)⊗
L= mvd1-mvd2 as d2>d1
So total angular momentum will be inwards so I = l = mv (d2-
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