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Formula Sheet – PHY 162 – Exam C
Formula Sheet – PHY 162 – Exam C

printable version - Gosford Hill School
printable version - Gosford Hill School

Charge, Coulomb`s Law and the Electric Field problem set
Charge, Coulomb`s Law and the Electric Field problem set

Gravity and handedness of photons
Gravity and handedness of photons

... ηab and the ordinary derivative ∂a are replaced by the curved metric tensor gµν and the associated covariant derivative ∇µ , and the curved spacetime α- and the β-matrices are obtained from the flat spacetime ones by using an orthonormal tetrad or vierbein, (αµ )νi (x) = eµa (x) eνb (x) (αa )b i . W ...
Review
Review

... Electricity and Gravity Review 1) Gravity between two electrons differs from the electrical force because the gravity is a) weaker and attractive b) stronger and attractive c) weaker and repulsive d) stronger and repulsive 2) An electron is heading directly toward a positive plate of charge. Therefo ...
Advanced Higher Physics learning outcomes
Advanced Higher Physics learning outcomes

EXAM 1 – 100 points - WebPhysics
EXAM 1 – 100 points - WebPhysics

... times when the glass is held 3.0 cm from it. Calculate (A) the focal length of the lens. +2.33 cm (B) the height of the image. –3.22 cm 8) A diffraction grating is designed to have the 2nd order maxima at 10° from the central maximum for red light (λ = 700 nm). How many lines per cm does the grating ...
V - barransclass
V - barransclass

Slide 1
Slide 1

... A conducting sphere initially has no net charge. A positively charged rod is then brought close to the sphere. The sphere is then connected to ground. The rod is then removed, and then the connection to ground is broken. After these steps, what is the net charge on the sphere? ...
Exercise 9 - Magnetism-The Lorentz Force
Exercise 9 - Magnetism-The Lorentz Force

... A metal wire of mass m slides without friction on two horizontal rails spaced a distance d apart, as shown in Fig. 32-36 below. The track lies in a vertical uniform magnetic field B. A constant current i flows from the generator G along one rail, across the wire, and back down the other rail. Find t ...
PHY 231 Lecture 29 (Fall 2006)
PHY 231 Lecture 29 (Fall 2006)

electric field
electric field

Electric Fields PPT
Electric Fields PPT

The Meaning of the Maxwell Field Equations
The Meaning of the Maxwell Field Equations

Physics Charge-to-mass Ratio Questions
Physics Charge-to-mass Ratio Questions

Elementary Particles in the theory of relativity
Elementary Particles in the theory of relativity

Electromagnetism G. L. Pollack and D. R. Stump The Exercise
Electromagnetism G. L. Pollack and D. R. Stump The Exercise

... A point charge q is located on the z axis at z = 2R. A grounded conducting sphere of radius R is centered at the origin. Then there is an image charge q 0 = −q/2 on the z axis at z = R/2. What does the electric field look like? The figure below shows the field lines (red and green curves) according ...
Answers
Answers

Unit 1 Day 3 – Electric Field Properties
Unit 1 Day 3 – Electric Field Properties

Electric Fields
Electric Fields

... By superposition we know that the new E field in the X direction is just the answer from (1) plus the Xcomponent of E3, which in this case will be the entire value of E3. ...
ECE Lecture 22: Electrostatics – Coulomb`s Law
ECE Lecture 22: Electrostatics – Coulomb`s Law

7.6 Electric Field Strength
7.6 Electric Field Strength

... We can create a uniform electric field by applying a potential difference across two parallel conducting plates separated by a distance d. In the diagram, below, field lines are drawn to show the electric field. ...
4.3.2 The multipole expansion
4.3.2 The multipole expansion

... Qij is symmetric (Qij = Qji ) and traceless (Tr Q = 0). A simple example is given by the charge distribution of two opposite dipoles ρ(~r) = q[δ(~r − ~a) − δ(~r)−δ(~r −~a−~b)+δ(~r −~b)] which gives p~ = 0 and Qij = 2q[~a·~bδij − 23 (ai bj +aj bi )]. Similar considerations also hold for the gravitati ...
Investigated Charges Virtual Lab
Investigated Charges Virtual Lab

... Click on the link - http://phet.colorado.edu/sims/charges-and-fields/charges-and-fields_en.html to complete this assignment. Objective: To explore electric field based on different charge configurations. Background: A charge affects the space around it, creating an electric field. Other charges arou ...
Motion of a Point Charge in a Magnetic Field
Motion of a Point Charge in a Magnetic Field

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Field (physics)



In physics, a field is a physical quantity that has a value for each point in space and time. For example, on a weather map, the surface wind velocity is described by assigning a vector to each point on a map. Each vector represents the speed and direction of the movement of air at that point. As another example, an electric field can be thought of as a ""condition in space"" emanating from an electric charge and extending throughout the whole of space. When a test electric charge is placed in this electric field, the particle accelerates due to a force. Physicists have found the notion of a field to be of such practical utility for the analysis of forces that they have come to think of a force as due to a field.In the modern framework of the quantum theory of fields, even without referring to a test particle, a field occupies space, contains energy, and its presence eliminates a true vacuum. This lead physicists to consider electromagnetic fields to be a physical entity, making the field concept a supporting paradigm of the edifice of modern physics. ""The fact that the electromagnetic field can possess momentum and energy makes it very real... a particle makes a field, and a field acts on another particle, and the field has such familiar properties as energy content and momentum, just as particles can have"". In practice, the strength of most fields has been found to diminish with distance to the point of being undetectable. For instance the strength of many relevant classical fields, such as the gravitational field in Newton's theory of gravity or the electrostatic field in classical electromagnetism, is inversely proportional to the square of the distance from the source (i.e. they follow the Gauss's law). One consequence is that the Earth's gravitational field quickly becomes undetectable on cosmic scales.A field can be classified as a scalar field, a vector field, a spinor field or a tensor field according to whether the represented physical quantity is a scalar, a vector, a spinor or a tensor, respectively. A field has a unique tensorial character in every point where it is defined: i.e. a field cannot be a scalar field somewhere and a vector field somewhere else. For example, the Newtonian gravitational field is a vector field: specifying its value at a point in spacetime requires three numbers, the components of the gravitational field vector at that point. Moreover, within each category (scalar, vector, tensor), a field can be either a classical field or a quantum field, depending on whether it is characterized by numbers or quantum operators respectively. In fact in this theory an equivalent representation of field is a field particle, namely a boson.
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