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Changing momentum: curving motion

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Presentation on theme: "Changing momentum: curving motion"— Presentation transcript:

1 Changing momentum: curving motion
Parallel component (Along trajectory) Rate of change of direction Perpendicular component (to trajectory) Remind – p is a function of time, and both |p| and p^ may also depend on time. Direction of motion in point A A

2 Rate of change of direction
Length of path A = vt Similar triangles Angle = For small angle: Direction: For small angles is perpendicular to This is now done in the same order and the same way as in new (black) version of the book is directed toward the center of the kissing circle - Normal to the path toward center of the “kissing” circle

3 The Momentum Principle for components
A Direction of motion in point A Parallel component: Perpendicular component:

4 The Momentum Principle for components
A Direction of motion in point A Parallel component: Perpendicular component: Discuss briefly: The magnitude is changed only if there is a force component along path The direction is changed only if there is force component perpendicular to path Rate of change of magnitude p Rate of change of direction of p

5 Example: the Moon and the Earth
Mass of the Moon: mM = 7×1022 kg Distance from the Earth: R = 4×108 m Period: T = 28 days Question: = ? R Solution: mM Parallel: =0 Perpendicular: What is the direction of ?

6 Example: the Moon and the Earth
Mass of the Moon: mm = 7×1022 kg Distance from the Earth: R = 4×108 m Period: T = 28 days Mass of the Earth: mE = 6×1024 kg Question: FEarth on M=? R mE mM Solution: From motion path: Discuss the fact that following motion we can determine dp/dt, and if we know dp/dt we know that there was interaction and we can deduce what was the force. However, nature of the interaction (force) does not matter. And vice versa – if we know force we can predict motion. any force motion of any object these are not the same things! This is precise – works at any speed!


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