## Lecture 24: Rolling Motion - Gyroscopes - VERY NON-INTUITIVE

author: Walter H. G. Lewin, Center for Future Civic Media, Massachusetts Institute of Technology, MIT
recorded by: Massachusetts Institute of Technology, MIT
published: Oct. 10, 2008,   recorded: November 1999,   views: 46732
released under terms of: Creative Commons Attribution Non-Commercial Share Alike (CC-BY-NC-SA)

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# Description

1. Pure Roll of Hollow and Solid Cylinders:

In pure roll, the object is not skidding or slipping, and the speed of the center of mass equals the circumferential speed. Professor Lewin derived an equation for the acceleration of an object rolling down a ramp (under pure roll conditions). For solid cylinders with uniform mass density, this acceleration is independent of the mass and radius of these cylinders (this is rather non-intuitive). However, the acceleration is higher for a solid cylinder than it is for a hollow cylinder. This is demonstrated.

2. Applying Torque to a Spinning Wheel:

When you apply a torque to a fast spinning wheel, it moves the spin angular momentum in the direction of the torque (torque is a vector). This is called precession. This very non-intuitive concept is demonstrated with a bicycle wheel.

3. Precession of a Flywheel:

The bizarre behavior of a spinning flywheel that experiences a torque due to gravity is explored. Professor Lewin demonstrates this by suspending the axle of a fast rotating bicycle wheel from a rope. By increasing the torque, the precession frequency increases. The direction of precession can be reversed if the direction of rotation of the bicycle wheel is reversed. You can also observe this very non-intuitive behavior with a toy gyroscope.

4. Mysterious Suitcase:

A suitcase is brought in that requires special handling. There is a fast rotating flywheel inside! A student volunteers to carry the suitcase around. The suitcase behaves in a weird manner as the student turns around.

5. Gyroscope in Gimbals:

A spinning object, e.g. a coin on edge, is more stable against falling over than when it isn't spinning. This concept is used in mechanical inertial guidance systems, where a spinning wheel is mounted in gimbals to prevent torques to the axis of the wheel. Professor Lewin walks through the lecture hall with such a 3-axis gimballed gyroscope. The direction of the axis of rotation of the spinning flywheel does not change as he moves around.

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1 ARIHANT, October 22, 2008 at 1:38 p.m.:

Nicely demonstrated

2 tvgupta, July 29, 2010 at 3:05 p.m.:

Our minds are conditioned with respect to gravity. But the resultant moment of inertia has a different ball game in space where there are no external forces.

3 Badri!, November 8, 2010 at 4:48 a.m.:

Your demonstrations improved my uunderstanding of the concept of precession better. Nice job, Professor Lewin!

4 manikanth, August 3, 2012 at 2:11 p.m.:

conceptual and easy to understand

5 Gassn lahham, October 4, 2012 at 7:14 p.m.:

yes very wendrfull

6 Utkarsh, June 6, 2013 at 4:36 p.m.:

Lovely video... however could somebody explain to me why in the experiment performed at the 23:10 mark, does the stool Walter Lewin is seated on start rotating? I know it has to do with conservation of angular momentum but as I draw the vector arrows for torque and spin angular momentum I still can't put together why the stool rotates in the direction that it does. A clear picture of what's happening would be nice

7 akshaya jalasteen, March 8, 2015 at 4:57 a.m.:

thank you sir

8 Davor form VideoLectures, December 18, 2017 at 10:33 a.m.:

Hi all!

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