CHAPTER NINE:
COAXIAL COMPONENTS
9.1 Overview
9.2 Two-wire line
9.3 Coaxial Cables, Terminations, Connectors and
Transitions
9.4 Coaxial Attenuators:
Phase Shifters
Baluns
9.1 OVERVIEW
• The coaxial cable is a transmission line consisting of two coaxial
cylindrical conductors, separated by a dielectric (see Fig. 2.1).
• The two conductors, here shown as homogeneous, are often made of
braided small diameter copper wires.
• If Er denotes the relative permittivity of the insulator, the line
parameters are given by:
• Coaxial Cable.
• The Field Lines Of The Electric
Field Are Shown By Solid Lines,
Those Of The Magnetic Field
By Dashed Lines.
• Geometry Of The Coaxial Cable.
• The Maximum Freq For Which The Coaxial Cable Is Single Mode Is
Approximately:
• Where V (z) Is The Voltage.
• Hence The Maximum Electric Field,
Not To Be Exceeded In Order To Avoid
Sparks, Is On The Surface Of The Inner
Conductor And Has The Value:
• Worked Example
•
• Compute the parameters of a cable, with inner conductor diameter d
=1.6 mm, outer conductor diameter D = 5.8 mm, ²r = 2.3.
• Solution:
• Applying the previous formulas we get L = 0.26 µH/m, C = 99.35 pF/m,
Z∞ = 50.92 Ω, Vf /c = 1/ √ Er = 65.9%, fmax = 17.0 GHz.
• Plse kindly Very these Answers,
• The normalized maximum electric field is Emax = 485.3V/m if the voltage
V is 1V.
•Typical Coaxial Components Employed in Microwave Systems
9.2 Two-wire line
• Two-Wire Lines The two-wire transmission line consists of two parallel
cylindrical conductors of radius a separated by distance d from each other,
as shown below
• Examples of TL: (a) coaxial cable, (b) two wire line, (c) optical fiber, (d)
microstrip , (e) stripline.
• Shielded two-wire line
• To avoid the electromagnetic compatibility problems of the two-wire line,
the structure below can be used.
• Shielded two-wire line and field configuration of the symmetric (balanced)
TEM mode.
• Note That This Is A Three Conductor Line (Two Plus A Grounded One).
• In This Case There Are Two TEM Modes,
• A Symmetric (Balanced) One Where The Potentials Of The Two Inner Conductors Are
Symmetric With Respect To That Of The Outer One, Connected To Ground,
• And An Asymmetric (Unbalanced) One, With Different Parameters.
• The Parameters For The Symmetric Mode Can Be Computed From The
Following Equations:
9.2 COAXIAL CABLES, TERMINATIONS, CONNECTORS &
TRANSITIONS
COAXIAL CABLES
• The Coaxial Cable Is A Transmission Line Consisting Of Two Coaxial
Cylindrical Conductors, Separated By A Dielectric.
• The Two Conductors, Here Shown As Homogeneous, Are Often Made Of
Braided Small Diameter Copper Wires.
• The Line Parameters Are Given By:
• Coaxial Cable
• The Field Lines Of The Electric Field Are
Solid Lines Shown By ,
• Those Of The Magnetic Field By Dashed Lines.
• Observe That:
• The Electric Field Configuration Is That Of A Cylindrical Capacitor,
• Consistently With The Fact That The TEM Mode Has Zero Cutoff Frequency.
• If The Operation Frequency Increases,
• A Point Is Reached In Which Higher Order Modes Start To Propagate.
• The Maximum Freq For Which The Coaxial Cable Is Single Mode Is Approx:
• Where V (z) Is The Voltage.
• The Maximum Electric Field, Not To Be Exceeded In Order To
Avoid Sparks,
• Is On The Surface Of The Inner Conductor @ Has The Value:
• Note That, Coaxial Cable Is An Unbalanced Line,
• Meaning That,
• The Return Conductor Is Connected To Ground.
• Hence, The Voltage Of The Inner Conductor Is Referred To Ground.
• Please kindly See Worked Example in the Handout.
 Coaxial Cables
• These Are Used To:
• Transmit Electrical Energy, Or Signals, From One Location To Another, i.e.,
• To Connect A Source To A Load, Such As A Transmitter To An Antenna.
• This Is Accomplished With A Transverse Electrometic (TEM) Wave Field
Distribution Propagation Within The TL, Or Coaxial Cable,
• Governed By TL Theory.
