amphenol rf connector training course sept. 9, 2002

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Amphenol RF Connector Training Course Sept. 9, 2002

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Page 1: Amphenol RF Connector Training Course Sept. 9, 2002

Amphenol RF Connector Training Course

Sept. 9, 2002

Page 2: Amphenol RF Connector Training Course Sept. 9, 2002

There are basic RF questions that should be asked before helping a customer choose a connector

However, first we should discuss

• Why is it necessary to ask these questions?

• The Sales Engineer must be able to speak to the customer and understand his needs

• A basic understanding of RF as it relates to helping the customer choose a connector is essential to accomplish this

• The Sales Engineer is the means by which this information is transmitted from the customer to the design engineer

• Clear, specific information leads to quick, correct designs

Page 3: Amphenol RF Connector Training Course Sept. 9, 2002

Understanding RF and how it relates to cable and connectors

1. Transmission Lines

2. Impedance

3. Frequency Range

4. Return Loss-VSWR

5. Insertion Loss

6. Passive Intermodulation Distortion

7. Power Handling-Voltage

8. Isolation-Crosstalk

9. RF Leakage

10. Cable Assembly

11. Amphenol RF Design Engineering Support and Capabilities

Page 4: Amphenol RF Connector Training Course Sept. 9, 2002

Connector Anatomy

• What is a Connector?• A connector is a device used to connect to cables or other devices through

which electromagnetic energy is transferred from one place to another• Body-Contact-Insulator

Body

ContactInsulator

Page 5: Amphenol RF Connector Training Course Sept. 9, 2002

Connector Anatomy

Lots of changes in a very short length

Mechanical rigidity

Hold Contacts in place

Prevent Insulator rotation or lateral movement

Adapt to different cable sizes

Transform between connector series

Creates many impedance variations or discontinuities in a very short distance

Reflections are important, Attenuation not as important

Page 6: Amphenol RF Connector Training Course Sept. 9, 2002

Connector Anatomy

Various Captivation Methods

Barbs

Grooves

Shoulders

Knurls

Staking

Page 7: Amphenol RF Connector Training Course Sept. 9, 2002

Connector Anatomy

Discontinuity Compensation Steps

Dielectric Support Bead

Contact BarbSlotted Contact

Page 8: Amphenol RF Connector Training Course Sept. 9, 2002

Cable Anatomy

• What is Cable?• Cable is a transmission line through which electromagnetic energy is

propagated and transferred from one place to another• Jacket-Braid-Shield-Dielectric-Center Conductor Conductor

Dielectric

Jacket

ShieldBraid

Page 9: Amphenol RF Connector Training Course Sept. 9, 2002

Cable Anatomy

No changes in a very long length

No impedance changes or discontinuities

Usually very few reflections, but Attenuation is important

Page 10: Amphenol RF Connector Training Course Sept. 9, 2002

Assistance on the Web

Amphenol RF Newsletter

Technical Questions: http://www.amphenolrf.com/rf_made_simple/techquestions.asp

VSWR Conversion Charts: http://www.amphenolrf.com/rf_made_simple/vswr.asp

Glossary: http://www.amphenolrf.com/rf_made_simple/glossary.asp

Page 11: Amphenol RF Connector Training Course Sept. 9, 2002

# 1. Transmission Line

• What is a transmission line?• A transmission line is a conduit by which electromagnetic energy is transferred

from one place to another• Coaxial Cable- Unbalanced Line: Center conductor surrounded by a

concentric dielectric and outer conductor-Most popular type of transmission line

Page 12: Amphenol RF Connector Training Course Sept. 9, 2002

# 1. Transmission Line

•What is a transmission line?•A transmission line is a conduit by which electromagnetic energy is transferred from one place to another

•Waveguide: Rectangular, Circular

Page 13: Amphenol RF Connector Training Course Sept. 9, 2002

# 1. Transmission Line

•What is a transmission line?•A transmission line is a conduit by which electromagnetic energy is transferred from one place to another

•Planar Transmission Line: Microstrip, Stripline, Coplanar waveguide are most common

Page 14: Amphenol RF Connector Training Course Sept. 9, 2002

# 1. Transmission Line

•What is a transmission line?•A transmission line is a conduit by which electromagnetic energy is transferred from one place to another

•Twin Line- balanced line: two parallel conductors separated by a dielectric

. .

Page 15: Amphenol RF Connector Training Course Sept. 9, 2002

# 1. Transmission Line

• The type of transmission line will determine the connector style

• Cable Connector-Coaxial Cable, Twin Line• Surface Mount Connector-Microstrip• Tab Launch Connector-Microstrip, Stripline, Coplanar• End Launch Connector-Microstrip, Coplanar• Pin Launch Connector-Microstrip, Stripline, Coplanar

Page 16: Amphenol RF Connector Training Course Sept. 9, 2002

# 2. Impedance

Ohm’s Law

Page 17: Amphenol RF Connector Training Course Sept. 9, 2002

# 2. Impedance

• What is the Characteristic Impedance?• The ratio of Voltage to Current at any point in a transmission line• A transmission line can be represented as shown, with the values of C. L,

R, and G determining the impedance

Coaxial Line Equivalent Circuit

Page 18: Amphenol RF Connector Training Course Sept. 9, 2002

# 2. Impedance

•50 and 75 Ohms are the most common impedances•Do not confuse impedance with LOSS: •A 50 ohm impedance does not have less loss than a 75 ohm impedance. It is not like resistance•Impedance is independent of the length of the cable or connector•Impedance is independent of frequency

•The Impedance will help determine the connector series•Some series are only one impedance: C, SC, HN, 7-16•Some series can be both 50 or 75 ohms: BNC, TNC, N

Page 19: Amphenol RF Connector Training Course Sept. 9, 2002

# 2. Impedance

•Impedance of Coaxial Cable: Zo=(138/(E))*log(D/d))= (L/C)•L=.0117*Log (D/d) uh/inch C=.614*E/Log (D/d) pf/inch

•Characteristic Impedance is determined by the geometry and dielectric constant of the transmission line

Page 20: Amphenol RF Connector Training Course Sept. 9, 2002
Page 21: Amphenol RF Connector Training Course Sept. 9, 2002
Page 22: Amphenol RF Connector Training Course Sept. 9, 2002
Page 23: Amphenol RF Connector Training Course Sept. 9, 2002

# 2. Impedance

Page 24: Amphenol RF Connector Training Course Sept. 9, 2002

# 2. ImpedanceImpedance: The impedance of the connector generally must match that of the transmission line

Non-Constant 50, 75 ohm 50 ohm 75 ohmBNC Twinaxial BNC 7/16 1.6/5.6

UHF SMB C, SC, HN Type F

Twinaxial MCX Mini-UHF Type G

1.0/2.3 MMCX

TNC SMA

N

Outer Diameter Inner Diameter Dielectric Constant Impedance

.063 .020 2.0 50 Ohms

.063 .012 2.0 75 Ohms

.276 .120 1.0 50 Ohms

Page 25: Amphenol RF Connector Training Course Sept. 9, 2002

# 3. Frequency Range• Frequency is the number of electromagnetic waves that pass a given

point in 1 second• Hertz is the unit of frequency measurement• Generally, the RF performance of a connector degrades as the

frequency is increased (c=f)• Wavelength decreases, therefore smaller disruptions cause more problems

• Specifying the frequency will make it easier for the design engineer to optimize the performance

• Whenever possible, don’t specify a high frequency connector when a low frequency connector will work do the job

Page 26: Amphenol RF Connector Training Course Sept. 9, 2002

# 3. Frequency Range

• If a frequency range is not specified, then the connector will be designed to catalog specs and this could cause the design process to take a lot longer

• For example-A customer needs a new SMA to operate up to 12 Ghz. The catalog specifies 18 Ghz for some SMA connectors. If the connector is optimized for 18 Ghz, it will likely take a lot longer than necessary to design

• Give as much information about the application of the connector to the design engineer as possible

• Is it used in a high power, narrow frequency band amplifier?• Is it used in a band pass filter?

