handout lecture01 introduction and vector analysis
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FI 2201 Electromagnetism
Alexander A. Iskandar, Ph.D.Physics of Magnetism and Photonics Research Group
General Information• Lecture Schedule :
18 19 R120127 28 R????
• Tutorials57 58 R9132Teaching Assistant : Mr. Andika Putra.During the tutorial there will be several Quizes and average mark of the Quizes will be one of the component of the Final Mark
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Mark
• Walk Out time : 20 minutes• Textbook :
Introduction to Electrodynamics, D. J. Griffiths, Prentice Hall, 1991.
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General Information• Evaluation :
2 Midterm Exams (15/3 and 10/5)A Re-evaluation Exam, if taken will replace the worst mark of Midterm Exam
• Expected Exam Answer :Answer should show good understanding of the physical phenomena considered in the problem, as evident by sound arguments and clear and correct steps in finding the solution.The use of correct formulas and notation (vector and scalar) and the right units
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the right units.Final correct numerical value (if asked).
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Introduction
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The Realm of Mechanics and Electromagnetism
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• Electromagnetism is the ONLY theory that is well understood in all realm of mechanics.
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Early Observation of ElectricityObservation from early Greeks time.If you rubbed a piece of amber, it will attract bits of straw.attract bits of straw.If you rubbed two pieces of amber, they will repels each other.Thus there are two results from one phenomena.There is a another force of nature aside gravity
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aside gravity.
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Origin of Electricity : Electric ChargeNeeds a physical quantity to specify the property of a material with specific response of this phenomena.This physical quantity is called (electric) charge.Two types of charges: positive and negative
Like charges repel (unlike gravity)Opposite charges attract (like gravity)
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Opp g ( g y)
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Particles Discovered 1898 – 1964
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Particles Discovered since 1964
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Interlude: The Strong Nuclear Force• In early 1960s there was a particle
explosion – in the time span of weeks new particles were discovered.
• The particles cannot be explained with the known theories at that time (electromagnetism).
• Need a new theory !! Hence new physical quantity that goes with this
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p y q y gtheory !!
• The theory states that these particles were not elementary !!
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Interlude: The Strong Nuclear Force• These particles were build up from
smaller constituents called the QUARKS. Some particles consist of 3 quarks, others consist of 2 quarks.
• Interaction between the quarks cannot be seen from far away.
• Hence need a physical quantity like charge that has to be of three kinds
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gand are invisible from far away →color charge.
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Interlude: The Strong Nuclear Force3/22/2010
Mesons consist of a quark-antiquarkpair, while baryons consist of three
quarks.
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The current view of how matter is composed of basic units.
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The Structure of an Atom
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The Four Forces of Nature
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Fundamental Interactions of Nature
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Comparison between the two Forces• Determine the electrostatic force and the gravitational
force between an electron and a proton that is separated 1 m apart
( )( )
mm
N
rQQkFC
28219
9
221
103.21106.1109 −
−
×=×
×=
=r
Gravity is 1040
times weaker
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( )( )( ) N
rmmGFG
682731
11
221
10015.11
1067.11011.91067.6 −−−
− ×=××
×=
=r
than Electrostatic
force.
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Interaction Strength
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The Ultimate Goal of Physics: Unification of All Forces
GRAVITATION
MAGNETISMELECTRICITY
WEAK
ELECTROWEAK
SINGLE FORCE?
GRAVITATION
ELECTROMAGNETISM
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STRONG
GRANDUNIFICATION
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Unification : the Standard Model• Description of strong, weak, and electromagnetic
interactions• No known discrepancy with particle physics experimentsNo known discrepancy with particle physics experiments• Three types of fundamental particles
Stuff things are made of – spin ½Force carriers – spin 1Higgs field – spin 0
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Fundamental Particles• There are only 12
fundamental particles of matter (also the antiparticles)
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Fundamental Particles
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Interaction in Field Formulation• Action at a Distance – Electric Field• How do we explain the nature of non-contact force or
“force at a distance” between two charges?force at a distance between two charges?
• The concept of “Electric Field” - a charge creates an “electric field” in the space around it. Other charges interact with this field.
• The nature of an Electric Field - an electric field has a defined magnitude and direction at all points in space
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defined magnitude and direction at all points in space. I.e. it is a vector field.
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Sources in Electromagnetism• Electric charge :
two typesconservedthe number of positive and negative charges exactly the same, compare gravity and electrostatic forces (if there are excess charges on the moon → the orbit won’t be like what is predicted by gravity alone)quantizedalthough there are fractional charges but there are not observed individually
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y
• For accelerated charges, a portion of the field “detaches” and travel off at the speed of light – electromagnetic radiation.
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Syllabus• Continuation and extension of classical electricity and
magnetism phenomena that have been introduced in the Fundamental Physics course. The aim of this course is to introduce a unified formulation of electric and magnetic phenomena as one of the fundamental interaction in nature. The main topics considered in this course are
Electrostatics, Techniques in solving Electric Potential, Electric field in matter,
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Magnetostatics, Magnetic field in matter, Electrodynamics and an introduction to Electromagnetic wave.
