EE750 Advanced Engineering Electromagnetics Lecture 3 · EE750,2003, Dr. Mohamed Bakr 2 Special Cases in Maxwell’s Equations. •With no sources, Maxwell’s Equations are written

1

EE750Advanced Engineering Electromagnetics

Lecture 3

2EE750,2003, Dr. Mohamed Bakr

Special Cases in Maxwell’s Equations.

• With no sources, Maxwell’s Equations are written as

,

• In Cartesian coordinates we have

t∂∂−=×∇ B

E)(t

c ∂∂+=×∇ D

JH )(

tB

zE

yE xyz

∂∂−=

∂∂

−∂

∂

tB

xE

zE yzx

∂∂

−=∂

∂−∂

∂

tB

yE

xE zxy

∂∂−=

∂∂−

∂∂

tD

Jz

HyH x

xyz

∂∂+=

∂∂

−∂

∂

tD

JxH

zH y

yzx

∂∂

+=∂

∂−∂

∂

tD

JyH

xH z

zxy

∂∂+=

∂∂−

∂∂


Special Cases (Cont’d)

• For a 1D case, the fields depend only on one coordinate(e.g. a uniform plane wave traveling in the x direction)

• For example, if ∂/∂y= ∂/∂z=0

, (propagation in –ve x)

or

, (propagation in +ve x)

Notice that these two systems are decoupled

tB

xE yz

∂∂

−=∂

∂−t

DJ

xH z

zy

∂∂+=

∂∂

tB

xE zy

∂∂−=

∂∂

tD

JxH y

yz

∂∂

+=∂

∂−


Special Cases (Cont’d)

• For the 2D problems, the fields depend only on twocoordinates (e.g. TE10 mode in waveguides)

• For example, if ∂/∂y=0

tB

zE xy

∂∂−=

∂∂

−

tB

xE

zE yzx

∂∂

−=∂

∂−∂

∂

tB

xE zy

∂∂−=

∂∂

tD

Jz

H xx

y

∂∂+=

∂∂

−

tD

JxH

zH y

yzx

∂∂

+=∂

∂−∂

∂

tD

Jx

H zz

y

∂∂+=

∂∂

TEy TMy

Notice that the two systems are decoupled


Transient Response of a Transmission Line

• Cd capacitance per unit length F/m

Ld inductance per unit length H/m

u velocity of propagation

• After time ∆t, the disturbance traveled a distance ∆x.A charge ∆Q=Cd ∆x Vs been transferred. It follows that

i=∆Q/∆t i=Cd Vs (∆x/ ∆t)= Cd Vs u

x∆

C

L


Transient Response of a TL (Cont’d)

• The flow of current establishes a flux Φ associated withline inductance through Φ=Ld ∆x i= Ld ∆x Cd Vs u

• Using Faraday’s law we have

Vs=∆Φ/ ∆t =LdCdVsu2 LdCdVsu

2=1.0

m/s

• It follows that i= Cd Vs u=Vs

LCu

dd

1=

L

C

d

d

Ω===C

LiV

Zd

ds

currentincident

voltageincidento


Open-Ended Transmission Line

• After time τ, the incident voltage and current wavesreach the open end. A reflected current wave ofamplitude is initiated to make the totalcurrent at the open end zero

• It follows that for an open-ended transmission line wehave V i= V s , and V r= V s,

ZVI sr

o/−=

ZVI si

o/= ZVI sr

o/−=

τt <1

τt <1

l/u=τ


Thevenin Equivalent of a Transmission Line

• The open circuit voltage is 2V i (open-ended line)

• The equivalent resistance is Zo

• This Thevenin equivalent is valid only for limited timeperiod where no reflections takes place on the line(same V i)


Example on Utilizing Thevenin’s Equivalent of a TL

• Using Kirchtoff’s voltage law we have

• But V=V i+V r V r= V -V i

• For open circuit termination R=∞, Γ=1, V r= V i

• For short circuit termination R=0, Γ=-1, V r= -V i

ZR

RVV i

o

2+

=

VZR

RVV iir −

+=

o

2 VVZRZ-R

V iir Γ=

+

=o

o


• Remember that for a steady-state sinusoidal analysiswe need only the amplitude and phase at each point onthe line

• Applying KVL, we get

Leading to

• Applying KCL we get

Leading to

Sinusoidal Steady-State Response of a TL

))(Re(),( tjexpVtxV ω=

)()()( xIxLjxxVxV d ∆=∆+− ω

)()(

xILjx

xVdω=

∂∂−

)()()( xVxCjxxIxI d ∆=∆+− ω

)()(

xVCjx

xIdω=

∂∂−

xx ∆+

xLd ∆

xCd ∆)(xV )( xxV ∆+

)(xI )( xxI ∆+


Sinusoidal Steady State of a TL (Cont’d)

