(10) Applying Newton's Laws

# (10) Applying Newton's Laws - Lecture 10 Applying Newton's...

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Lecture 10 Applying Newton’s Laws

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ACT: Bowling on the Moon An astronaut on Earth kicks a bowling ball horizontally and hurts his foot. A year later, the same astronaut kicks a bowling ball on the moon with the same force. His foot hurts: A. More B. Less C. The same Ouch ! F B,A F A,B
Movie from Apollo 17

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String Theory” Tension: magnitude of the force acting across a cross-section of the rope/ string/ cable at a given position (it’s the force you would measure if you cut the rope and grabbed the ends).
Consider a segment with mass m of a rope with an acceleration a to the right. If we neglect gravity, the forces on the segment are: m a T 1 T 2 2 1 2 1 T T ma T T - = 2 1 2 1 I f 0, 0 m T T T T = - = = (also, then the weight of the segment really is negligible) We’ll assume ideal (constant length), massless strings (i.e, mass much smaller than the rest of the masses in the system).

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T T Massless string: The tension is the same throughout the string. It can only pull in the direction of its length. Constant length string: All objects attached to it move together (same acceleration and velocity) This makes our lives a lot easier (and it is a good approximation most of the time).
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## This note was uploaded on 03/27/2008 for the course PHYS 221 taught by Professor Herrera-siklody during the Fall '08 term at Iowa State.

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(10) Applying Newton's Laws - Lecture 10 Applying Newton's...

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