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Chapter 1 Forces and Pressure
Chapter 1 Forces and Pressure

... D. INERTIA (Idle or lazy)  The tendency of an object to resist changes in motion.  Objects seem _________ because they do not easily change the way they __________.  Objects at rest don’t want to start ________, objects moving do not want to ___________. 1. MASS (effects on inertia) Q. Is it eas ...
Materialy/01/Applied Mechanics-Lectures/Applied Mechanics
Materialy/01/Applied Mechanics-Lectures/Applied Mechanics

... Let us consider that the particle follows during the time interval [t1, t2] a motion trajectory u i* distinct from the real one ui. This allows us to define the virtual displacement of the particle the relationship ...
Q1. (a) State the difference between vector and scalar quantities
Q1. (a) State the difference between vector and scalar quantities

further force and motion considerations
further force and motion considerations

... – any two objects with masses attract each other and the magnitude of this attracting force is proportional to the product of the masses and inversely proportional to the square of the distance. This also holds for the gravitation between the earth and an object on the earth. The gravitational force ...
Work and Energy
Work and Energy

... Energy is a conserved quantity, like mass. This means that the total amount of energy in a closed system remains constant. The initial energy must equal the final energy. Energy conservation is relatively simple as long as you keep this in mind. Begin by adding all the energy terms at the beginning ...
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221syllabusSum13 - Oakton Community College

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Kinetic Energy

... Types of Energy Thermal energy - due to temperature (recall that this comes from the motion of molecules, so it is really kinetic energy) Heat energy -transfer of thermal energy Chemical Potential Energy - stored in ...
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Work – Energy Theorem: W = AKE

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Work, Energy and Power

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... Newton’s First law of Motion I. Every object in a state of uniform motion tends to remain in that state of motion unless an external force is applied to it. Newton's Second Law of Motion: II. The relationship between an object's mass m, its acceleration a, and the applied force F is F = ma. Accelera ...
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... object in motion continues in motion with constant velocity (constant speed in straight line) unless acted on by a net external force. “in motion” or “at rest” – with respect to the chosen frame of reference “net force” – vector sum of all the external forces acting on the object – FNet,x and FNet,y ...
Unit 6 - PowerPoint
Unit 6 - PowerPoint

... Conservation of energy and momentum can also be used to analyze collisions in two or three dimensions, but unless the situation is very simple, the math quickly becomes unwieldy. Here, a moving object collides with an object initially at rest. Knowing the masses and initial velocities is not enough; ...
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Lecture Outline Chapter 9 Physics, 4th Edition James S. Walker

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Newton`s Second Law Lab

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Physics 106P: Lecture 5 Notes

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Work and Energy

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... And when you put it all together for a given object at the top of a ramp: PEtop = KErot at bot + KElin at bot mghtop = ½ c mv2 + ½mv2 so mass cancels too! So for a particular h, what determines which object will have the greater v (win), is its smaller “c” value which is only based on shape & axis o ...
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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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