Page 27: Amphenol RF Connector Training Course Sept. 9, 2002

# 3. Frequency Range

Giga = 1,000,000,000 Billion

Mega = 1,000,000 Million

Kilo = 1,000 Thousand

Milli = 1/1000 One thousandth

Micro = 1/1,000,000 One millionth

Nano = 1/1,000,000,000 One billionth

Pico = 1/1,000,000,000,000 One trillionth

Page 28: Amphenol RF Connector Training Course Sept. 9, 2002

Some Typical Frequencies:

House current 60 Hz in the US (50 Hz in many other countries)

AM Radio 500 - 1500 kHz

Shortwave Radio 10 MHz

TV (channels 2-13) 60 - 250 MHz

Cellular Phone 824 - 894 MHz

Digital (PCS) Phone 1850 - 1990 MHz

Radar 6 - 26 GHz

Direct Broadcast Satellite (DBS) 12 GHz

Page 29: Amphenol RF Connector Training Course Sept. 9, 2002

Frequency Chart (GHz)

Page 30: Amphenol RF Connector Training Course Sept. 9, 2002

# 4. Return Loss or VSWR

• A measure of how much power is reflected Return Loss: The portion of a signal that is lost due to a reflection of

power at a line discontinuity. Return Loss is similar to VSWR and is generally preferred in the CATV industry to a VSWR specification

• VSWR: Acronym for Voltage Standing Wave Ratio. VSWR is the ratio of voltage applied to voltage reflected. It is the major factor contributing to the total signal efficiency of the connector.

• Best performance is achieved when the impedance of the cable and the connector are the same (matched)

Page 31: Amphenol RF Connector Training Course Sept. 9, 2002

# 4. Return Loss or VSWR• Reflections are created by deviations from the characteristic impedance caused by:

•variations in machining tolerances•Variations in the dielectric constants of insulators•transitions within the connector:

•transitioning from the cable size or stepping the connector from one line size to another line size

Page 32: Amphenol RF Connector Training Course Sept. 9, 2002

# 4. Return Loss or VSWR

• Reflection Coefficient is the basic measure of reflection: r=abs(Zo-Zl/Zo+Zl) where Zo is the characteristic impedance and Zl is the actual impedance

• Generally, this is the most important RF figure of merit for a connector

• VSWR=(1+r)/(1-r)• Return Loss=-20*log (r), in dB (decibels)• These are all the same thing, just expressed in different ways• Return Loss and VSWR are most commonly used

Page 33: Amphenol RF Connector Training Course Sept. 9, 2002

ComponentCable

Power transmittedinto componentIncident Power

Reflected Power

Return Loss = Ratio of reflected to incident power in dB

VSWR = Ratio of maximum to minimum electric field (Voltage)

Page 34: Amphenol RF Connector Training Course Sept. 9, 2002

Relative Magnitudes:Power Power Transmitted ReturnReflected into Component Loss VSWR

1% 99% 20 dB (1/100=10-2) 1.25

5% 95% 13 dB 1.58

10% 90% 10 dB (10/100=10-1) 1.95

50% 50% 3 dB 5.80

• Try to get a realistic idea of the Return Loss really required for a specific application

• Trying to design very low VSWR connectors, when not really needed, can take a long time and can add to the cost

Page 35: Amphenol RF Connector Training Course Sept. 9, 2002

dB Notation Increase Decibel (dB)of Signal Equivalent

1 = 100 = 0dB

2 = 100.3 = 3dB

10 = 101 = 10dB

20 = 101.3 = 13dB

100 = 102 = 20dB

1000 = 103 = 30dB

1/10 = 10-1 = -10dB

1/100 = 10-2 = -20dB

1/1000 = 10-3 = -30dB

Rather than say “The gain of the amplifier is 100 times”,

we say, “The gain is 20 decibels.”

