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Physics 2961
Intro. to Modern Physics!
Textbook: Rohlf, Modern Physics, Wiley!
Imaginary Numbers and Complex Notation!
x= Re(z)
y=
Im(z) !
z z = x + iy = r(cos! + i sin! )
ei!= cos! + i sin!
z = r cos! + i sin!( ) = rei!
z* = r cos! " i sin!( ) = re" i!
cos! =
ei!+ e
"i!
2; sin! =
ei!
" e"i!
2i
z
2
= zz* = (x+ iy)(x! iy)= x2+ y2
= r 2 or z2
= rei"re!i"= r 2
Magnitude!
Solve above two equations for ei! !Euler"s identity.!
Representation on a 2-dimensional complex plane.!
Plane Wave in Complex Notation
Plane wave: f (x, t) = A cos(kx !"t +# )
Wave number: k = 2$ / % Angular Frequency: " = 2$& = 2$ /T
Complex notation: f (x, t) = Aei(kx!"t+# )= A cos(kx !"t +# )+ i sin(kx !"t +# )( )
Phase angle: f (0,0) = A cos# + i sin#( ), Real part of f : # = cos!1 f (0,0)
A
'()
*+,
Intensity: I - ff*= Aei(kx!"t+# )A*e!i(kx!"t+# ) = AA* = A2
k!!k , x!
!r , kx! kx x + ky y + kzz =
!k i!r
f (x, y,z,t) = Aei(kxx+kyy+kzz"#t+$ )
= Aei(!k i!r"#t+$ )
Three Dimensions!
Vector Wave!
!E =!E0ei(!k i!r!"t+# )
Vector Calculus!
Read Rohlf, P576 to 577!
Gradient Operator
The gradient operator gives the direction and magnitude of the steepest!
rate of increase of a scalar function . !
!
!F "#F
#s1
u1+#F
#s2
u2+#F
#s3
u3
!
!F "#F
#xi +
#F
#yj +
#F
#zk
Cartesian coordinates.!
General coordinates.!
F(x, y, z)
The del or gradient operator in Cartesian and spherical coordinate systems.!Rohlf, Appendix E, P 587.!
Cartesian coordinates
Spherical Coordinates:
f = f (r,!,")
!#f = u
r
$f
$r+ u!
1
r
$f
$!+ u"
1
r sin!
$f
$"
!!f "
#f
#xi +
#f
#yj +
#f
#zk
$
%&'
()
!
!
Divergence and Curl
Since is a vector one can “dot” it with another vector. !
This is known as the divergence of a vector field.!!!
!! •!E = div(
!E) =
"
"xE
x+
"
"yE
y+
"
"zE
z
Cylindrical coordinates: !
!! •!E =
1
r
"
"rrE
r( ) +
1
r
"
"#E#( ) +
"
"zE
z( )
Spherical coordinates:
!! •!E =
1
r2
"
"rr
2E
r( ) +1
r sin#
"
"#E#
sin#( ) +1
r sin#
"E$
"$
Cartesian coordinates.!
Cross product or curl !
!! "!E = curl(E) =
i j k
#
#x
#
#y
#
#z
Ex
Ey
Ez
!A!!E =
i j k
Ax
Ay
Az
Ex
Ey
Ez
Cross product or curl !
!! "!E = curl(E) =
i j k
#
#x
#
#y
#
#z
Ex
Ey
Ez
!! "!E =
1
r
ur
ru#
uz
$
$r
$
$#
$
$z
Er
rE#
Ez
!! "!E =
1
r2
sin#
ur
ru#
r sin#u$
%
%r
%
%#
%
%$
Er
rE#
r sin#E$
Cartesian coordinates:!
Circular cylindrical coordinates: !
Spherical coordinates:
Some Vector Calculus Identities:
!! •"
!u = "
!! •!u +!u •!!"
!! #"
!u = "
!! #!u +!!" #
!u
!! •!u #!v =!v •!! #!u $!u •!! #!v
!! #
!u #!v( ) =!v •!!!u $!u •!!!v +!u
!! •!v( ) $!v
!! •!u( )
!!!u •!v( ) =!u •!!!v +!v •!!!u +!u "
!! "!v( ) +!v "!! "!u( )
!! "
!!#( ) = 0
!! •
!! "!u( ) = 0
!! "
!! "!u( ) =
!!!! •!u( ) $
!! •!!!u
!! •
!!#
1"!!#
2( ) = 0
In the above, assume that operates on all terms to its right that are not separated from it by intervening parentheses.
!!
!!f " #f
#xi +
#f
#yj +
#f
#zk
$
%&
'
()
Gradient: !
!! •!E = div(
!E) =
"Ex
"x+"Ey
"y+"Ez
"z
Divergence: !
!! "!E = curl(E) =
i j k
#
#x
#
#y
#
#z
Ex Ey Ez
Curl:!
Laplacian:!
!2f "!!i
!!f( ) =
#2f
#x2+#2f
#y2+#2f
#z2
Vector Calculus Operations!
Read Rohlf Appendix C, P576-577!
.
!P"!! id!a =
!"i
!P!!! dv
Divergence Theorem
The flux of a vector over a closed surface = the integral over the enclosed volume of the divergence.!
For example, for the electric field due to a charge distribution:!
(Rohlf, P 576)!
d!a
!P
.
!Aid!a"!! =
!"i
!A!!! dv
Example of Divergence Theorem
!Eid!a =
1
!0
""" #dv =q
!0
"""
!$i"""!Edv =
q
!0
#dv =q
!0
""" !0# =
!$i
!E (Gauss's Law)
Gauss" Law!
(!!"!P)id!a## =
!P•d!l"#
The “flux” of is the circulation of around any closed loop which bounds
the surface. The curl therefore is a measure of the rotation of the vector field. !
!!"!P
!P
Stokes Law
!P
d!l
d!a
(Rohlf, P 577)!
Class Exercise - Vector Calculus !
2. A sticky fluid is moving past a flat horizontal surface!
such that the velocity is given by m/s.!
Find both magnitude and direction of the curl,.!
!v = 10yi
3. The electric field inside a uniformly charged dielectric!
is . Find the divergence and therefore the charge!
distribution.!
!E = 10xi
1.The gravitational potential is U=Gy J/kg-m. Find the gradient.!
and the gravitational field, which is .!
!g = !
!
"U