• Coaxial Cable (Coax) Is Typically Identified Or Classified According To Its
Impedance Or Rg-type.
• E.g., A 50-ohm Coax Or An RG-8 Type Coax.
• Construction:
• A Typical Coaxial
Cable is as shown
• The Center Conductor May Be Made Of Various Materials & Constructions.
• Most Common Constructions Are Solid Or Seven-strand Conductors.
• Solid Conductors Are Used In:
• Permanent, Infrequently Handled Or Low Flex Applications &
• Stranded Conductors Are Used In Flexible Cable Appns.
• Common Materials Include:
• Copper, Tinned Or Silver Plated Copper, Copper Clad Steel & Copper Clad Aluminum, Details are in
the Handout.
•Electrical Properties:
• The Most Common Electrical Property Referred To In Coax Cable Is The
Characteristic Impedance, Or Simply Impedance.
• Coax Cable Is Typically Designed As 50 Ohm, 75 Ohm, And 93 Ohm
Depending Upon The Application.
• A Simple Formula To Determine The Impedance Of A Coaxial Is:
• The Propagation Delay in Coaxial Cable is given By:
 Physical Properties:
• The Mechanical & Physical Properties May Be Critical In Selecting The Appropriate
Cable For The Appn.
• Physical Dimensions Are Critical To Assure That An Industry Standard Connector Is
Available.
• Other Odd-size Dimensions Will Require The Use Of A Custom Termination.
• Diameter Of The Center Conductor, Core, & Jacket Are Critical Values
• Applications:
• One Of The Broadest Uses Of Coaxial Cable Is For Video Distribution.
• From Catv Signals Around The Neighborhood To Precision Digital Signals In A
Post-production Studio,
• These Signals Are Routed On 75 Ohm Coaxial Cable.
• Widely Used In Wireless & Antenna Applications,
COAXIAL TERMINATIONS
• To Avoid Confusing Reflections From The Ends Of Cables, It Is Essential
That:
• All Cables Carrying Fast Pulses Be Terminated At Their Outputs By Their
Characteristic Impedance Of 50 Ohms,
oEither With A Terminating Plug On A T-connector, Or By An Internal
Termination At The Input Of A Circuit.
• When using coaxial cables it is usually important to avoid reflections at the
end of the cable.
• If a cable is terminated with an impedance Z ,
• The ratio of the incoming voltage Vi to the reflected voltage Vr is given by:
Vr/Vi = [Z - Zo]/[Z + Zo].
• The total voltage across the terminating resistance is V = Vi + Vr.
• Three cases are of interest:
1. If Z = 0: Then Vi = - Vr and V = 0, as you would expect for a short
circuit.
2. If Z = 8: Then Vi = + Vr and V = 2 Vi.
3. If Z = Ro: Then Vi = 0 and V = Vi.
•When Z = Zo = 50 Ohms,
• The Cable Is Properly Terminated And There Is No Reflected Signal.
•Proper Termination Is Also Important For Maintaining The
Line Shape For Sharply Rising Pulses;
•If The Termination Is Not Proper,
• The Rise & Fall Times For A Square Pulse Will Be Slowed &
• The Pulse Will Be Broadened.
9.3 COAXIAL CONNECTORS
• For HF Operations The Average Circumference Of A Coaxial Cable Must Be
Limited To About One Wavelength,
• In Order To Reduce Multimodal Propagation & Eliminate Erratic Reflection
Coefficients, Power Losses, & Signal Distortion.
 Seven types of microwave coaxial connectors are described below.
• APC-3.5 The APC-3.5 (Amphenol Precision Connector-3.5 mm.
• It provides repeatable connections and has a very low voltage standing-wave
ratio (VSWR).
2. APC-7: The APC-7 (Amphenol Precision Connector-7 mm)
• Provides A Coupling Mechanism Without Male Or Female Distinction
• The Most Repeatable Connecting Device Used For Very Accurate 5o-Ohm Measurement
Applications. Its VSWR Is Extremely Low, In The Range Of 1.02 to 18 GHz.
3. BNC: The BNC (Bayonet Navy Connector) Operates Very Well At Freq Up To About 4 GHz;
• Beyond That It Tends To Radiate Electromagnetic Energy.
• The BNC can accept flexible cables with diameters of up to 6.35 mm (0.25
in.) Zo of 50 to 75 ohms.
• It is now the most commonly used connector for frequencies under 1 GHz.
