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Lec 12 | 8.01 Physics I: Classical Mechanics, Fall 1999

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Uploaded by on Jan 14, 2008

Non-Conservative Forces - Resistive Forces - Air Drag - Terminal Velocity

View the complete course: http://ocw.mit.edu/8-01F99

License: Creative Commons BY-NC-SA
More information at http://ocw.mit.edu/terms
More courses at http://ocw.mit.edu

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  • Whatever i do for professor walter lewin it will not be enough to thank him in any way his way of teaching is revolutionary. I really wish that i meet him someday.

  • AWESOME!! =D

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All Comments (59)

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  • is this really mit stuff because i am barely in high school

  • I looked up parabolas and got this

  • REALY AA PEEERRRFEECTT PPHHYYSSIICCSS TTEEAACCHHEERR

  • AMAZINGGGGGGGGGGGGGGGGGGGGGGGG­­GG!!!!!!!!

  • My Respects

  • Before watching this video, I thought that the force of air resistance is proportional to the velocity, and it followed the equation F=bv, where b is some constant. Wouldn't that mean that air is in Regime I?

  • this is why its MIT..............

  • wait..so is it longer or shorter?

  • how is it possible to cross from regime 1 into regime 2? Is the force of gravity not enough to break the barrier? Would more force be needed to apply to cross the barrier? How would the graph look once if crossed from regime 1 to regime 2?

  • i learned alot more by watching this, than my prof trying to teach...

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