Lecture 11: Work - Kinetic Energy - Potential Energy - Conservative Forces - Conservation of Mechanical Energy - Newton's Law of Universal Gravitation

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: October 1999,   views: 20236
released under terms of: Creative Commons Attribution Non-Commercial Share Alike (CC-BY-NC-SA)

See Also:

Download Video - generic video source Download mit801f99_lewin_lec11_01.m4v (Video - generic video source 105.7 MB)

Download Video - generic video source Download mit801f99_lewin_lec11_01.rm (Video - generic video source 107.2 MB)

Download Video Download mit801f99_lewin_lec11_01.flv (Video 106.6 MB)

Download Video Download mit801f99_lewin_lec11_01.wmv (Video 433.5 MB)

Download subtitles Download subtitles: TT/XML, RT, SRT


Help icon Streaming Video Help

Related content

Report a problem or upload files

If you have found a problem with this lecture or would like to send us extra material, articles, exercises, etc., please use our ticket system to describe your request and upload the data.
Enter your e-mail into the 'Cc' field, and we will keep you updated with your request's status.
Lecture popularity: You need to login to cast your vote.
  Bibliography

Description

>>PLEASE TAKE A QUICK SURVEY<<

1. 1D Work and Kinetic Energy:

The equation for work, and its units are introduced. The work-energy theorem is derived showing that the change in kinetic energy equals the work done on a particle by the sum of all forces (thus the net force). Gravity does negative work on an object thrown upwards until it reaches its maximum height of its trajectory.

2. Work Calculated in 3-Dimensions:

Work in 3D is shown to decompose into the sum of each 1D component.

3. Gravity is a Conservative Force:

Work done by gravity while a particle moves upwards a vertical distance h is -mgh, regardless of the path taken. When the work done by a force is independent of the path, that force is called a conservative force.

4. When Gravity is the only Force:

The equation for gravitational potential energy is introduced by rearranging the work-energy theorem. Potential energy and kinetic energy can be converted back and forth but their sum, the mechanical energy, is conserved if only conservative forces are involved. Friction is not a conservative force. When friction is at stake, the work-energy theorem can be applied, but mechanical energy is not conserved.

5. What Matters is the Difference in Potential Energy:

Gravitational potential energy can be positive, negative or zero depending on your choice of origin. It really doesn't matter where you choose the origin.

6. A Roller Coaster, Upside-down:

The conservation of mechanical energy is used to analyze the velocity of an object on a roller coaster. The centripetal acceleration, when the roller coaster is upside down, must be greater than g; the mechanical energy must therefore exceed a threshold value.

7. Newton's Law of Universal Gravitation:

Newton's law of universal gravitation is introduced. The gravitational force falls off as one over the distance squared. If large distances are involved, the gravitational potential due to an object of mass M is taken to be zero at infinity. The gravitational potential is proportional to M and inversely proportional to the distance from M. This formalism is consistent with the small distance approximation used near the Earth's surface.

8. Conservation of Mechanical Energy and a Wrecking Ball:

A wrecking ball is converting gravitational potential energy into kinetic energy and back and forth. If released with zero speed, the wrecking ball should NOT swing higher than its height when it was released. Professor Lewin puts his life on the line by demonstrating this.

Link this page

Would you like to put a link to this lecture on your homepage?
Go ahead! Copy the HTML snippet !

Reviews and comments:

Comment1 jtl, May 8, 2009 at 11:10 p.m.:

this guy rulez...


Comment2 Vanessa, May 6, 2012 at 3:38 a.m.:

What if there is a resistance act on the object when it is sliding downward on the inclined horizontal


Comment3 wahidullah, May 8, 2014 at 8:24 a.m.:

this lectures are very useful for me


Comment4 Davor form VideoLectures, December 18, 2017 at 10:27 a.m.:

Hi all!

We have translated this entire course for you from English into 11 languages.

Check this video and give us some feedback in this short survey https://www.surveymonkey.co.uk/r/6DMBC3Q

Write your own review or comment:

make sure you have javascript enabled or clear this field: