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Lab 2 Force and Acceleration

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d - mazarelloscience.com

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... consider he is at a state of rest in a place with no gravitational field. Einstein then considered the force producing an acceleration on a mass, m (the inertial mass), F = ma, and the acceleration due to gravity on this same mass (its gravitational mass), W = mg. Einstein concluded that inertial ma ...
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7. conservation of momentum - essie-uf

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... 17. A model airplane has mass of 0.90 Kg and moves on a 17m guideline at constant speed in a circle that is parallel to the ground. Find the tension in the guideline for speeds of 19m/s and 38 m/s. (19.11 N, 76.45 N) 18. An athlete swings a 5 kg ball horizontally on the end of an 0.8 m long rope. Th ...
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Potential energy

... • By the work-energy theorem, the change in an object’s kinetic energy equals the net work done on the object: ∆K = Wnet • When only conservative forces act, the net work is the negative of the potential-energy change: Wnet = –∆U • Therefore when only conservative forces act, any change in potential ...
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... and one where the quantity is conserved. Represent each scenario with a conservation bar chart. Write a mathematical expression to show the conservation of this quantity. a) In the morning, you leave the house with $5.00 in your pocket. At lunchtime, you pay the cashier $2.75 for a tray of pasta, ga ...
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... Superposition Example: Calculate the field (gravitational) at a special point due to two point masses Find the field at point P on x-axis due to two identical mass chunks m at +/- y0 • Superposition says add fields created at P by each mass chunk (as vectors!!) • Same distances r0 to P for both ma ...
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Newton`s Laws - Ccphysics.us

... ____ 21. Two blocks of masses 20 kg and 8 kg are connected together by a light string and rest on a frictionless level surface. Attached to the 8-kg mass is another light string, which a person uses to pull both blocks horizontally. If the two-block system accelerates at 0.5 m/s 2 what is the tensio ...
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... Which statement best describes the transformation of energy that occurs between times ti and tf? 1. Gravitational potential energy at ti is converted to internal energy at tf. 2. Elastic potential energy at ti is converted to kinetic energy at tf. 3. Both elastic potential energy and kinetic ener ...
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AP Physics Pacing Curriculum

... should include uniform circular motion and projectile motion. 4.C.1 The energy of a system includes its kinetic energy, potential energy, and microscopic internal energy. Examples should include gravitational potential energy, elastic potential energy, and kinetic energy. 4.C.1.1 The student is abl ...
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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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