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Chapter 6 Experiment 4: Conservation of Energy
Chapter 6 Experiment 4: Conservation of Energy

... development of classical and analytic mechanics by early luminaries such as JosephLouis Lagrange (1736-1813) and William Rowan Hamilton (1805-1865). Scalar quantities are often much easier to work with than vectors, and the concepts of mechanics using scalars implied by the Work-Energy theorem trans ...
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Work, Energy, and Power Packet

... Background and Theory: There are several ways that the motion of objects can be analyzed. One way is by using kinematic equations and the idea of independence of horizontal and vertical components of the motion. Another way is by using the Law of Conservation of Mechanical Energy. In this laboratory ...
Psc CH-10 Work_ Energy_ _ Machines
Psc CH-10 Work_ Energy_ _ Machines

... A 100.0 cm handle is connected to 5.0 cm wheel with teeth connecting it to another 50.0 cm wheel connected to a 2.5 cm axle. A cable is connected to the axle. The efficiency of this system is 90.0 %. Calculate IMA & MA ...
blackboard course
blackboard course

... acceleration are not constant. In this case, the Newton’s laws of motion actually become the differential equations and their solution becomes not so simple as before. But more important is following problem. Using this approach that is called force approach, we need to know force at any instant of ...
Gravitational Potential Energy
Gravitational Potential Energy

... When only the force of gravity does work on a system, the total mechanical energy of that system is conserved. This is an example of the conservation of mechanical energy. Figure 7.3 below illustrates this. ...
CP Physics – Midterm Review
CP Physics – Midterm Review

Energy
Energy

... it cannot be created or destroyed. This means that all the energy in a system before some event must be accounted for m afterwards. For example, suppose a mass is dropped from some height. The gravitational potential energy it had originally is not destroyed. Rather it is converted into kinetic ener ...
ENERGY OF A TOSSED BALL LAB WHS PHYSICS objectives
ENERGY OF A TOSSED BALL LAB WHS PHYSICS objectives

Energy of a Tossed Ball
Energy of a Tossed Ball

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Chapter 11 Clickers
Chapter 11 Clickers

... both ends. The radius of the cylinder is r. At what angular speed  must the this cylinder rotate to have the same total kinetic energy that it would have if it were moving horizontally with a speed v without rotation? v2 a)   2r ...
Potential Energy - ShareStudies.com
Potential Energy - ShareStudies.com

Chapter 11
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... does not take very much force to change the motion of a baseball. It takes much more force to change the motion of a bowling ball. The bowling ball resists changes in motion more than the baseball does. The tendency of an object to resist changes in motion is called inertia. All objects have inertia ...
Lecture PowerPoints Chapter 6 Physics: Principles with Applications
Lecture PowerPoints Chapter 6 Physics: Principles with Applications

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Multiple Choice

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3.6MB Word - Clydeview Academy

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OVERVIEW

... The goal of a physics experiment is to determine how two sets of measurements are related to each other. In some physics experiments, you do not have clearly defined independent and dependent variables. Instead, your focus is in understanding the two things you are measuring and why you need to meas ...
CfE Advanced Higher Physics – Unit 1 – Rotational Motion
CfE Advanced Higher Physics – Unit 1 – Rotational Motion

File - Mr. Walsh
File - Mr. Walsh

... until the beaker is about 2 cm from the edge of the table and then quickly jerk the cloth out from under the beaker. The beaker should remain on the table, and no water should spill. As one gains confidence, the demonstration can be done with other objects such as an entire table setting, but it's e ...
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tri-quarterly practice answers

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4. Work-Energy

... The net work done on the glider will be calculated from the net force acting on the glider and the distance it moved between the two positions. II. THEORY Work Done by a Constant Force Consider an air track glider of mass M connected to a hanging mass m by a string which goes over a smooth pulley at ...
Linear motion topics  1 A
Linear motion topics 1 A

Energy
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... • Potential Energy: energy that is stored and held in readiness to do work. • Any substance that can do work has potential energy. – Fossil Fuels – Electric Batteries – Food ...
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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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