Please Refer to Handout for the Remaining 4 Types
• Typical Male 50 ohm BNC connectors
• Microwave Coaxial Connectors
•COAXIAL TRANSITIONS
•
• Coaxial Transitions Are Components Used To Move From One Tx
Medium Type To A Different Tx Medium.
• This Could Be From One Waveguide Size To Another Or
• From Full Height To Reduced Height Waveguide Or From Waveguide
Tube To Coaxial Line Or From Coaxial Line To Waveguide Tube.
• Typical Examples are the transition of RF signals from:
• Coaxial Cables to Waveguides &
• From Waveguides to A Coaxial Cables
• Transition Types
Coaxial Attenuators
• A coaxial attenuator is a linear passive bidirectional TL component designed
to be inserted b/n two coaxial lines,
• In order to reduce the Pin in a matched system by a predetermined ratio without
otherwise disturbing the behaviour of the equipment.
• The ratio of input to output power is expressed in logarithmic terms where 3
dB as a power ratio is 2, 6 dB is 10, 20 dB is 100 and 30 dB is 1000 etc...
• The power absorbed by an attenuator is returned to the environment
through heat transfer by convection or conduction cooling.
• Typical Coaxial Attenuators
• Attenuator Related Parameters
• "NOMINAL ATTENUATION OR ATTENUATION VALUE:
• The nominal value of attenuation is the standard value determined by
the manufacturer.
• This parameter is a representation of the power ratio b/n the input &
the ouput of the attenuator.
• It is expressed in dB :
• P out (W) Attenuation in dB = 10 log P in (W)
• "ATTENUATION DEVIATION
• The attenuation over full specified bandwidth does not exceed
the nominal value ¦ attenuation deviation.
• This parameter is expressed in dB.
• For example, an attenuator with 6 dB nominal value and ¦ 0.3 dB
deviation
• Do not exceed 5.7dB minimum value and 6.3 dB maximum value.
• " TEMPERATURE SENSITIVITY
• The maximum change of attenuation in dB per dB per °C over the
operating temperature range.
• Example:
• If temperature sensitivity is 5.10--4 dB/dB/°C,
• For a 20 dB attenuator over a 20* 20* 5.10--4 = 0.2 dB Attenuation
Variation.
• " FREQUENCY RANGE
• The Freq range indicated for each device is the range which RADIALL
specifies the device performance.
• " AVERAGE POWER HANDLING
• It is the maximum Continues Wave input power applied for a long time at
room temperature, or at the maximum temperature of 75°C.
• That the attenuator can handle whithout permanently changing the specifications
of the component.
• Any overpowering beyond this limit can significantly alter the input power
handling of the attenuator.
• " PEAK POWER HANDLING
• It Is The Maximum Peak Power Which, When Applied At Maximum
Room Temperature Under A Pulse Of One Microsecond Every
Millisecond,
• Will Not Permanently Change The Specifications Of The Attenuator.
• Any Overpowering Beyond This Limit Will Alter The Input Power
Handling Of The Attenuator.
•Coaxial Phase Shifters
• Phase Shifters Are Used To Change The Transmission Phase Angle (Phase Of S21) Of A Network.
• Ideal Phase Shifters Provide Low Insertion Loss, & Equal Amplitude (Or Loss) In All Phase States.
• While The Loss Of A Phase Shifter Is Often Overcome Using An Amplifier Stage, The Less Loss,
The Less Power That Is Needed To Overcome It.
• Most Phase Shifters Are Reciprocal Networks,
• Meaning That They Work Effectively On Signals Passing In Either Direction.
• Phase Shifters Can Be Controlled Electrically, Magnetically Or Mechanically.
• Can Be Analogue / Digital
• Typical Coaxial Phase Shifter
• Coaxial Baluns
• A Balun Is An Electrical Device That Converts Between A Balanced Signal (Two
Signals Working Against Each Other Where Ground Is Irrelevant) & An
Unbalanced Signal (A Single Signal Working Against Ground Or Pseudo-ground).
• A Balun Can Take Many Forms & May Include Devices That Also Transform
Impedances But Need Not Do So.
• Transformer Baluns Can Also Be Used To Connect Lines Of Differing Impedance.
• The Origin Of The Word Balun Is “Balanced To Unbalanced”.
• Typical Coaxial Baluns
THE END OF
CHAPTER NINE

LECTURE No. 9.pptEngineeringEngineeringEngineeringEngineering

  • 1.
