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SC81 Physics Curriculum Map 2010/2011 Revised 7/29/2010
SC81 Physics Curriculum Map 2010/2011 Revised 7/29/2010

... 2. Calculate the magnitude of centripetal force and centripetal acceleration for an object in circular motion. S5 C2 PO 11 1. Predict how the force will change between two masses when the distance between them increases or decreases. Predict how the force will change between two masses when the mass ...
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HW 4 solutions

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Lecture 13

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Lecture 10.DragForce.. - Faculty Web Sites at the University of Virginia

... longer a force to keep it going in a circle. Therefore, it simply continues in a straight line, as Newton’s First Law ...
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Chapter 4: Fundamental Forces Newton`s Second Law: F=ma In

Sample Unit – Physics – Year 11
Sample Unit – Physics – Year 11

The ball rolls up the ramp, then back down. Let +x direction be up
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ICNS 132 : Work, Energy and Power

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Simple Harmonic Motion

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Physics and Beyond PowerPoint

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AP Physics Laws of Motion MC Sample Test

... III. Inertia is a consequence of having mass. IV. It changes with the strength of gravity g. (A) I only. (B) II only. (C) I and II. (D) I and III. (E) All of these are true for mass. ...
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item[`#file`]->filename - Open Michigan

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File - Malone Science . com

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Ch 6 Newton`s Third Law Summary

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Go over midterm, Springs

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Vectors and Scalars

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forces and newton`s laws of motion

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chapter 4 - forces and newton`s laws of motion

... direction. The converse is also true. If an object maintains a constant velocity, then it is in equilibrium. The equations for equilibrium are: ...
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Laws of Motion Notes

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Note that in the following three figures, which show
Note that in the following three figures, which show

< 1 ... 414 415 416 417 418 419 420 421 422 ... 642 >

Classical central-force problem



In classical mechanics, the central-force problem is to determine the motion of a particle under the influence of a single central force. A central force is a force that points from the particle directly towards (or directly away from) a fixed point in space, the center, and whose magnitude only depends on the distance of the object to the center. In many important cases, the problem can be solved analytically, i.e., in terms of well-studied functions such as trigonometric functions.The solution of this problem is important to classical physics, since many naturally occurring forces are central. Examples include gravity and electromagnetism as described by Newton's law of universal gravitation and Coulomb's law, respectively. The problem is also important because some more complicated problems in classical physics (such as the two-body problem with forces along the line connecting the two bodies) can be reduced to a central-force problem. Finally, the solution to the central-force problem often makes a good initial approximation of the true motion, as in calculating the motion of the planets in the Solar System.
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