• Differentiating to eliminate the current term we get

• Similarly

• Using the telegapher’s differential equations we canshow that and

• It follows that

and

)()()( 22

2

2

xVxVCLx

xVdd βω −=−=

∂∂

)()()( xjexpVxjexpVxV ri ββ +−=

)()()( xjexpIxjexpIxI ri ββ +−=

ZVI iio/= ZVI rr

o/−=

)()()( xjexpVxjexpVxV ri ββ +−=

)()()()()( oo xjexpZ/VxjexpZ/VxI ri ββ −−=


ABCD Matrix of a TL Section

• At x=0, we have and

• Expressing the solutions in terms of the amplitudes atx=0, we get

VVV ri +=(0) )()()0( oo Z/VZ/VI ri −=

−

−=

)0(

)0(

)cos(/)sin(

)sin()cos(

)(

)(

I

V

xZxj

xZjx

xI

xV

o

o

ββββ

=

)(

)(

)cos(/)sin(

)sin()cos(

(0)

(0)

xI

xV

xZxj

xZjx

I

V

o

o

ββββ

ABCD matrix of a TL section with length x


Discrete Models of Lumped Elements

• The lumped element is replaced by a section of atransmission line

• Using these models the voltages and currents are obtainedonly at discrete instants of time

• Cd∆l=C, Cd is the capacitance per unit length

• u=∆l/ ∆t=1/ CL ddCl

tL

dd

12

∆∆=

l∆

C


Discrete Models of Lumped Elements (Cont’d)

•

• Le = equivalent (parasitic) inductance =

• ∆t is selected small enough such that the parasiticinductance is small

C

t

lC

t

C

LZ

dd

dc

∆=∆

∆==( )

C

tlLd

∆=∆2

Modeling Steps:

1.Select ∆t, ∆l 2. evaluate Cd, Ld and Zc

3. Assume certain incident voltage at the kth time step

4. Use Thevenin’s equivalent to get the reflected voltages

5. Obtain incident impulses at the (k+1) time step


Discrete Models of Lumped Elements (Cont’d)

• Using a similar derivation Cd ∆l=C

u=∆l/(∆t/2)=1/ , notice that ∆t is the round-trip time

= error inductance

CL dd

Cl

tL

dd

12

2

∆∆=

lCt∆

∆=4

2

C

t

C

LZ

d

dc

2

∆==

( )C

tlLL de

4

2∆=∆=

Zc

l∆

Open circuit


Example

• Evaluate the transient response of the shown circuit

• Evaluate the current

• Evaluate the capacitor voltage

• Scattering:

• Connection:

R)ZVVi cik

Skk +−= /()2(

iZVV kci

kCk += 2

VVV ik

Ck

rk −=

VV rk

ik

=+1

V ik

V sk V C

k


Example (Cont’d)

V sk V C

k

V ik2

Open circuitOpen circuit

Zc

V rk

V ik 1+


Example (Cont’d)

Try It!


Link Model of an Inductor

• Using similar derivation to that of the capacitor we have

Ld∆l=L

Error capacitance Ce=Cd∆l=(∆t)2/L

CLtl/u dd/1=∆∆=Ll

tC

dd

12

∆∆=

t

L

C

LZ

d

dL ∆

==


Stub Model of an Inductor

• Using similar derivation we have

Ld∆l=L

Error capacitance Ce=Cd∆l=(∆t)2/(4L)

CLt/l/u dd/1)2( =∆∆=Ll

tC

dd

4

12

∆∆=

t

L

C

LZ

d

dL ∆

== 2

L

Z

l∆

L

short circuit


Example

• Evaluate the transient response of the shown circuit

Try It!


Example (Cont’d)

• Evaluate the current

• Evaluate the inductor voltage

• Scattering:

• Connection:

R)ZVVi Lik

Skk +−= /()2(

iZVV kLi

kCk += 2

VVV ik

Ck

rk −=

VV rk

ik

−=+1

VrkVrkVrkVr

ZL

VV rk

i

k−=+1

EE750 Advanced Engineering Electromagnetics Lecture 3 · EE750,2003, Dr. Mohamed Bakr 2 Special Cases in Maxwell’s Equations. •With no sources, Maxwell’s Equations are written

Documents