Page 36: Amphenol RF Connector Training Course Sept. 9, 2002

# 5. Insertion Loss

• Insertion Loss is expressed in dB, and is a measure of the total loss of power going through a device

• IL = -20*log (Pout/Pin)• Includes losses due to reflection (usually the dominant factor unless the Return

Loss is very low <-26 dB), plus losses due to the dielectric and metal conductors (Attenuation)

• Long Cable assembly-Connector insertion loss not usually significant• Short cable assembly- Connector insertion loss can be significant

• Typically, connector insertion loss is very small (.1-.25 dB)

Page 37: Amphenol RF Connector Training Course Sept. 9, 2002

# 5. Insertion Loss

•As frequencies increase, the insertion loss increases (as a square law function (P=E^2/Z)

•Most of the electromagnetic energy (current) travels through the conductors in a circumferential ring

•Most of it in center conductor, but there is some impact from outer conductor

•Current flow is restricted to the surface layer or “skin” of the conductor

• Approximately 98% of the current density travels within 4.6 skin depths

Page 38: Amphenol RF Connector Training Course Sept. 9, 2002

# 5. Insertion Loss

• The length of the connector and the materials chosen will impact the insertion loss

• shorter is better• Plate the conductors with a high conductivity material

• Nickel-Inexpensive, hard material with good conductivity, but high relative permeability resulting in higher insertion loss

• Gold-Hard material and an excellent conductor, but expensive• Silver-Excellent conductor, less expensive than gold, better

permeability than nickel, but softer, and tarnishes• Stainless Steel-Rugged material for small connectors such as SMA,

but steel has high relative permeability

Page 39: Amphenol RF Connector Training Course Sept. 9, 2002

# 5. Insertion Loss

Page 40: Amphenol RF Connector Training Course Sept. 9, 2002

# 6. Passive Intermodulation Distortion• Not well known until mid 1990’s

• Primarily concern to satellite, microwave relay industries

• Modern Frequency plans

• High Power levels

• Sensitive Receivers

• Spurious Signals created by non-linear mixing of 2 or more

frequencies in a passive device

• Active PIM-generated by amplifiers-is reduced by filtering

• Passive PIM-filtering not possible

• Common to many channels

• Must be low PIM designs

Page 41: Amphenol RF Connector Training Course Sept. 9, 2002

# 6. Passive Intermodulation Distortion

• Spurious Signals created by non-linear mixing of 2 or more

frequencies in a passive device

• PIM products fall in receive (uplink) band

• Block Channels

• 3rd order generally greatest amplitude

• 5th and 7th may be of concern

• fIM = mf1 +/- nf2

• (2f1-f2), where m = 2 and n = 1 is a 3rd order product

Page 42: Amphenol RF Connector Training Course Sept. 9, 2002

# 6. Passive Intermodulation Distortion

F1 = 930 Mhz and F2 = 955 Mhz, then Fim = 905 Mhz

Page 43: Amphenol RF Connector Training Course Sept. 9, 2002

# 6. Passive Intermodulation DistortionBase Station Antenna Systems

•Simplex-

•Most prone to PIM effects

•Most economical

•Duplex

•Less Prone to PIM

•More expensive

•Cross Polarization

•Least PIM susceptible

•May require more space

Page 44: Amphenol RF Connector Training Course Sept. 9, 2002

# 6. Passive Intermodulation Distortion

•dBm-measure of power relative to 1 milliwatt

•dBc-measure of dB below a specified carrier level

•+43 dBm input

•PIM: -120 dBm

•Spec: -163 dBc

•Common Spec is -143 to -163 dBc (-100 to -120 dBm)

