Why Study Electromagnetics? What is Electromagnetics?
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Transcript of Why Study Electromagnetics? What is Electromagnetics?
Why Study Electromagnetics?
What is Electromagnetics?
What is a charge q?
Fundamental Laws of Electromagnetics
Steps in Studying Electromagnetics
SI (International System) of Units
Units Derived From the Fundamental Units
Fundamental Electromagnetic Field Quantities
Three Universal Constants
VECTOR REPRESENTATION
3 PRIMARY COORDINATE SYSTEMS:
• RECTANGULAR
• CYLINDRICAL
• SPHERICAL
Choice is based on symmetry of problem
Examples:
Sheets - RECTANGULAR
Wires/Cables - CYLINDRICAL
Spheres - SPHERICAL
Orthogonal Coordinate Systems: (coordinates mutually perpendicular)
Spherical Coordinates
Cylindrical Coordinates
Cartesian Coordinates
P (x,y,z)
P (r, Θ, Φ)
P (r, Θ, z)
x
y
zP(x,y,z)
θ
z
rx y
z
P(r, θ, z)
θ
Φ
r
z
yx
P(r, θ, Φ)
Page 108
Rectangular Coordinates
-Parabolic Cylindrical Coordinates (u,v,z)-Paraboloidal Coordinates (u, v, Φ)-Elliptic Cylindrical Coordinates (u, v, z)-Prolate Spheroidal Coordinates (ξ, η, φ)-Oblate Spheroidal Coordinates (ξ, η, φ)-Bipolar Coordinates (u,v,z)-Toroidal Coordinates (u, v, Φ)-Conical Coordinates (λ, μ, ν)-Confocal Ellipsoidal Coordinate (λ, μ, ν)-Confocal Paraboloidal Coordinate (λ, μ, ν)
Parabolic Cylindrical Coordinates
Paraboloidal Coordinates
Elliptic Cylindrical Coordinates
Prolate Spheroidal Coordinates
Oblate Spheroidal Coordinates
Bipolar Coordinates
Toroidal Coordinates
Conical Coordinates
Confocal Ellipsoidal Coordinate
Confocal Paraboloidal Coordinate
Cartesian CoordinatesP(x,y,z)
Spherical CoordinatesP(r, θ, Φ)
Cylindrical CoordinatesP(r, θ, z)
x
y
zP(x,y,z)
θ
z
rx y
z
P(r, θ, z)
θ
Φ
r
z
yx
P(r, θ, Φ)
VECTOR NOTATION
VECTOR NOTATION:
zzyyxx aAaAaAA ˆˆˆ Rectangular or
Cartesian Coordinate
System
x
z
y
zzyyxx BABABABA
Dot Product
zyx
zyx
zyx
BBB
AAA
aaa
BA
ˆˆˆ
Cross Product
21
222zyx AAAA
Magnitude of vector
(SCALAR)
(VECTOR)
Coulomb’s Law
1 2212
q qF k12 r
Coulomb’s law gives the force (in Newtons) between charges q1 and q2, where r12 is
the distance in meters between the charges, and k=9x109 N·m2/C2.
Coulomb’s law quantifies the magnitude of the electrostatic force.
To make this into a “really good” starting equation I should specify “repulsive for like,” but that makes it too wordy. You’ll just have to remember how to find the direction.
1 2212
q qF k ,12 r
attractive for unlike
Force is a vector quantity. The equation on the previous slide gives the magnitude of the force. If the charges are opposite in sign, the force is attractive; if the charges are the same in sign, the force is repulsive. Also, the constant k is equal to 1/40, where
0=8.85x10-12 C2/N·m2.
Remember, a vector has a magnitude and a direction.
One could write Coulomb’s Law like this…
The equation is valid for point charges. If the charged objects are spherical and the charge is uniformly distributed, r12 is the distance between the centers of the spheres.
If more than one charge is involved, the net force is the vector sum of all forces (superposition). For objects with complex shapes, you must add up all the forces acting on each separate charge (turns into calculus!).
+ -
r12
+
++
-
--
We could have agreed that in the formula for F, the symbols q1 and q2 stand for the
magnitudes of the charges. In that case, the absolute value signs would be unnecessary.
1 2212
q qF k ,12 r
However, in later equations the sign of the charge will be important, so we really need to keep the magnitude part.
On your homework diagrams, show both the magnitudes and signs of q1 and q2.
Your starting equation sheet has this version of the equation:
which gives you the magnitude F12 and tells you that you need to figure out the direction separately.
Gauss’ Law
Electric Flux
We have used electric field lines to visualize electric fields and indicate their strength.
We are now going to count the number of electric field lines passing through a surface, and use this count to determine the electric field. E
The electric flux passing through a surface is the number of electric field lines that pass through it.
Because electric field lines are drawn arbitrarily, we quantify electric flux like this: E=EA, except that…
If the surface is tilted, fewer lines cut the surface.
EA
Later we’ll learn about magnetic flux, which is why I will use the subscript E on electric flux.
E
E
A
The “amount of surface” perpendicular to the electric field is A cos .
A = A cos so E = EA = EA cos .
We define A to be a vector having a magnitude equal to the area of the surface, in a direction normal to the surface.
Because A is perpendicular to the surface, the amount of A parallel to the electric field is A
cos .
Remember the dot product?E E A
If the electric field is not uniform, or the surface is not flat…
divide the surface into infinitesimal surface elements and add the flux through each…
dAE
iE i i
A 0i
lim E A
E E dA
A
If the surface is closed (completely encloses a volume)…
E
…we count* lines going out as positive and lines going in as negative…
E E dA
dA
a surface integral, therefore a double integral
Question: you gave me five different equations for electric flux. Which one do I need to use?
E E dA
E E dA
E E A
E EAcos
E EA
Answer: use the simplest (easiest!) one that works.
Flat surface, E A, E constant over surface. Easy!
Flat surface, E not A, E constant over surface.
Flat surface, E not A, E constant over surface.
Surface not flat, E not uniform. Avoid, if possible.
Closed surface. Most general. Most complex.
If the surface is closed, you may be able to “break it up” into simple segments and still use E=E·A for each segment.