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Physics 106P: Lecture 1 Notes
Physics 106P: Lecture 1 Notes

... You are towing a car up a hill with constant velocity. The work done on the car by the gravitational force is: ...
Part I
Part I

... Newton’s First Law • 1st Law: (“Law of Inertia”): “In the absence of external forces and when viewed from an inertial reference frame, an object at rest remains at rest and an object in motion remains in motion with a constant velocity (constant speed in a straight line).” Sir Isaac Newton  as an ...
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... where we set L1  1000 m in the last step. Thus, if L1 and L2 are no different than about 1.4 m, then runner 1 is indeed faster than runner 2. However, if L1 is shorter than L2 by more than 1.4 m, then runner 2 would actually be faster. 13. We use Eq. 2-2 for average velocity and Eq. 2-4 for instant ...
Ch 8 Dynamics II Review Problems
Ch 8 Dynamics II Review Problems

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Physics Talk 2.3

...  LO/SC  Physics Talk  PTG ...
Newton’s Laws of Motion
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... watch it slide to a rest position. The book comes to a rest because of the presence of a force that force being the force of friction which brings the book to a rest position. ...
In the case of zero total energy, E = 0 , the orbit is parabolic. Since
In the case of zero total energy, E = 0 , the orbit is parabolic. Since

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Slide 1

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... Newton's second law states that "Force equals mass times acceleration (F = ma)": the net force on an object is equal to the mass of the object multiplied by its acceleration A skydiver needs this equation to figure out when he's gonna hit the ground and when to pull the parachute. The skydiver can f ...
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...  First law describes how an object moves when the net force acting on it is zero  First law states that an object at rest will remain at rest, or an object in motion will continue in motion unless an outside force acts on it. This occurs when a balanced force is applied  Inertia is an example of ...
Physics 144 (section 1) Homework 4
Physics 144 (section 1) Homework 4

... (b) Find
the
magnitude
of
the
total
momentum
of
the
system
from
the
given
data.
 (c) Find
the
speed
of
he
center
of
mass
of
the
system.
 (d) Find
the
total
momentum
of
the
system
using
the
speed
of
the
center
of
mass.

 Compare
to
your
results
in
part
(b)
and
comment.
 ...
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Chapter 20 Concept Tests - University of Colorado Boulder
Chapter 20 Concept Tests - University of Colorado Boulder

... the B-field is up, and the forces cancel. But if charge is negative, both forces switch direction and the forces still cancel. In either case, the fact that the particles is moving with constant velocity implies that Fnet = 0. Since the net force is zero, the magnetic force (magnitude |q|vB) must ca ...
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... in a horizontal circle of radius 20 cm. a. Find the tension is the string and b. the angular speed of the ball in rpm. Analysis: The mass moves in a horizontal circle of radius The acceleration and the net force vector point to the center of the circle, not along the string. The only two forces are ...
Unit 6 notes - Killeen ISD
Unit 6 notes - Killeen ISD

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CCA Review - Net Start Class

... 12. Which of the following best describes the force when an elevator car moves downward with a constant velocity? Circle the correct answer. A. the FT is greater B. the FW is greater C. the FT equals the FW 13. A crate has a weight of 56 N. What is the mass of the crate? 14. To accelerate at 300 m/s ...
Lecture Notes - Flipping Physics
Lecture Notes - Flipping Physics

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Physics 101: Lecture 12 Work and Energy

... ÎThermodynamics (movement of heat) ÎQuantum mechanics... Very useful tools ÎYou will learn new (sometimes much easier) ways to solve problems ...
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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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