Page 45: Amphenol RF Connector Training Course Sept. 9, 2002

# 6. Passive Intermodulation Distortion• Causes of PIM

• Poor Contact Junctions-Non linear rectifying

• Solder outer-Solder inner- over molded design are best

• Most stable

• Ferromagnetic materials-Non-linear hysteresis

• No Nickel, Stainless Steel

• Contamination

• Types of Connectors

• 7-16 DIN

• Type N

• TNC-Occasionally

• Never use Bayonet (BNC) or Push on styles

Page 46: Amphenol RF Connector Training Course Sept. 9, 2002

# 7. Power Handling Capability

• There are 2 types of power handling (expressed in watts) that must be considered

• Average Power• Peak Power

• Average Power-the input power to a cable/connector which will produce a maximum safe center conductor temperature under steady state conditions when terminated with a matched load. A safe center conductor temperature is one that will not melt the dielectric

Page 47: Amphenol RF Connector Training Course Sept. 9, 2002

# 7. Power Handling Capability

• Average Power is inversely proportional to frequency and must be derated accordingly

• Average Power=Power Rating @ 1 Mhz/ (Frequency in Mhz)

• Connectors generally have higher power ratings than the cable to which they are attached

• They have metal shell-cables have braids covered by plastic jackets• They can be attached to bulkheads which help dissipate heat• They usually have lower attenuation per unit length due to air

sections within the connector

Page 48: Amphenol RF Connector Training Course Sept. 9, 2002

# 7. Power Handling Capability

• Peak Power-is limited by the voltage rating of the connector. The peak power is determined by the equation V^2/Z where V=the peak voltage rating and Z is the characteristic impedance

• Peak Power is not a function of frequency• Peak Power is an inverse function of VSWR and modulation schemes

and must be derated• Peak and Average Power are functions of altitude and must be derated

accordingly• Maximum power ratings will always be the lesser of the

cable/connector combination

Page 49: Amphenol RF Connector Training Course Sept. 9, 2002

Max. Operating Voltage (volts) Used to determine Peak Power Ratings

Page 50: Amphenol RF Connector Training Course Sept. 9, 2002

# 8. Isolation-Crosstalk

• Isolation and Crosstalk are used interchangeably• They are a measure of how much signal is picked up by an adjacent

line• Ganged style connectors on PC boards• Harnessed or “parallel run” cable assemblies

• They are measured in dB and usually range from –60 to –100 dB• If frequency increases or the length of the lines increase, crosstalk gets

worse• If the distance between the lines increases, crosstalk gets better

Page 51: Amphenol RF Connector Training Course Sept. 9, 2002

# 8. Isolation-Crosstalk

There will be significant crosstalk between the lines on this ganged connector unless some precautions (such as shielding) are taken

Page 52: Amphenol RF Connector Training Course Sept. 9, 2002

Question # 9. RF-Leakage

• RF Leakage is a measure of how much signal leaks out from a connector in dB at both the interface and at the cable entry

• As frequency increases, the leakage gets worse• Typical RF Leakage values range from –40 dB for Push-On types to

-90 dB for threaded styles on Semi Rigid cables• Generally not a big concern except if epoxy captivation is used

Page 53: Amphenol RF Connector Training Course Sept. 9, 2002

#10: Is the connector used on a cable assembly

• 2 connectors separated by a distance on a cable• At specific frequencies, all of the reflections can add up

(both connectors and cable)• When specifying a connector for a cable assembly, the cable

assembly requirements must be known• Catalog connectors, even if performance levels meet MIL Spec

requirements, may not be able to perform to the cable assembly specifications

Page 54: Amphenol RF Connector Training Course Sept. 9, 2002

#10: Is the connector used on a cable assembly

• Calculate the total worst case VSWR by multiplying all of the VSWR’s: For example- The cable assembly specification is 1.45 maximum

• 1st connector VSWR=1.25• 2nd connector VSWR=1.15• Cable VSWR=1.05• Total worst case VSWR=1.25*1.15*1.05=1.51

• Choosing a catalog BNC connector with a VSWR=1.25 and a catalog SMA connector with a VSWR of 1.15 obviously won’t work. Special connectors are needed.

