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energy - TeacherWeb
energy - TeacherWeb

... velocity. Which ball will roll more forcefully? • You would have to exert a greater force on the bowling ball because it has more mass than the golf ball. • Since energy is transferred during work, the more work you do, the more energy you give to the ball. • So the bowling ball has more kinetic ene ...
Force and Acceleration in Circular Motion
Force and Acceleration in Circular Motion

Conservation of Energy
Conservation of Energy

Grade 11 Physics – Homework 5 1. A skydiver of mass 80 kg falls
Grade 11 Physics – Homework 5 1. A skydiver of mass 80 kg falls

peden (jp5559) – Simple Harmonic Motion – peden
peden (jp5559) – Simple Harmonic Motion – peden

Newton`s Second Law (without friction)
Newton`s Second Law (without friction)

5. Forces and Motion-I Newton's First Law:
5. Forces and Motion-I Newton's First Law:

... P Newton's Law is valid only in an inertial reference frame, a frame that is not accelerating, e.g. a powerless spacecraft far away from all planets (good example) or close to the surface of the Earth (good approximation). Any frame that ...
Newton`s Second Law (without friction)
Newton`s Second Law (without friction)

... THEORY: One of the fundamental laws of nature is that forces do NOT cause motion, , but rather that forces cause changes in motion (accelerations), ...
-Energy of SHM -Comparing SHM to Circular Motion
-Energy of SHM -Comparing SHM to Circular Motion

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Chapter 05

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Question #1. 1. A tennis ball of mass m = 0.080 kg and speed v = 45
Question #1. 1. A tennis ball of mass m = 0.080 kg and speed v = 45

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2nd 9 weeks

... I can describe the forces acting on an object undergoing horizontal rotational motion. Note: Forces acting on an object in vertical rotational motion are best analyzed using calculus, at an Honors but not Standard level. I can calculate torque given perpendicular force and lever arm. I can calculate ...
Force and Acceleration
Force and Acceleration

... always seem to support this. For example, when you are driving a car, you must apply a constant force to keep the car moving with a constant velocity. In the absence of friction, the car would continue to move with a constant velocity after the force was removed. The continued application of force w ...
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Momentum - Northern Highlands

Physics TAKS Review
Physics TAKS Review

... This is because no machine can perfectly transfer your input work to the output side of the machine. There is always some loss of energy as thermal energy. If you think about it, it kind of makes sense. When have you ever gotten as much out of something as you put into it. However, The extra energy ...
Lecture 18
Lecture 18

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3.5 Application-Spring Mass Systems (Unforced Systems with Friction)

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Homework - Ryan, Susan

... AP Physics C - Force: Drag Problems ...
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Ch.4 Forces

... Forces - vector quantity that changes the velocity vector of an object. When you hit a baseball, the velocity of the ball changes. Can be a push or a pull on an object Contact forces – result from physical contact with an object (pulling a trailer, friction forces, normal force) Field forces – inter ...
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3 inertia newtons fi..

... because of its inertia (until the back of the seat applies a forward force to make it move with the bus). From the point of view of someone on the bus, it appears that the package is moving backward; however, someone watching from outside the bus would see the bus move forward and the package trying ...
Chapter4.2 - Department of Physics & Astronomy
Chapter4.2 - Department of Physics & Astronomy

1 Ch. 3: Newton on gravity and motion 3.1: Newton`s
1 Ch. 3: Newton on gravity and motion 3.1: Newton`s

... square of the radius of the surface. If the totality of the light is, in some sense, conserved, then the intensity of the light at any point of the surface must decrease as the inverse square of the radius, i.e., like 1 / (distance)2 ! This was the basis for expecting the acceleration to depend on d ...
sy16_oct26_f11a
sy16_oct26_f11a

... How much will the spring compress (i.e. x = xf - xi) to bring the box to a stop (i.e., v = 0 ) if the object is moving initially at a constant velocity (vo) on frictionless surface as shown below ? x Wbox  F ( x ) dx ...
Q1. A baby bouncer consisting of a harness and elastic ropes is
Q1. A baby bouncer consisting of a harness and elastic ropes is

Tutorial_07_HW_Sol - UMD Physics
Tutorial_07_HW_Sol - UMD Physics

... Work depends on both force and distance: Wprof on cart = Fprof on cart∆x. Along path 1, the professor pushes the cart for less distance (as noted in part A), but he exerts a greater force, since he’s fighting gravity head-on (as noted in part B). By contrast, along path 2, the professor pushes with ...
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Relativistic mechanics

In physics, relativistic mechanics refers to mechanics compatible with special relativity (SR) and general relativity (GR). It provides a non-quantum mechanical description of a system of particles, or of a fluid, in cases where the velocities of moving objects are comparable to the speed of light c. As a result, classical mechanics is extended correctly to particles traveling at high velocities and energies, and provides a consistent inclusion of electromagnetism with the mechanics of particles. This was not possible in Galilean relativity, where it would be permitted for particles and light to travel at any speed, including faster than light. The foundations of relativistic mechanics are the postulates of special relativity and general relativity. The unification of SR with quantum mechanics is relativistic quantum mechanics, while attempts for that of GR is quantum gravity, an unsolved problem in physics.As with classical mechanics, the subject can be divided into ""kinematics""; the description of motion by specifying positions, velocities and accelerations, and ""dynamics""; a full description by considering energies, momenta, and angular momenta and their conservation laws, and forces acting on particles or exerted by particles. There is however a subtlety; what appears to be ""moving"" and what is ""at rest""—which is termed by ""statics"" in classical mechanics—depends on the relative motion of observers who measure in frames of reference.Although some definitions and concepts from classical mechanics do carry over to SR, such as force as the time derivative of momentum (Newton's second law), the work done by a particle as the line integral of force exerted on the particle along a path, and power as the time derivative of work done, there are a number of significant modifications to the remaining definitions and formulae. SR states that motion is relative and the laws of physics are the same for all experimenters irrespective of their inertial reference frames. In addition to modifying notions of space and time, SR forces one to reconsider the concepts of mass, momentum, and energy all of which are important constructs in Newtonian mechanics. SR shows that these concepts are all different aspects of the same physical quantity in much the same way that it shows space and time to be interrelated. Consequently, another modification is the concept of the center of mass of a system, which is straightforward to define in classical mechanics but much less obvious in relativity - see relativistic center of mass for details.The equations become more complicated in the more familiar three-dimensional vector calculus formalism, due to the nonlinearity in the Lorentz factor, which accurately accounts for relativistic velocity dependence and the speed limit of all particles and fields. However, they have a simpler and elegant form in four-dimensional spacetime, which includes flat Minkowski space (SR) and curved spacetime (GR), because three-dimensional vectors derived from space and scalars derived from time can be collected into four vectors, or four-dimensional tensors. However, the six component angular momentum tensor is sometimes called a bivector because in the 3D viewpoint it is two vectors (one of these, the conventional angular momentum, being an axial vector).
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