  • 2.
    9.1 Overview 9.2 Two-wireline 9.3 Coaxial Cables, Terminations, Connectors and Transitions 9.4 Coaxial Attenuators: Phase Shifters Baluns
  • 3.
    9.1 OVERVIEW • Thecoaxial cable is a transmission line consisting of two coaxial cylindrical conductors, separated by a dielectric (see Fig. 2.1). • The two conductors, here shown as homogeneous, are often made of braided small diameter copper wires. • If Er denotes the relative permittivity of the insulator, the line parameters are given by:
  • 4.
    • Coaxial Cable. •The Field Lines Of The Electric Field Are Shown By Solid Lines, Those Of The Magnetic Field By Dashed Lines. • Geometry Of The Coaxial Cable.
  • 5.
    • The MaximumFreq For Which The Coaxial Cable Is Single Mode Is Approximately: • Where V (z) Is The Voltage. • Hence The Maximum Electric Field, Not To Be Exceeded In Order To Avoid Sparks, Is On The Surface Of The Inner Conductor And Has The Value:
  • 6.
    • Worked Example • •Compute the parameters of a cable, with inner conductor diameter d =1.6 mm, outer conductor diameter D = 5.8 mm, ²r = 2.3. • Solution: • Applying the previous formulas we get L = 0.26 µH/m, C = 99.35 pF/m, Z∞ = 50.92 Ω, Vf /c = 1/ √ Er = 65.9%, fmax = 17.0 GHz. • Plse kindly Very these Answers, • The normalized maximum electric field is Emax = 485.3V/m if the voltage V is 1V.
  • 7.
    •Typical Coaxial ComponentsEmployed in Microwave Systems
  • 8.
    9.2 Two-wire line •Two-Wire Lines The two-wire transmission line consists of two parallel cylindrical conductors of radius a separated by distance d from each other, as shown below • Examples of TL: (a) coaxial cable, (b) two wire line, (c) optical fiber, (d) microstrip , (e) stripline.
  • 9.
    • Shielded two-wireline • To avoid the electromagnetic compatibility problems of the two-wire line, the structure below can be used. • Shielded two-wire line and field configuration of the symmetric (balanced) TEM mode.
  • 10.
    • Note ThatThis Is A Three Conductor Line (Two Plus A Grounded One). • In This Case There Are Two TEM Modes, • A Symmetric (Balanced) One Where The Potentials Of The Two Inner Conductors Are Symmetric With Respect To That Of The Outer One, Connected To Ground, • And An Asymmetric (Unbalanced) One, With Different Parameters. • The Parameters For The Symmetric Mode Can Be Computed From The Following Equations:
  • 11.
    9.2 COAXIAL CABLES,TERMINATIONS, CONNECTORS & TRANSITIONS COAXIAL CABLES • The Coaxial Cable Is A Transmission Line Consisting Of Two Coaxial Cylindrical Conductors, Separated By A Dielectric. • The Two Conductors, Here Shown As Homogeneous, Are Often Made Of Braided Small Diameter Copper Wires. • The Line Parameters Are Given By:
  • 12.
    • Coaxial Cable •The Field Lines Of The Electric Field Are Solid Lines Shown By , • Those Of The Magnetic Field By Dashed Lines. • Observe That: • The Electric Field Configuration Is That Of A Cylindrical Capacitor, • Consistently With The Fact That The TEM Mode Has Zero Cutoff Frequency. • If The Operation Frequency Increases, • A Point Is Reached In Which Higher Order Modes Start To Propagate.
  • 13.
    • The MaximumFreq For Which The Coaxial Cable Is Single Mode Is Approx: • Where V (z) Is The Voltage.
  • 14.
    • The MaximumElectric Field, Not To Be Exceeded In Order To Avoid Sparks, • Is On The Surface Of The Inner Conductor @ Has The Value: • Note That, Coaxial Cable Is An Unbalanced Line, • Meaning That, • The Return Conductor Is Connected To Ground. • Hence, The Voltage Of The Inner Conductor Is Referred To Ground. • Please kindly See Worked Example in the Handout.
  • 15.