Page 55: Amphenol RF Connector Training Course Sept. 9, 2002

#10: Is the connector used on a cable assembly

Page 56: Amphenol RF Connector Training Course Sept. 9, 2002

#11: How can Amphenol RF adequately support the design and development of high performance, RF

connectors?• RF Design Capabilities

• ANSOFT High Frequency Structure Simulator

• Test Capabilities-Design Verification

• Network Analyzers• PIM Test Capabilities

Page 57: Amphenol RF Connector Training Course Sept. 9, 2002

RF Simulation Capability• ANSOFT 3D High Frequency Structure Simulator

• Model any Geometry

• No Frequency Limitation

• S Parameter Analysis

• Return Loss, VSWR, Insertion Loss etc.

• Radiated Power

• E Field Plots

• Time Domain Analysis

• Optimization Capability

Page 58: Amphenol RF Connector Training Course Sept. 9, 2002

RF Simulation Capability• The connector is designed using standard RF practices and 2D linear analysis

programs for “ballpark” performance

• Calculate impedances within the connector

• Calculate nominal compensation steps within the connector

• Draw the problem in HFSS-import from PRO-E: IGES (3D), or DXF (2D)File

• Assign the materials

• Set the ports and boundary conditions (symmetry)

• Solve

• Analyze frequency and time domain plots

Page 59: Amphenol RF Connector Training Course Sept. 9, 2002

RF Simulation Capability

Draw the RF Model from the Mechanical drawing

Page 60: Amphenol RF Connector Training Course Sept. 9, 2002

RF Simulation Capability

Plot the desired S Parameters

Page 61: Amphenol RF Connector Training Course Sept. 9, 2002

RF Simulation Capability

View Time Domain response to determine the location of impedance mismatch

Page 62: Amphenol RF Connector Training Course Sept. 9, 2002

RF Simulation Capability

•All design changes are made on the computer (No

samples made until the design is optimized)

•Simulations in a matter of minutes, or hours at most

•Numerous iterations in a matter of hours or days

•Final modifications (if needed) made after testing

Page 63: Amphenol RF Connector Training Course Sept. 9, 2002

Surface Mount Connector on Microstrip

Connector has excellent Return Loss (-35 to –40 dB)

When mounted on board, performance deteriorates (-20 dB) due to the mismatch at the launch

Customer must supply board

characteristics:

1. Thickness

2. Trace width

3. Material (dielectric constant)

4. Transmission line type (i.e.. Microstrip, stripline)

Page 64: Amphenol RF Connector Training Course Sept. 9, 2002

Surface Mount Connector on MicrostripInitial simulation results

Return Loss Insertion Loss

Page 65: Amphenol RF Connector Training Course Sept. 9, 2002

Surface Mount Connector on Microstrip

.010 wide .015 wide .022 wide

Modify launch area to reduce the negative (capacitive)

discontinuity at the launch area

Time Domain

Capacitance due to launch

Page 66: Amphenol RF Connector Training Course Sept. 9, 2002

Surface Mount Connector on Microstrip

Able to achieve a significant improvement in Return Loss and Insertion Loss by modifying the launch area

Return Loss Insertion Loss

Final Return Loss

Final Insertion Loss

Page 67: Amphenol RF Connector Training Course Sept. 9, 2002

Antenna Isolation Board

• Design Capabilities are not limited to connectors• Can model and simulate entire assemblies• Example:

