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Study Questions/Problems Week 5 Chapters 7 and 8 deal with
Study Questions/Problems Week 5 Chapters 7 and 8 deal with

... (a) The work required to stretch a spring depends on the square of the amount of stretch. Therefore, to stretch a spring by the amount x requires only 1/4 the work required to stretch it by the amount 2x. In this case, the work required is W0/4. (b) To stretch this spring by 3 cm from equilibrium re ...
Quiz - ScienceScene
Quiz - ScienceScene

... push it with a force of 20 lb.? A) 8 ft/sec2 B) 5 ft/sec2 C) 9 ft/sec2 D) 11 ft/sec2 8. 10, 4 A 50 kilogram mass ball-bearing moves through a mark on the floor with an acceleration of 4 m/sec2. What was the force (in Newton's) acting on the ball-bearing at that point? A) 150 Newton's B) 200 Newton's ...
Slide 1
Slide 1

...  You’ll notice as you pull the spring, that the further you extend the spring, then the greater the force that you have to exert in order to extend it even further.  As long as the spring is not streched beyond a certain extension, called elastic limit, the force is directly proportional to the ex ...
Forces-part2 [Compatibility Mode]
Forces-part2 [Compatibility Mode]

... Inertial reference frame • An inertial reference frame is one in which an observer: Sees no change in the velocity if the sum of all forces exerted on the system object is zero The force diagram and the motion diagram match. ...
Concept-Development Practice Page
Concept-Development Practice Page

Chapter 4 Kinetics of a particle
Chapter 4 Kinetics of a particle

... Therefore,   any path Fc  dr is a function of initial and end points only, It is defined as the change of potential energy, P.E. P.E. between two points is equal to the work done by an external force against the field of a conservative force for bringing  the particle from the starting point ...
115PowerPointReview
115PowerPointReview

PEKA 4
PEKA 4

... The acceleration of an object of constant mass will increase when the force acting on it increases. ...
Final Review Powerpoint
Final Review Powerpoint

2.Work and Energy Solutions
2.Work and Energy Solutions

The work-energy theorem
The work-energy theorem

... It equals the area of this rectangle on the graph. ...
Teachers Edition Sample Chapter 3 (483KB PDF)
Teachers Edition Sample Chapter 3 (483KB PDF)

Torque - curtehrenstrom.com
Torque - curtehrenstrom.com

Acceleration,
Acceleration,

Pressure
Pressure

...  The relative humidity, RH = 100  e/e*(T). • e* = e*(T) is the saturation vapour pressure, which is the maximum amount of water vapour, that an air parcel can hold, without condensation occurring.  The specific humidity, q = r/(1 + r), is the mass of water vapour per unit mass of moist air. ...
Forces and Newton`s Laws
Forces and Newton`s Laws

File
File

... Mechanical advantage – the ratio of the output force to the input force Mechanical advantage = output force (newtons) Input force (newtons) ...
Back
Back

... block of wood with a initial velocity of 100m/s sitting on a frictionless surface? What is the final velocity of the bullet and the block of wood? Back ...
Notes in pdf format
Notes in pdf format

... Since both blocks accelerate, there must be a net force acting on each one. The key to solving is to realize that Newton’s second law can be used separately for each block to relate the net force to the acceleration. Note also that both blocks have accelerations of the same magnitude a, since they m ...
Physics 605 – Mechanical Energy (Read objectives on screen
Physics 605 – Mechanical Energy (Read objectives on screen

Physics 101: Lecture 10
Physics 101: Lecture 10

... Wg = mg(h/cos)cos Wg = mgh Dy = yf-yi = -h Wg = -mgDy Physics 101: Lecture 10, Pg 6 ...
Stacey Carpenter - University of Hawaii System
Stacey Carpenter - University of Hawaii System

... weight, which they should already know. This should give them a deeper understanding. ...
Conservation of Momentum
Conservation of Momentum

5.1 The First Law: The Law of Inertia
5.1 The First Law: The Law of Inertia

... The Atwood’s machine is driven by a net force equal in magnitude to the weight difference between the two mass hangers. You will vary the two masses, m1 and m2, but you will keep the total mass constant. As you move plastic washers from m2 to m1, you will use a photogate to measure the acceleration ...
Recall: Gravitational Potential Energy
Recall: Gravitational Potential Energy

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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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