     Coaxial Cables •These Are Used To: • Transmit Electrical Energy, Or Signals, From One Location To Another, i.e., • To Connect A Source To A Load, Such As A Transmitter To An Antenna. • This Is Accomplished With A Transverse Electrometic (TEM) Wave Field Distribution Propagation Within The TL, Or Coaxial Cable, • Governed By TL Theory. • Coaxial Cable (Coax) Is Typically Identified Or Classified According To Its Impedance Or Rg-type. • E.g., A 50-ohm Coax Or An RG-8 Type Coax.
  • 16.
    • Construction: • ATypical Coaxial Cable is as shown • The Center Conductor May Be Made Of Various Materials & Constructions. • Most Common Constructions Are Solid Or Seven-strand Conductors. • Solid Conductors Are Used In: • Permanent, Infrequently Handled Or Low Flex Applications & • Stranded Conductors Are Used In Flexible Cable Appns. • Common Materials Include: • Copper, Tinned Or Silver Plated Copper, Copper Clad Steel & Copper Clad Aluminum, Details are in the Handout.
  • 17.
    •Electrical Properties: • TheMost Common Electrical Property Referred To In Coax Cable Is The Characteristic Impedance, Or Simply Impedance. • Coax Cable Is Typically Designed As 50 Ohm, 75 Ohm, And 93 Ohm Depending Upon The Application. • A Simple Formula To Determine The Impedance Of A Coaxial Is:
  • 18.
    • The PropagationDelay in Coaxial Cable is given By:  Physical Properties: • The Mechanical & Physical Properties May Be Critical In Selecting The Appropriate Cable For The Appn. • Physical Dimensions Are Critical To Assure That An Industry Standard Connector Is Available. • Other Odd-size Dimensions Will Require The Use Of A Custom Termination. • Diameter Of The Center Conductor, Core, & Jacket Are Critical Values
  • 19.
    • Applications: • OneOf The Broadest Uses Of Coaxial Cable Is For Video Distribution. • From Catv Signals Around The Neighborhood To Precision Digital Signals In A Post-production Studio, • These Signals Are Routed On 75 Ohm Coaxial Cable. • Widely Used In Wireless & Antenna Applications,
  • 20.
    COAXIAL TERMINATIONS • ToAvoid Confusing Reflections From The Ends Of Cables, It Is Essential That: • All Cables Carrying Fast Pulses Be Terminated At Their Outputs By Their Characteristic Impedance Of 50 Ohms, oEither With A Terminating Plug On A T-connector, Or By An Internal Termination At The Input Of A Circuit.
  • 21.
    • When usingcoaxial cables it is usually important to avoid reflections at the end of the cable. • If a cable is terminated with an impedance Z , • The ratio of the incoming voltage Vi to the reflected voltage Vr is given by: Vr/Vi = [Z - Zo]/[Z + Zo]. • The total voltage across the terminating resistance is V = Vi + Vr. • Three cases are of interest: 1. If Z = 0: Then Vi = - Vr and V = 0, as you would expect for a short circuit. 2. If Z = 8: Then Vi = + Vr and V = 2 Vi. 3. If Z = Ro: Then Vi = 0 and V = Vi.
  • 22.
    •When Z =Zo = 50 Ohms, • The Cable Is Properly Terminated And There Is No Reflected Signal. •Proper Termination Is Also Important For Maintaining The Line Shape For Sharply Rising Pulses; •If The Termination Is Not Proper, • The Rise & Fall Times For A Square Pulse Will Be Slowed & • The Pulse Will Be Broadened.
  • 23.
    9.3 COAXIAL CONNECTORS •For HF Operations The Average Circumference Of A Coaxial Cable Must Be Limited To About One Wavelength, • In Order To Reduce Multimodal Propagation & Eliminate Erratic Reflection Coefficients, Power Losses, & Signal Distortion.  Seven types of microwave coaxial connectors are described below. • APC-3.5 The APC-3.5 (Amphenol Precision Connector-3.5 mm. • It provides repeatable connections and has a very low voltage standing-wave ratio (VSWR).
  • 24.
    2. APC-7: TheAPC-7 (Amphenol Precision Connector-7 mm) • Provides A Coupling Mechanism Without Male Or Female Distinction • The Most Repeatable Connecting Device Used For Very Accurate 5o-Ohm Measurement Applications. Its VSWR Is Extremely Low, In The Range Of 1.02 to 18 GHz. 3. BNC: The BNC (Bayonet Navy Connector) Operates Very Well At Freq Up To About 4 GHz; • Beyond That It Tends To Radiate Electromagnetic Energy. • The BNC can accept flexible cables with diameters of up to 6.35 mm (0.25 in.) Zo of 50 to 75 ohms. • It is now the most commonly used connector for frequencies under 1 GHz. Please Refer to Handout for the Remaining 4 Types
  • 25.