• MCX angle PC connector on a capacitively coupled microstrip board

• 4” of RG-316 cable• Straight MCX connector and angle MCX PC connector on ends of

cable

Page 68: Amphenol RF Connector Training Course Sept. 9, 2002

919-101P-51SX

4” RG-316/U

47pf, 4000 V, capacitor

Board, Top View

.115 wide trace

.063 thick, FR4

Antenna Isolation Board

919-134C-51P1X

919-119J-51AX

Page 69: Amphenol RF Connector Training Course Sept. 9, 2002

47 pf Cap, 4000 V, capacitor

Ground PlaneBoard, Bottom View

Antenna Isolation Board

Page 70: Amphenol RF Connector Training Course Sept. 9, 2002

Return Loss

Insertion Loss

Spec: -15 dB Return Loss and -1.5 dB Insertion Loss at 900 Mhz

Antenna Isolation Board (Simulated vs. actual test results)

Page 71: Amphenol RF Connector Training Course Sept. 9, 2002

Example: Angle Plug for LMR400 Cable VSWR Improvement

Contact too close to body

5 mm Diameter too small (35 ohm impedance)

ANSOFT HFSS Model

Initial VSWR

Page 72: Amphenol RF Connector Training Course Sept. 9, 2002

Angle Plug for LMR400 Cable VSWR Improvement

Recommended Design Changes

1. Remove Chamfer at solder post on contact

2. Increase 5mm diameter to 6.3 mm diameter on Body

ANSOFT Model

Increase diameter to 6.3 mm

Remove chamfer and shorten contact by 1.25 mm

Final improved VSWR

Page 73: Amphenol RF Connector Training Course Sept. 9, 2002

Test Capability-S Parameters

• State of the art Network Analyzers• HP 8510: 26.5 Ghz Vector Network Analyzer• HP 8753D: 50 Ohm 6 Ghz Vector Network Analyzer• HP 8753D: 75 Ohm 3 Ghz Vector Network Analyzer

Return Loss Insertion Loss VSWR Crosstalk RF Leakage

Page 74: Amphenol RF Connector Training Course Sept. 9, 2002

Vector Network Analyzer (S Parameter Measurements)

RF Leakage Test chamber

Page 75: Amphenol RF Connector Training Course Sept. 9, 2002

Passive Intermodulation Distortion Testing

• There are no “high tech” computer programs to predict IMD performance

• Devices must be built and tested• State of the art measurement test set using 20 watt (+43 dbm)

signals with a system noise floor of -130 to -135 dbm• Computer Automated-in house programming capabilities to

customize test measurements• Typical specifications of –116 to –120 dBm for 7-16 and Type N

connectors on helical and annular cables

Page 76: Amphenol RF Connector Training Course Sept. 9, 2002

PIM Testing – Cont’d

Page 77: Amphenol RF Connector Training Course Sept. 9, 2002

PIM Testing – Cont’d

Computer Control (HP VEE Interface)

Page 78: Amphenol RF Connector Training Course Sept. 9, 2002

How to Select an RF Connector Select a connector based on the information learned from

asking questions about the 10 RF parameters:1. Impedance Typical impedance of a system is 50 or 75 ohm. See Overview in catalog for impedance by series.2. Frequency Range Connector series range from 100 MHz to 26.5 GHz. See Overview in catalog for frequency range by series.3. Cable Type Connector series are designed to terminate to a limited number of cable types. Is it a new cable required by the customer? Is it a PC style? See the “Cable Selection Chart” in the catalog.4. Electrical/Mechanical requirements VSWR, Voltage Rating, Temperature Range, and other environmental requirements are all key specifications.5. Coupling Type Choose between Threaded, Bayonet, Snap-on, and Push-pull based on all of the above.

Page 79: Amphenol RF Connector Training Course Sept. 9, 2002

Use all of the information gathered to make a final decision

• Coupling style• Frequency range: 6 Ghz• Power Handling: 5 Watts Average• RF Leakage: -70 dB (Eliminates Push on or

Bayonet styles)• PIM requirements: -None

• Connector style• Impedance: 50 Ohms• Return Loss: -20 dB• Insertion Loss: -.1 dB• Mechanical Restrictions

• Available Real Estate: .5 “ long• Cable: RG-142

• Cost, other mechanical requirements, etc.

N, TNC, SMA, 7-16

SMA, TNC

Final Connector Choice