Transcript Slide 1

RF Signal Cables
Amphenol RG58 coaxial cable (BNC)
Impedance 50 Ohm
Black PVC cable, tinned copper center conductor & braid
for high frequency performance
Nickel-plated connector body & Gold-plated center pin contact
Insulation: Solid PE (Polyethylene)
Rating < 500 V
Outer Diameter: 0.195 inches nominal
Velocity of Propagation: 66% (50ns/m)
Principles Meas/Electronics
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LEMO RG174 coaxial cable (LEMO)
RG59/U coaxial cable (BNC)
Stiffer than RG58
75 Ohm impedance
Dual shielded cable:
copper braid (60%) over foil
22 AWG copper covered steel center conductor
W. Udo Schröder, 2011
Impedance
50 ohms
Inner Conductor Diameter
0.48 mm
Dielectric Diameter
1.52 mm
Shield Diameter
2.23 mm
Capacitance
100.0 pF/meter (30.5
pF/foot)
Minimum Operating
Temperature
-40 C (-40.0 F)
Maximum Operating
Temperature
75 C (167.0 F)
Jacket Diameter
2.79 mm
Jacket Material
PVC
Velocity Ratio
66%
Core
stranded
Connectors for Coax Signal Cables
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BNC
Bayonet Neill-Concelman
W. Udo Schröder, 2011
Bayonet mount
locking
mechanism
LEMO
Léon Mouttet
Push-pull connectors
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HV Supply Cables
MHV connectors:
5000 volts DC and 3 amperes.
Hazards: HV on exposed central
pin, ground disconnects before
power. Do not use!
W. Udo Schröder, 2011
SHV connectors:
Do not mate to BNC connectors,
Power disconnects before ground.
Signal Transmission Lines
outer
casing
outer conductor/shield
inner conductor
dielectric
medium
z
outer conductor
5
Coaxial cables/transmission lines  traveling waves in cavity resonators
Elementary
replacement circuit
for transmission line
per unit length
Principles Meas/Electronics
U
L: inductivity C: capacity G: conductance dielectric, depend on diameter and dielectric
Wave equation ideal line
(R0, 1/G 0):
2
2
U
U

L

C

z 2
t 2
c 1
LC
Z0  L C
W. Udo Schröder, 2011
Characteristic resistance
Z0=Ohmic resistance!
For R≠0, Z0(w) complex
Impedance Z0 = 50, 75, 93 W
used for timing, spectroscopy,…
Signal propagation
speed (speed of light):
c-1  5 ns/m
Real Cables
U
For fixed frequency  :
i  t  kz 
i  t  kz 
U  z ,t   U1 e   z e 
 U2 e   z e 
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 
1
C
L
R

G

 attenuation
2 
L
C 
k   LC
wave number
c 1
propagation speed
LC
Traveling waves
Pulse distortion in long cables
Skin Effect :
 permeability  conductivity
R   
1
2

2
 1
1 



 rinner router 
RG 58 C / U :


R 10 Hz  
R 105 Hz  2.4  102 W m
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2.4 W m
W. Udo Schröder, 2011
 0    Length  
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Impedance Matching
Rd
receiver
sender
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Rload
Principles Meas/Electronics
Rd
W. Udo Schröder, 2011
Rload
For impedance matching,
Rload=Z0, cable looks
infinitely long: no
reflections from end.
For mismatch, Rload ≠ Z0,
reflection at end, traveling
back, superimpose on signal
Urefl Rload  Z0

Uin
Rload  Z0
Polarity of reflected signal Rload=0, ∞
Pulse Splitting/Adding
R1
Uin
Uout
R2
U
R1  R2 out
for slow ana log signals
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R2
Uout 
Principles Meas/Electronics
R
R
Uin
W. Udo Schröder, 2011
R
R
Uout
Uout
Uout
Z0
Z0
Z0
ZL  Matched
n  Way Splitter
R
n 1
 Z0
n 1
Also use in reverse as
3-way adder
Principles Meas/Electronics
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L
Rterm
Rload
Impedance Mismatch
Receiver input
impedance Rload ≠ Z0,
 use additional Ohmic
termination in parallel
Open end: Rload= ∞
Input and reflection
equal polarity, overlap
for t > 2Tcable
Tcable = 2L/c
L
W. Udo Schröder, 2011
Short: Rload=0, Input and
reflection opposite
polarity, superposition =
bipolar
Multiple (n) reflections attenuated by R-n
W. Udo Schröder, 2011
Principles Meas/Electronics
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