coupled line - even and odd mode

21
Chapter 7: Directional Coupler 1) Coupled Line 2) Even and Odd Mode 3) Coupled Line Even Mode 4) Coupled Line Odd Mode 5) Even and Odd Mode Analysis 6) Coupled Line Directional Couplers 7) Even and Odd Mode DC Voltage Analysis 8) Directional Coupler Example

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Page 1: Coupled Line - Even and Odd Mode

Chapter 7: Directional Coupler

1) Coupled Line 2) Even and Odd Mode3) Coupled Line Even Mode4) Coupled Line Odd Mode5) Even and Odd Mode Analysis6) Coupled Line Directional Couplers7) Even and Odd Mode DC Voltage Analysis8) Directional Coupler Example

Page 2: Coupled Line - Even and Odd Mode

Coupled Line - Even and Odd Mode

3 4

1 2

input through

coupled isolated

A very common type of power divider used in Microwave circuits is the coupled line. In the structure the coupling between the ports is due to the interaction of the electromagnetic fields along transmission lines which have been placed in close proximity.

Page 3: Coupled Line - Even and Odd Mode

Coupled Line - Even and Odd Mode

Coupled lines

V V V V

E wall - Odd modeH wall- Even mode

Electric wallMagnetic wall

Page 4: Coupled Line - Even and Odd Mode

Even and Odd Mode AnalysisOne method of analyzing multi-port transmission line circuits such as coupled line is through even and odd mode analysis. In this case, the circuit input voltage is split into two, an even or symmetric mode and an odd or anti-symmetric mode.The total response of the circuit can then be described as the superposition of the two separate responses (Even and Odd).

21: VVModeEven

21: VVModeOdd

Page 5: Coupled Line - Even and Odd Mode

Coupled Line - Even and Odd Mode

C11 and C22 represent the capacitor to ground for one strip (without the presence of the other). C12 is the capacitance between the two lines without any ground plane. If the strips are identical, then C11= C22.

Page 6: Coupled Line - Even and Odd Mode

Coupled Line – Even Mode

In the even mode, a virtual open circuit occurs along the axis of symmetry, which removes the C12 from the circuit. The resulting capacitance to the ground is the even mode capacitance Ce= C11= C22. If the two strips are identical, the even mode impedance Zoe can be calculated as:

ee

e

eoe vCC

LC

C

LZ

1

Page 7: Coupled Line - Even and Odd Mode

Coupled Line – Odd Mode

In the odd mode, a virtual ground forms along the axis of symmetry, which may be considered as a ground plane through the middle of C12, resulting in the capacitance as it shown above. The resulting capacitance for each conductor to the ground in the odd mode is Co: Co= C11+ 2C12. The Zoo can be calculated as:

oo

o

ooo vCC

LC

C

LZ

1

Page 8: Coupled Line - Even and Odd Mode

Coupled Lines – Even and Odd Modes

Zoe is the characteristic impedance of one of the transmission lines under even mode operation and Zoo is the characteristic impedance of one of the lines under the odd mode excitation.

The design relations for the dimensions of the transmission line for given values of Zoe and Zoo have been tabulated by Pozar, with a complete solution for the microstrip lines. But only for r = 10.

These results are required for the design of coupled line directional couplers.

Page 9: Coupled Line - Even and Odd Mode

Coupled Lines – Even and Odd Modes

Even and Odd mode characteristic impedance design data for coupled microstrip lines on a substrate with r = 10.

Page 10: Coupled Line - Even and Odd Mode

Coupled Line Directional Couplers

By using the even and odd mode analysis we can show that two coupled lines can be used as a power divider with predictable coupling ratio and isolation.

Page 11: Coupled Line - Even and Odd Mode

Coupled Line Directional Couplers

For the analysis we will use the schematic as shown in the above figure, with the excitation at port 1 and all other ports terminated in the characteristic impedance.

Page 12: Coupled Line - Even and Odd Mode

Coupled Line Directional Couplers- Even and Odd Modes

= +

Using the superposition the excitation at port 1 can be treated as the sum of the even and odd mode excitations.

