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Pdf - Text of NPTEL IIT Video Lectures
Pdf - Text of NPTEL IIT Video Lectures

cos rFrF оvоо ∆ =∆⋅
cos rFrF оvоо ∆ =∆⋅

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NEWTON`S LAWS OF MOTION 1 Newton`s Laws of Motion

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... By the end of grade 2. [Intentionally left blank.] ...
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RevfinQans

... Answer: The tension is zero. By the same v  v2  v1 argument as in the question above, one can show that the acceleration is straight down when the mass on the extreme right with the string horizontal. Since the acceleration is straight down, the net force must be straight down, so there can be no ...
Dynamics Pupil Notes Name
Dynamics Pupil Notes Name

Torque and rotational inertia
Torque and rotational inertia

Wednesday, Jan. 30, 2002
Wednesday, Jan. 30, 2002

... Any velocity once imparted to a moving body will be rigidly maintained as long as the external causes of retardation are removed!! This statement is formulated by Newton into the 1st law of motion (Law of Inertia): ...
Rotational Motion
Rotational Motion

4 Class exercise sheet
4 Class exercise sheet

... horizontal plane are related to θ by (x, y) = R sin θ(cos ωt, sin ωt), up to a phase. Since this relation involves t, the Hamiltonian is not the energy. But H is in fact conserved, because there is no t dependence in L. The Hamiltonian differs from the energy due to the minus sign in the second term ...
Tutorial 4
Tutorial 4

PHYSICS 111 HOMEWORK SOLUTION #10 April 8, 2013
PHYSICS 111 HOMEWORK SOLUTION #10 April 8, 2013

Hong Kong Polytechnic University
Hong Kong Polytechnic University

... Hong Kong Polytechnic University Potential Energy & Conservation of Energy If, instead, the system is not isolated, then an external force can change the total energy of the system by doing work, W  Etot  K  U  Eint If a nonconservative applied force F does work on particle that is part of ...
Applying Newton second law to horizontal motion practice problems
Applying Newton second law to horizontal motion practice problems

... 24. A force of 300 N applied to a stove on a kitchen floor produces an acceleration of 5.0 m/s2. If the magnitude of the frictional force is 100 N, what is the mass of the stove? ...
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Lecture 13
Lecture 13

... change in translational kinetic energy of that object (as long as this energy does not go into internal energy…compressed spring, for instance) Wnet   W  KE  ...
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Energy - MHS Chemistry

... - implies another body (as position is defined relative to something else) - if there are two bodies, they interact by one or more forces - PE is the energy stored in the bodies due to the force between them - the magnitude of the force changes as the relative position of the bodies changes, so….. t ...
Energy Transfer And First Law
Energy Transfer And First Law

... Since heat and work are path dependent functions, they have inexact differentials designated by the symbol . The differentials of heat and work are expressed as Q and W. The integral of the differentials of heat and work over the process path gives the amount of heat or work transfer that occurr ...
Newton`s Second Law
Newton`s Second Law

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Kinetics of Particles: Oblique Central Impact
Kinetics of Particles: Oblique Central Impact

Ch 5 Study Guide 2013-2014 Multiple Choice Identify the choice that
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... ____ 21. If friction is the only force acting on an object during a given physical process, which of the following assumptions can be made in regard to the object’s kinetic energy? a. The kinetic energy decreases. b. The kinetic energy increases. c. The kinetic energy remains constant. d. The kineti ...
CHAPTER 11: Vibrations and Waves Answers to Questions
CHAPTER 11: Vibrations and Waves Answers to Questions

CHAPTER 11: Vibrations and Waves Answers to Questions
CHAPTER 11: Vibrations and Waves Answers to Questions

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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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