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Vector Analysis
REVIEW ON VECTOR QUANTITIES
Vector Quantity• Graphical representation and transformation graphically.• A vector can be identified by specifying its three Cartesian
components:components:
zAyAxA zyx ˆˆˆ ++=A
Unit vectors
z axis
y axis
A
• Operations on Vectors :
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x axis
pTo add vectors, add like componentsTo multiply a vector by a scalar, multiply each components
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Operations between vectors• The dot product of two vectors is obtained by multiplying
like components and add:BABABA ++=⋅BA
• This operation is also called inner product and it yielded a scalar quantity, it is needed for finding distance.
zzyyxx BABABA ++=BA
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Operations between vectors• The cross product of two vectors is obtained from the
determinant:
zyx ˆˆˆ
the Levi-Civita tensor
ikjijk
zyx
zyx eBABBBAAAzyx
ˆε==×BA
⎪
⎪⎨
⎧−+
=ε npermutatiooddanis)(if1npermutatioevenanis)(if1
ijkijk
ijk
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• This operation yielded a vector quantity and it has anticommuting property as can be seen from the property of the Levi-Civita tensor.
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⎪⎩ otherwise0
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Vector Transformation• The components of a vector
depend on the choice of the coordinate system.
• Different coordinate system will produce different components for the same vector.
• The choice of coordinate system being used can significantly change the complexity of
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g p yproblems in electrodynamics.
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Vector Transformation• The coordinates of vector in
coordinate system S are related to the coordinates of vector in
Ar
Ar
coordinate system S′ by
• The rotation considered here leaves the x axis untouched. Thex coordinate of vector will thus
⎟⎟⎠
⎞⎜⎜⎝
⎛⎟⎟⎠
⎞⎜⎜⎝
⎛−
=⎟⎟⎠
⎞⎜⎜⎝
⎛
′
′
z
y
z
y
AA
AA
φφφφ
cossinsincos
Ar
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x coordinate of vector will thus not change:
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A
ARAAA
AAA
x
z
y
x
z
y
x rt⋅=
⎟⎟⎟
⎠
⎞
⎜⎜⎜
⎝
⎛
⎟⎟⎟
⎠
⎞
⎜⎜⎜
⎝
⎛
−=
⎟⎟⎟
⎠
⎞
⎜⎜⎜
⎝
⎛
′
′
′
φφφφ
cossin0sincos0001
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Vector Transformation• The 3 by 3 transformation matrix is the matrix
representation of the transformation tensor .• Coordinate transformation resulting from a rotation around
Rt
Coordinate transformation resulting from a rotation around an arbitrary axis can be written as:
or, more compactly,
⎟⎟⎟
⎠
⎞
⎜⎜⎜
⎝
⎛
++++++
=⎟⎟⎟
⎠
⎞
⎜⎜⎜
⎝
⎛
⎟⎟⎟
⎠
⎞
⎜⎜⎜
⎝
⎛
=⎟⎟⎟
⎠
⎞
⎜⎜⎜
⎝
⎛
′
′
′
zzzyzyxzx
zyzyyyxyx
zxzyxyxxx
z
y
x
zzzyzx
yzyyyx
xzxyxx
z
y
x
ARARARARARARARARAR
AAA
RRRRRRRRR
AAA
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∑=
=′→⋅=′3
1jjiji ARAARA
rtr
Vector Transformation• The rotation matrix is an example of a unitary
transformation: one that does not change the magnitude of the object on which it operates:
Rt
• If is unitary, thenAAAAandARA =′→=′⋅=′
rrrtr
∑=
δ=3
1ijkikij RR
⎧ =if1 kj
Rt
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where (Kronecker delta)
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⎩⎨⎧ =
=δotherwise0if1 kj
jk
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Vector Transformation• A reflection or inversion is given by the transformation
matrix: which changes the right-handed coordinate system into a left-handed coordinate system.
ijijR δ−=
z axis
x axis
y axis
rrz’ axis
x’ axis
y’ axis
r ′r
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• The vector transform into . Reversing the direction of the coordinate system and changing the sign of the components give .
• Vectors with this property are called polar vectors.
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),,( zyxr =r
rr rr ′=
),,(),,( zyxzyxr −−−=′′′=′r
Vector Transformation• A fundamental difference is encountered when a vector is
defined as the cross-product of two polar vectors, , . and are polar vectors. When the coordinate axes are
BACrrr
×=Br
Ar
inverted, the cross-product vector does not behave like polar vectors under inversion, i.e
iikkjjkjijki CCBBAABAC ′+→′−→′−→ε= yields,with,
Cr
z’ axis
x’ axisCr
y axis
Ar
Br
A′r
Br′
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• Vectors with this property are called axial or pseudo-vectors. Magnetic field is an example of a pseudo vector.
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y’ axisz axis
x axis
B
Cr′