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Unit Objectives: At the completion of this unit, you should be able to
Unit Objectives: At the completion of this unit, you should be able to

... o Given the potential energy function U(x) for a one-dimensional force, calculate the magnitude and direction of force o Write an expression for the force exerted by an ideal spring and for the potential energy stored in a compressed or stretched spring o State the generalized work-energy theorem an ...
Centripetal acceleration
Centripetal acceleration

... The small subscript c specifies that this is a centripetal acceleration. It is called this because centripetal means “center-seeking”. If you look back at the velocity vector diagram, the change in velocity vector points down and to the left, anti-parallel to the s2 vector. The s2 vector is pointin ...
CT8b
CT8b

... bottom of hill (before puck hits rug) = (1/2)m2 = heat generated by friction as puck slows and stops = magnitude of work done by friction = Wfric  K N x  K mg x . So we have the equation mgh = Kmgx or h = Kx = x (since K=1). ...
Introduction to Forces Guided Discussion ppt
Introduction to Forces Guided Discussion ppt

ROTATION
ROTATION

Ex. 1 - Mr. Schroeder
Ex. 1 - Mr. Schroeder

... Both you (the dot) and the car (the box) are originally moving with the same velocity (red vector), together. The force that made the body of the car turn has not acted on you. Your body’s tendency is to keep moving in its original direction. With respect to the car, it seems you are pushed left. ...
∑ ∑ ∑ - Mr. Tiesler`s Physics Page!
∑ ∑ ∑ - Mr. Tiesler`s Physics Page!

on that object
on that object

Standard - Peak to Peak Charter School
Standard - Peak to Peak Charter School

Honors - Peak to Peak Charter School
Honors - Peak to Peak Charter School

Unit 1 B
Unit 1 B

ME2 – MECHANICAL COMPONENTS
ME2 – MECHANICAL COMPONENTS

Sir Isaac Newton Laws of Motion
Sir Isaac Newton Laws of Motion

Force and Motion. Gravitation.
Force and Motion. Gravitation.

Sir Isaac Newton Laws of Motion
Sir Isaac Newton Laws of Motion

... Is an example of Newton’s 1st Law when a car turns left and you appear to slide to the right? ...
Friday PS Forces Part 2 - elyceum-beta
Friday PS Forces Part 2 - elyceum-beta

... • The resistance of an object to change of motion • The more massive an object, the more inertia it possesses ...
L2 Slides - University of Brighton
L2 Slides - University of Brighton

TAKE OUT SWING EXAMPLE IF DOING PIG LAB
TAKE OUT SWING EXAMPLE IF DOING PIG LAB

... Newton reasoned that if you fired a projectile fast enough horizontally, it would continually fall from its straight-line path but never hit the earth…”falling around” or orbiting the earth. ...
Force and Motion
Force and Motion

Like-charged particles at liquid interfaces
Like-charged particles at liquid interfaces

Section 2: Gravity
Section 2: Gravity

... ▪ All objects, regardless of their mass, accelerate at the same rate when they are in free fall. Why? Newton’s 2nd Law of Motion explains it: an object’s acceleration increases if the force on it increases, but its acceleration decreases if its mass increases. So, the more massive an object is, the ...
Newton`s Laws PPT
Newton`s Laws PPT

... An object at rest will stay at rest, and an object in motion will stay in motion at constant velocity, unless acted upon by an unbalanced force. This a short video clip that demonstrates this law. ...
Newton`s Laws - Industrial ISD
Newton`s Laws - Industrial ISD

... Natural – objects on Earth seek natural resting place, such a boulder rolling downhill; the planets and stars Violent – imposed motion (external cause), such as that which makes a cart move, pulling on a rope, wind pushing a ship ...
Newton*s Laws - Lindbergh School District
Newton*s Laws - Lindbergh School District

... An object in motion tends to stay in motion with a constant velocity and an object at rest tends to stay at rest unless acted upon by a net force. So what does that mean?... ...
1. A skydiver of mass 80 kg falls vertically with a constant
1. A skydiver of mass 80 kg falls vertically with a constant

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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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