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Motion With Constant Acceleration
Motion With Constant Acceleration

... wait about a half second, and let the cart go. The computer will record data until you hit . You should wait 3 or 4 seconds after the cart stops moving before hitting ...
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Document

... A surface wave generated by an earthquake was recorded at Seismic Station 1. Forty seconds later the same wave was recorded at Seismic Station 2. What accounts for the time difference? A.The origin of the wave is closer to Seismic Station 1. B.The speed of the wave decreases with distance. C.The wav ...
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Chapter 11

AP Physics 1
AP Physics 1

... The student is able to plan data collection strategies designed to investigate torque, angular velocity, angular acceleration, and angular momentum. [SP 3.2, 4.1, 4.2, 5.1, 5.3] The student is able to use appropriate models and mathematical routines to calculate values for initial or final angular m ...
First integrals. Reduction. The 2-body problem.
First integrals. Reduction. The 2-body problem.

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Chapter 4 Lagrangian mechanics

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forces christina danielle ali
forces christina danielle ali

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Chapter 8—Conservation of Energy MULTIPLE CHOICE 1. A single

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... calculus, a very important mathematical tool in science. He extended Galileo’s work and developed the three fundamental laws of motion. He also formulated a theory of the nature of light and showed, using prisms, that white light is composed of all colors of the rainbow. It was his experiments with ...
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... no balls are gained. Such a system, which does not gain or lose mass, is said to be a closed system. The second condition is that the forces involved are internal forces; that is, there are no forces acting on the system by objects outside of it. When the net external force on a closed system is zer ...
Example 1 - UCSB Campus Learning Assistance Services
Example 1 - UCSB Campus Learning Assistance Services

... A 0.260kg mass is attached to a vertical spring. When the mass is put into motion, its period is 1.12sec. How much does the mass stretch the spring when it is at rest in its equilibrium position? ...
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Physics 6B - UCSB C.L.A.S.

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SFU Phys101 Summer 2013 ( MPCHEN69716 )

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... A rubber band obeys the force law F = -kx - cx 4. Assume that x = 0 for one end of the unstretched rubber band. If this end is stretched from x 1 to x 2 (x 1 and x 2 are both greater than zero) calculate the work done on the rubber band. The potential energy as a function of position for an object o ...
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EXPERIMENT 1- Measurements and Accuracy
EXPERIMENT 1- Measurements and Accuracy

... Method 2: The initial velocity Vo of the projectile can also be determined by using the ballistic pendulum (Fig 2). It consists of a spring gun that fires a metallic ball of mass m which is caught by a catcher at the end of a pendulum of mass M. The collision between the ball and pendulum is perfect ...
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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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