Even Mode

Odd Mode

Page 13: Coupled Line - Even and Odd Mode

Coupled Line Directional Couplers- Even Mode

For the Even Mode from the symmetry we can see that:

ee II 31 ee II 42

ee VV 31 ee VV 42

Page 14: Coupled Line - Even and Odd Mode

Coupled Line Directional Couplers- Odd Mode

For the Odd Mode from the symmetry we can see that:

oo II 31 oo II 42

oo VV 31 oo VV 42

Page 15: Coupled Line - Even and Odd Mode

Even and Odd Mode Characteristic Impedances

The input impedance at port 1 can be written as:

oe

oein II

VV

I

VZ

11

11

1

1

We can calculate the even and odd input impedances for the line terminated in Zo using:

)tan(

)tan(

ljZZ

ljZZZlZ

Lo

oLoin

We can define Zine and Zin

o as:

)tan(

)tan(

ljZZ

ljZZZlZ

ooe

oeooe

ein

)tan(

)tan(

ljZZ

ljZZZlZ

ooo

ooooo

oin

Even mode input impedance. Odd mode input impedance.

Note: The line looks line a transmission line of characteristic impedance Zoe and Zoo terminated in a load impedance Zo.

Page 16: Coupled Line - Even and Odd Mode

Even and Odd Modes - DC Voltage Analysis

Now we can calculate the input voltage and current as a function of the even and odd modes input impedances:

ooin

oino

ZZ

ZVV

1

oein

eine

ZZ

ZVV

1

oein

e

ZZ

VI

1

ooin

o

ZZ

VI

1

Even mode Odd mode

Page 17: Coupled Line - Even and Odd Mode

Even and Odd Modes - DC Voltage Analysis

Substitution of these values in this equation yields:

oe

oein II

VV

I

VZ

11

11

1

1

o

ein

oin

oein

oin

oin ZZZ

ZZZZZ

2

2 2

Now if we set:

Then the input impedance at port 1 is matched. By symmetry all of the other ports are matched as well.What about the other ports voltages and currents?Can we find V3, V4 or V2?

oinoein

oin ZZZZZ 2

Page 18: Coupled Line - Even and Odd Mode

Even and Odd Modes - DC Voltage Analysis

From the even and odd mode voltage and current relations we can write:

o

oin

oin

oein

einoeoe

ZZ

Z

ZZ

ZVVVVVV 11333

V3 can also be written as a function of the input voltage and even and odd mode impedances:

lZZjZ

lZZjVV

oooeo

oooe

tan2

tan3

Page 19: Coupled Line - Even and Odd Mode

Even and Odd Modes - DC Voltage Analysis

lZZjZ

lZZjVV

oooeo

oooe

tan2

tan3

Therefore, we could derive the voltage at port 3 as a function of input voltage and even and odd mode characteristic impedances. Now if we define the Coupling Factor C as:

Then we have:

By similar reasoning:

oooe

oooe

ZZ

ZZC

ljC

ljCVV

tan1

tan23

ljlC

CVV

sincos1

12

2

2

and 04 V

Page 20: Coupled Line - Even and Odd Mode

Directional Coupler Performance

If l = /4, then 223 1 CjV

VandC

V

V

The final step is to relate the coupling factor to the even and odd mode impedances to determine the dimensions of the coupler.

C

CZZ ooe

1

1

C

CZZ ooo

1

1and

This allows us to use the even and odd mode characteristic impedance plots to determine the width and separation of the lines for a given coupling coefficient.

Page 21: Coupled Line - Even and Odd Mode

Directional Coupler ExampleDesign a 5 dB microstrip directional coupler for an r of 10

(Zo=200).

The required coupling is –5 dB,

So 5623.010 20

5

C

49.11910

87.377

1

1

C

CZZ

r

ooe

48.3310

87.105

1

1

C

CZZ

r

ooo

From the figure 1, we have:

3.0/05.0/ dWdS

S=Separation W=Width of Microstrip lines d=Dielectric thickness