physics 1901 (advanced)
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Physics 1901 (Advanced). Prof Geraint F. Lewis Rm 560, A29 [email protected] www.physics.usyd.edu.au/~gfl/Lecture. Rotational Motion. So far we have examined linear motion; Newton’s laws Energy conservation Momentum - PowerPoint PPT PresentationTRANSCRIPT
Semester 1 2009 http://www.physics.usyd.edu.au/~gfl/Lecture
Physics 1901 (Advanced)
Prof Geraint F. LewisRm 560, [email protected]/~gfl/Lecture
Semester 1 2009 http://www.physics.usyd.edu.au/~gfl/Lecture
Rotational Motion
So far we have examined linear motion; Newton’s laws Energy conservation Momentum
Rotational motion seems quite different, but is actually familiar.
Remember: We are looking at rotation in fixed coordinates, not rotating coordinate systems.
Semester 1 2009 http://www.physics.usyd.edu.au/~gfl/Lecture
Rotational VariablesRotation is naturally described in polar coordinates, where we can talk about an angular displacement with respect to a particular axis.
For a circle of radius r, an angular displacement of corresponds to an arc length of
Remember: use radians!
Semester 1 2009 http://www.physics.usyd.edu.au/~gfl/Lecture
Angular VariablesAngular velocity is the change of angle with time
There is a simple relation between angular velocity and velocity
Semester 1 2009 http://www.physics.usyd.edu.au/~gfl/Lecture
Angular Variables
Angular acceleration is the change of with time
Tangential acceleration is given by
Semester 1 2009 http://www.physics.usyd.edu.au/~gfl/Lecture
Rotational KinematicsNotice that the form of rotational relations is the same as the linear variables. Hence, we can derive identical kinematic equations:
Linear Rotational
a=constant constant
v=u+at o+ t
s=so+ut+½at2 o+ot+½t2
Semester 1 2009 http://www.physics.usyd.edu.au/~gfl/Lecture
Net AccelerationRemember, for circular motion, there is always centripetal acceleration
The total acceleration is the vector sum of arad and atan.
What is the source of arad?
Semester 1 2009 http://www.physics.usyd.edu.au/~gfl/Lecture
Rotational Dynamics
As with rotational kinematics, we will see that the framework is familiar, but we need some new concepts;
Linear Rotational
Mass Moment of Inertia
Force Torque
Semester 1 2009 http://www.physics.usyd.edu.au/~gfl/Lecture
Moment of Inertia
This quantity depends upon the distribution of the mass and the location of the axis of rotation.
Semester 1 2009 http://www.physics.usyd.edu.au/~gfl/Lecture
Moment of InertiaLuckily, the moment of inertia is typically;
where c is a constant and is <1.
Object I
Solid sphere 2/5 M R2
Hollow sphere 2/3 M R2
Rod (centre) 1/12 M L2
Rod (end) 1/3 M L2
Semester 1 2009 http://www.physics.usyd.edu.au/~gfl/Lecture
Energy in Rotation
To get something moving, you do work on it, the result being kinetic energy.
To get objects spinning also takes work, but what is the rotational equivalent of kinetic energy?
Problem: in a rotating object, each bit of mass has the same angular speed , but different linear speed v.
Semester 1 2009 http://www.physics.usyd.edu.au/~gfl/Lecture
Energy in RotationFor a mass at point P
Total kinetic energy
Semester 1 2009 http://www.physics.usyd.edu.au/~gfl/Lecture
Parallel Axis Theorem
The moment of inertia depends upon the mass distribution of an object and the axis of rotation.
For an object, there are an infinite number of moments of inertia!
Surely you don’t have to do an infinite number of integrations when dealing with objects?
Semester 1 2009 http://www.physics.usyd.edu.au/~gfl/Lecture
Parallel Axis Theorem
If we know the moment of inertia through the centre of mass, the moment of inertia along a parallel axis d is;
The axis does not have to be through the body!
Semester 1 2009 http://www.physics.usyd.edu.au/~gfl/Lecture
TorqueOpening a door requires not only an application of a force, but also how the force is applied;
It is ‘easier’ pushing a door further away from the hinge.
Pulling or pushing away from the hinge does not work!
From this we get the concept of torque.
