Upload
whoopi-cohen
View
47
Download
1
Tags:
Embed Size (px)
DESCRIPTION
Modeling and Simulating with Electromagnetism. Tim Thirion COMP 259 Physically-based Modeling, Simulation and Animation April 13, 2006. Before We Begin …. - PowerPoint PPT Presentation
Citation preview
Modeling and Simulating with Electromagnetism
Tim ThirionCOMP 259
Physically-based Modeling, Simulation and Animation
April 13, 2006
04/19/23 2
Before We Begin …
A question: If I place a proton at the North pole and another at the South pole, what is the approximate ratio of the strength of the electrostatic force to the gravitational?
1. 12. 10¹3. 10²4. 10³
SolutionThe gravitational force is
The Coulomb force isThe ratio is
Relevant constants:
04/19/23 4
Why is gravity so weak?• The Four Physical Forces
– Strong Nuclear (binds nucleons)– Weak Nuclear (some forms of nuclear decay)– Electromagnetic– Gravitational
• The first three have been shown to be indistinguishable in certain (Big Bang-like) conditions
• “Uniting” the four forces is the greatest outstanding problem in physics (String Theory, etc.)
04/19/23 5
Outline
• Why should a computer scientist care about electromagnetism (EM)?
• The Fundamentals: Statics and Dynamics
• Visualizing Vector Fields using LIC• Application: Modeling the
Magnetosphere• FEMs, Materials Science and
Nanoscience• Questions and (Hopefully) Answers
04/19/23 6
Orders of Magnitude
Electromagnetism is the prevailing force on a huge range of physical scale …
On the smallest scales, EM dominates where nuclear forces drop off.– Scale: ~10 pm (average atom radius) – 10
nm– Must use QEM– Fundamental particles, origin of the universe– Molecule formation (chemistry)– Smallest feature of Intel’s chips (65 nm, as of
2006)
04/19/23 7
Orders of Magnitude
From 1 nm = 10 Å to 1 cm, we can begin modeling nanomolecules, organic molecules, and microdevices.– 1 nm is the radius of a carbon nanotube– 2 nm is the diameter of a DNA helix– Nanoscience and materials science
simulation would occur mostly at this scale– Electrostatic effects are prevalent
04/19/23 8
Orders of Magnitude
On the scale of everyday experience, we again see multiple applications– 1 cm – 1,000 km = 1 Mm– Approximations of the interaction of light
and matter (rendering)– Modeling of solids, crystals, x-ray
diffraction simulations
On the scale of the earth, geo* applications– The ionosphere and magnetosphere– Lightning and weather systems
04/19/23 9
And Beyond…
At higher scales, gravity dominates. However, EM still plays a role as light…– Star formation (QM, gravity, fluids, and
light propagation)– Galaxial modeling, supernovae (models
needed to predict release of energy and particles)
– Cosmic background radiation models– And so on…
04/19/23 10
Electrostatics: Coulomb’s Law
Coulomb’s Law gives the force between two charged particles at rest:
04/19/23 11
Coulomb’s Law
The Law of Superposition holds
Why doesn’t an electron collide with the positively charged protons in a nucleus?
Does an electron act on itself?
04/19/23 12
Vector FieldsVector fields associate a
vector with each point in space.
The curl of a vector field gives the circulation within a volume.
The divergence of a vector field gives the outward flow from a volume.
04/19/23 13
Fields
All of electromagnetism is concerned with deriving and utilizing the magnetic and electric fields.
Both are functions of space and time:
As we shall see, they are deeply interconnected.
In fact, they are essentially different aspects of the same phenomenon.
04/19/23 14
Electric Fields
What force will a positive “test” charge feel if placed into an electric field?
More concisely
04/19/23 15
FluxSuppose we have a closed surface.In the case of a fluid, we can ask, are we
losing or gaining fluid in the enclosed volume?
The net outward flow or flux is:
04/19/23 16
Electric Flux
Electric fields do not “flow” because they are not the velocity of anything.
We can still compute the flux using E.It turns out that
Or
04/19/23 17
Gauss’ Law
A result from vector calculus, Gauss’ Theorem, says
Using a charge density:
Taking the limit as V goes to zero
The first of Maxwell’s Equations:
04/19/23 18
CirculationAs with flux, we can define the amount of
circulation present in a field.Draw a closed curve, how quickly does
the fluid inside travel around this curve?
The circulation is:
04/19/23 19
Circulation with the Magnetic Field
The circulation of the magnetic field around a closed loop is proportional to the net current flowing through it.
04/19/23 20
Ampere’s Law
From vector calculus, Stokes’ Theorem says
Apply this, and make the surface infinitesimally small:
Differential form of Ampere’s Law:
04/19/23 21
Ampere’s Law
This is not fully general. Also must consider electric flux through S:
Using techniques from vector calculus, we arrive at the general differential form of Ampere’s Law:
04/19/23 22
Problem
Coulomb’s Law holds for static charge configurations.
Moving charges generate magnetic fields.
How do magnetic fields affect the motion of charged particles?
