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Thursday, Sept. 18, 2014
Thursday, Sept. 18, 2014

Lecture 8 - Columbia Math Department
Lecture 8 - Columbia Math Department

Chapter 6 The Gravitational Force and the Gravitational Field
Chapter 6 The Gravitational Force and the Gravitational Field

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Ch15

... Variations of K and U can also be observed with respect to position. The energy is continually being transformed between potential energy stored in the spring and the kinetic energy of the block. The total energy remains the same ...
Chapter1
Chapter1

Chapter 7
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... Planets move in elliptical orbits with Sun at one of the focal points. Line drawn from Sun to planet sweeps out equal areas in equal times. The square of the orbital period of any planet is proportional to cube of the average distance from the Sun to the planet. ...
Ch 7 Kinetic Energy and Work
Ch 7 Kinetic Energy and Work

... U.S. unit of power is horsepower 1 hp = 746 W For electric power generation/usage, use the kilowatt-hour. This is the energy transferred in 1hr at the rate of 1kW (1000 J/s). 1kWh = (1000J/s)(3600s) = 3.6x106J ...
Rotational Dynamics II
Rotational Dynamics II

Exam #: Printed Name: Signature: PHYSICS DEPARTMENT
Exam #: Printed Name: Signature: PHYSICS DEPARTMENT

... Two weights, each with mass m, are connected with a massless string and suspended from two massless, frictionless pulleys in a gravitational field as shown above. Denote the length of string from pulley A to mass A by x. The length of string from pulley B to mass B is L − x, where L is fixed by the ...
Slide 1 - Phy 2048-0002
Slide 1 - Phy 2048-0002

... speed of light Einstein’s special theory of relativity. 2) The interacting bodies are on the scale of the atomic structure  Quantum mechanics I. Newton’s first law: If no net force acts on a body, then the body’s velocity cannot change; the body cannot accelerate  v = constant in magnitude and di ...
Chapter 1
Chapter 1

Physics 140 HOMEWORK Chapter 10B Q7. Figure 10
Physics 140 HOMEWORK Chapter 10B Q7. Figure 10

... Newton’s second law with rotation. XFBD for double-pulley (“device”): T downward at r on right; Fappl at top at R to left; n at com upward; mdevice g downward at com. ~a = 0. α CCW. FBD for box: T upward; mg down. ~a = 0.8 m/s2 upward. Make +x upward. Eq for box: T − mg = ma ⇒ T = m(g + a) = (30 kg) ...
2.2 Biomechanics - Force - NCEA-Physical
2.2 Biomechanics - Force - NCEA-Physical

... • For every action there is an equal an opposite reaction ...
Student notes Chap 1 & 2
Student notes Chap 1 & 2

... km/h to zero in 0.1 s is equal to 14 times the force that gravity exerts on the person • belt loosens a little as it restrains the person, increasing the time it takes to slow the person down • this reduces force exerted on the person • safety belt also prevents the person from being thrown out of t ...
Example: I take an object of mass m = 1 kg and raise it to the height
Example: I take an object of mass m = 1 kg and raise it to the height

Vocabulary Chapter 3: Newton`s Second Law of Motion
Vocabulary Chapter 3: Newton`s Second Law of Motion

Energy Conservation
Energy Conservation

... time trial stage was a steep climb with its finish 1200 m higher than the start. Lance Armstrong won with a time Dt of 39:41 (2381 s). He and his gear had a combined mass of 84 kg. What was Lance’s average power DE/Dt during the stage? Hint: Use change in gravitational potential energy for DE. ...
Living Things - Christian Heritage School
Living Things - Christian Heritage School

... Unbalanced Forces Unbalanced forces acting on an object result in a net force and cause a change in the object’s motion. ...
HW6.1 – This is a lot of work!
HW6.1 – This is a lot of work!

2009 Final Exam
2009 Final Exam

... Newton’s First Law Newton’s Second Law Newton’s Third Law Newton’s Law of Universal Gravitation ...
SCI 101 - Onondaga Community College
SCI 101 - Onondaga Community College

... 14) A cannonball is fired straight up at 50 m/s. Neglecting air resistance, when it returns to its starting point its speed A) is 50 m/s. C) is less than 50 m/s. B) is more than 50 m/s. D) depends on how long it is in the air. ...
ch10_shm_16slides
ch10_shm_16slides

Conservation of Momentum
Conservation of Momentum

Chapter 10 Homework and Practice Problems 10.1, 10.10, 10.17
Chapter 10 Homework and Practice Problems 10.1, 10.10, 10.17

Semester 1 Review
Semester 1 Review

... Define work and calculate the work done by a force. Identify where work is being performed in a variety of situations. Calculate the net work on an object, when many forces act upon it. Calculate the kinetic energy for an object. Apply the work-energy theorem to solve problems. Distinguish between t ...
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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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