Semester 1 2009 http://www.physics.usyd.edu.au/~gfl/Lecture
Torque
Torque causes angular acceleration
Only the component of force tangential to the direction of motion has an effect
Torque is
Semester 1 2009 http://www.physics.usyd.edu.au/~gfl/Lecture
Torque
Like force, torque is a vector quantity (in fact, the other angular quantities are also vectors). The formal definition of torque is
where the x is the vector cross product.
In which direction does this vector point?
Semester 1 2009 http://www.physics.usyd.edu.au/~gfl/Lecture
Vector Cross ProductThe magnitude of the resultant vector is
and is perpendicular to the plane containing vectors A and B.Right hand grip rule defines the
direction
Semester 1 2009 http://www.physics.usyd.edu.au/~gfl/Lecture
Torque and AccelerationAt point P, the tangential force gives a tangential acceleration of
This becomes
Semester 1 2009 http://www.physics.usyd.edu.au/~gfl/Lecture
Torque and Acceleration
For an arbitrarily shaped object
We have the rotational equivalent of Newton’s second law!
Torque produces an angular acceleration.
Notice the vector quantities. All rotational variables point along the axis of rotation.
(Read torques & equilibrium 11.0-11.3 in textbook)
Semester 1 2009 http://www.physics.usyd.edu.au/~gfl/Lecture
Rolling without Slipping
For a rolling wheel which does not slide, then the distance it travels is related to how much it turns.
Semester 1 2009 http://www.physics.usyd.edu.au/~gfl/Lecture
Rolling without Slipping
The total kinetic energy is
and
Where C is the constant of the Moment of Inertia
Semester 1 2009 http://www.physics.usyd.edu.au/~gfl/Lecture
Rolling without SlippingConservation of energy
Independent of mass & size
Any sphere beats any hoop!
What is the source of torque?
Semester 1 2009 http://www.physics.usyd.edu.au/~gfl/Lecture
Rolling without SlippingTorque is provided by friction acting at the surface (otherwise the ball would just slide).
Note that the normal force does not produce a torque (although it can with deformable surfaces and rolling friction).
Semester 1 2009 http://www.physics.usyd.edu.au/~gfl/Lecture
Rotational WorkIn linear mechanics, the work-kinetic energy theorem can be used to solve problems.
In rotational mechanics, we note that a force, Ftan, applied to a point on a wheel always points along the direction of motion.
Semester 1 2009 http://www.physics.usyd.edu.au/~gfl/Lecture
Rotational Work
If the torque is constant
Hence, we now have a rotational work-kinetic energy theorem, except
Semester 1 2009 http://www.physics.usyd.edu.au/~gfl/Lecture
Angular Momentum
In linear dynamics, complex interaction (collisions) can be examined using the conservation of momentum.
In rotational dynamics, the concept of angular momentum similarly eases complex interactions.
(Derivation similar to all other rotational quantities)
Semester 1 2009 http://www.physics.usyd.edu.au/~gfl/Lecture
Angular Momentum
In linear dynamics:
In rotational dynamics:
Hence, the net torque is equal to the rate of change of angular momentum. Hence, if there is no net torque, angular momentum is conserved.
Semester 1 2009 http://www.physics.usyd.edu.au/~gfl/Lecture
Angular Momentum
We can change the angular velocity by modifying the moment of inertia.
Angular momentum is conserved, but where has the extra energy come from?
Semester 1 2009 http://www.physics.usyd.edu.au/~gfl/Lecture
Angular MomentumI have to apply a force on the mass to change its linear velocity.
Through NIII, the mass applies a force on me.
For every torque there is an equal and opposite “retorque”.
Semester 1 2009 http://www.physics.usyd.edu.au/~gfl/Lecture
Angular Momentum
Consider a lecturer on a rotating stool holding a spinning wheel, with the axis of the wheel pointing towards the ceiling.
What happens when the wheel is turned over?
http://www.physics.lsa.umich.edu/demolab/demo.asp?id=696
Semester 1 2009 http://www.physics.usyd.edu.au/~gfl/Lecture
Angular Momentum
As with linear momentum, we can use conservation of angular momentum without having to worry about the various (internal) torques in action.
External torques will change the value of the total angular momentum.