Coulomb’s Law is no longer the full story …
04/19/23 23
The Lorentz Force
The total force on a charged particle due to electric and magnetic fields is
Note the presence of the cross product and the dependency on velocity, not acceleration.
04/19/23 24
ApplicationModeling the dynamics of charged particles immersed in
E and B fields.Simply need to balance quantities, and use your favorite
integrator with the Lorentz force!
See: http://www.levitated.net/p5/chamber/
04/19/23 25
Circulation of the Electric Field
Suppose we have a surface S with a curve boundary C, then
In the language of vector calculus
04/19/23 26
Faraday’s Law
As we did for Gauss’ Law, shrink S to an infinitesimally small surface to get the differential form:
Faraday’s Law of Induction:
04/19/23 27
The Last Equation
Recall Gauss’ Law
Is there a similar analog for magnetism?
That is, can we encapsulate magnetic “charges” in a surface, and measure the magnetic flux?
04/19/23 28
The Last Equation
There is no (as yet observed) magnetic charge or “monopole.”
The magnetic field is divergence free, there is no inward or outward flow, to or from a point.
The last of Maxwell’s Equations:
04/19/23 29
The Maxwell Equations
Gauss’ Law
Faraday’s Law of Induction
Analog of Gauss’ Law for Magnetism
Ampere’s Law with Maxwell’s Extension
04/19/23 30
Visualizing Vector FieldsThere are many techniques available for
determining and rendering field lines.
We can trace particles through the field, use stream lines, or use icons. That is, place a relevant symbol along regular sample points (arrows, ellipsoids, etc.)
Some methods use Gaussian linear solvers, conjugate gradient methods, spot noise, reaction diffusion textures, etc.
One of the most interesting is Line Integral Convolution.
04/19/23 31
Line Integral Convolution
“LIC emulates the effect of a strong wind blowing a fine sand.”
Idea:– For each sample in the vector field
• Compute a stream line starting at a cell, moving forward and backward a determined distance
• Use the points covered to index a white noise texture
• Convolve the texture points to determine the corresponding pixel color for the cell.
04/19/23 32
Visual LIC
LIC improves on DDA (digital differential analyzer).
DDA used straight line approximations in the vector field.
04/19/23 33
Visual LIC
To generate streamlines:
04/19/23 34
LICThe final convolution step:
k(w) is the convolution kernel.
04/19/23 35
LIC Results
04/19/23 36
Modeling the Magnetosphere
Earth’s magnetosphere is caused primarily by two effects:
• The convection of ionized liquid metals in the Earth’s outer core
• The solar winds: a vast flow of plasma (a stream of free ions)
The strength of earth’s magnetic field decays exponentially; half-life 1400 years, reversals every 250,000 years (500,000 years overdue)
04/19/23 37
Visualizationshttp://
svs.gsfc.nasa/gov/search/Keyword/Magnetosphere.html
04/19/23 38
Finite Element Methods (FEMs)
• As we have seen, FEMs begin with discretization (tetrahedra, cubes, …)
• Nearly every computational physics problem can be represented by matrices…
• Highly specialized, dense:– “A Finite Element Computation of the Gravitational
Radiation emitted by a Point-like object orbiting a Non-rotating Black Hole”
– “Advanced Finite Element Method for Nano-Resonators”
– “An Algorithm for Constructing Polynomial Systems Whose Solution Space Characterizes Quantum Circuits”
04/19/23 39
Computational Materials Science
• Already becoming an important new topic in physical simulation
• Current topics:– Deformation of metals (bouncing metal balls?)– Micromagnetic modeling (with mesoscale
physics)– Phase Field Modeling (applied: solidification)– Discovering/Designing effective Hamiltonians– Quantum dots, quantum information,
superconductors– Surfaces and interfaces
04/19/23 40
Final Thoughts
Electromagnetic phenomena are incredibly diverse.
Theory and methods are relatively simple.Phenomena can be incredibly complex.
There’s plenty of room at the bottom!
04/19/23 42
Bibliography• Classical Electrodynamics, J.D. Jackson, John Wiley
& Sons, Inc., 2001• The Feynman Lectures on Physics, R.P. Feynman,
R.B. Leighton, and M. Sands, Addison Wesley Publishing Company, Inc., 1963
• Fundamentals of Physics, D. Halliday, R. Resnick, J. Walker, John Wiley & Sons, Inc., 2003
• A Dynamical Theory of the Electromagnetic Field, J.C. Maxwell, Scottish Academic Press, Ltd., 1982
• The Nature of Solids, A. Holden, Dover Publications, Inc., 1965
04/19/23 43
Bibliography
• Finite Element Method for Electromagnetics, J.L. Volakis, A. Chatterjee, and L.C. Kempel, IEEE Press, 1998
• Imaging Vector Fields using Line Integral Convolution, B. Cabral and L. Leedom, Proceedings of ACM SIGGRAPH 1993
• Computational Physics Lecture Notes, A. MacKinnon, available on the internet (please e-mail me)
04/19/23 44
Links
• Center for Theoretical and Computational Materials Science – http://www.ctcms.nist.gov/
• TEAL at MIT: http://web.mit.edu/8.02t/www/802TEAL3D/index.html