    • Typical Male50 ohm BNC connectors
  • 26.
  • 27.
    •COAXIAL TRANSITIONS • • CoaxialTransitions Are Components Used To Move From One Tx Medium Type To A Different Tx Medium. • This Could Be From One Waveguide Size To Another Or • From Full Height To Reduced Height Waveguide Or From Waveguide Tube To Coaxial Line Or From Coaxial Line To Waveguide Tube. • Typical Examples are the transition of RF signals from: • Coaxial Cables to Waveguides & • From Waveguides to A Coaxial Cables
  • 28.
  • 29.
    Coaxial Attenuators • Acoaxial attenuator is a linear passive bidirectional TL component designed to be inserted b/n two coaxial lines, • In order to reduce the Pin in a matched system by a predetermined ratio without otherwise disturbing the behaviour of the equipment. • The ratio of input to output power is expressed in logarithmic terms where 3 dB as a power ratio is 2, 6 dB is 10, 20 dB is 100 and 30 dB is 1000 etc... • The power absorbed by an attenuator is returned to the environment through heat transfer by convection or conduction cooling.
  • 30.
  • 31.
    • Attenuator RelatedParameters • "NOMINAL ATTENUATION OR ATTENUATION VALUE: • The nominal value of attenuation is the standard value determined by the manufacturer. • This parameter is a representation of the power ratio b/n the input & the ouput of the attenuator. • It is expressed in dB : • P out (W) Attenuation in dB = 10 log P in (W)
  • 32.
    • "ATTENUATION DEVIATION •The attenuation over full specified bandwidth does not exceed the nominal value ¦ attenuation deviation. • This parameter is expressed in dB. • For example, an attenuator with 6 dB nominal value and ¦ 0.3 dB deviation • Do not exceed 5.7dB minimum value and 6.3 dB maximum value.
  • 33.
    • " TEMPERATURESENSITIVITY • The maximum change of attenuation in dB per dB per °C over the operating temperature range. • Example: • If temperature sensitivity is 5.10--4 dB/dB/°C, • For a 20 dB attenuator over a 20* 20* 5.10--4 = 0.2 dB Attenuation Variation.
  • 34.
    • " FREQUENCYRANGE • The Freq range indicated for each device is the range which RADIALL specifies the device performance. • " AVERAGE POWER HANDLING • It is the maximum Continues Wave input power applied for a long time at room temperature, or at the maximum temperature of 75°C. • That the attenuator can handle whithout permanently changing the specifications of the component. • Any overpowering beyond this limit can significantly alter the input power handling of the attenuator.
  • 35.
    • " PEAKPOWER HANDLING • It Is The Maximum Peak Power Which, When Applied At Maximum Room Temperature Under A Pulse Of One Microsecond Every Millisecond, • Will Not Permanently Change The Specifications Of The Attenuator. • Any Overpowering Beyond This Limit Will Alter The Input Power Handling Of The Attenuator.
  • 36.
    •Coaxial Phase Shifters •Phase Shifters Are Used To Change The Transmission Phase Angle (Phase Of S21) Of A Network. • Ideal Phase Shifters Provide Low Insertion Loss, & Equal Amplitude (Or Loss) In All Phase States. • While The Loss Of A Phase Shifter Is Often Overcome Using An Amplifier Stage, The Less Loss, The Less Power That Is Needed To Overcome It. • Most Phase Shifters Are Reciprocal Networks, • Meaning That They Work Effectively On Signals Passing In Either Direction. • Phase Shifters Can Be Controlled Electrically, Magnetically Or Mechanically. • Can Be Analogue / Digital
  • 37.
    • Typical CoaxialPhase Shifter
  • 38.
    • Coaxial Baluns •A Balun Is An Electrical Device That Converts Between A Balanced Signal (Two Signals Working Against Each Other Where Ground Is Irrelevant) & An Unbalanced Signal (A Single Signal Working Against Ground Or Pseudo-ground). • A Balun Can Take Many Forms & May Include Devices That Also Transform Impedances But Need Not Do So. • Transformer Baluns Can Also Be Used To Connect Lines Of Differing Impedance. • The Origin Of The Word Balun Is “Balanced To Unbalanced”.
  • 39.
  • 40.