Title: SCTE Reverse Path Overview Carrier to Noise and Reverse Carrier loading
1SCTE Reverse Path OverviewCarrier to Noiseand
Reverse Carrier loading
- Steve DuChene
- Bright House Networks
- steve.duchene_at_mybrighthouse.com
- 1/26/2006
2What are we going to cover today
- Carrier to Noise elements in the reverse path and
how they interact with each other - Laser set up and drive parameters
- Noise Power Ratio
3Different Services require Different CNR
- HSD
- 16 QAM
- STB (VOD)
- QPSK
- Telemetry
- FSK
- Business Services
- QPSK to 16 QAM
- Modulation Type Required CNR
- Required CNR for various modulation schemes to
achieve 10E-7 BER - BPSK 12dB
- QPSK 15dB
- 16QAM 22dB
- 64QAM 28 dB
- Multiple services on the return path with
different types of modulation schemes will
require allocation of bandwidth and amplitudes. - Can be engineered.
- Requires differential padding in Headend
4Four Main Noise Areas
Drop System
Optical Plant
Coaxial Plant
Headend
5Typical Two-Way HFC CATV System?
6Carrier to Noise
7Four Main Sources of Reverse Path Noise
- Home or Business drop plant (Ingress)
- RF Ingress should be over 60 dB down but many
times it is not - Coaxal RF plant
- About 45 to 55 dB C/N-3.2 MHz BW
- (Including Amplifier Noise and Drop Ingress)
- Thermal noise only will be 54 to 58 dB the rest
is RF ingress - Optical link from the node to Headend or Hub
- About 43 to 48 dB C/N -3.2 MHz BW (For FP Laser)
- Node combining in Headend and Hub
- (Two or more nodes combined to make service
groups) - All these sources add together to make your final
C/N at the given receive system - About 35 to 40 db C/N at 3.2 MHZ BW per carrier
with up to 4 carriers
8Carrier to Noise in Coaxial Plant
9Reverse Path Unity Gain
- Unity gain in the upstream path exists when the
amplifiers station gain equals the loss of the
cable and passives upstream from that location.
In this example, the gain of each reverse
amplifier is 15 dB. The 30 MHz losses following
each amplifier are 15 dB as well. - For example, the 4 dB loss between the first and
second amplifier is all due to the cable itself,
so the second amplifier has an 11 dB output
attenuator. The amplifier input is 20 dBmV,
making the reverse amplifier module output 35
dBmV. In order to obtain unity gain and the
correct input at the first upstream amplifier
location, an 11 dB output attenuator is required
at the second amplifiers reverse output so that
the total loss equals the gain of the amplifier. - The third amplifier (far right) feeds a span that
has 3 dB of loss in the cable and another 2 dB of
passive loss in the directional coupler, for a
total loss of 5 dB. In order for the total loss
to equal the amplifiers 15 dB of gain, it is
necessary to install a 10 dB output attenuator at
the third amplifier. - In the upstream plant, the unity gain reference
point is the amplifier input.
10CATV Return Distribution Network Design
Level Values shown are at 30 MHz with a 2 port
drop splitter
Amplifier upstream input 18 dBmV
0.6 dB
0.8 dB
1.2 dB
1.3 dB
1.9 dB
125 ft
125 ft
125 ft
125 ft
125 ft
26
23
20
17
14
8
0.5 dB
0.5 dB
0.5 dB
0.5 dB
0.5 dB
125 ft splitter
125 ft splitter
125 ft splitter
125 ft splitter
125 ft splitter
125 ft splitter
5 dB
5 dB
5 dB
5 dB
5 dB
5 dB
Modem TX
49 dBmV
47 dBmV
45 dBmV
44 dBmV
43 dBmV
39 dBmV
Feeder cable 0.500 PIII, 0.4 dB/100 ft Drop
cable 6-series, 1.22 dB/100 ft
11CATV Return Distribution Network Design
Level Values shown are at 30 MHz with a 4 port
drop splitter
Amplifier upstream input 18 dBmV
0.6 dB
0.8 dB
1.2 dB
1.3 dB
1.9 dB
125 ft
125 ft
125 ft
125 ft
125 ft
26
23
20
17
14
8
0.5 dB
0.5 dB
0.5 dB
0.5 dB
0.5 dB
125 ft splitter
125 ft splitter
125 ft splitter
125 ft splitter
125 ft splitter
125 ft splitter
8.5 dB
8.5 dB
8.5 dB
8.5 dB
8.5 dB
8.5 dB
Modem TX
52.5 dBmV
50.5 dBmV
48.5 dBmV
47.5 dBmV
46.5 dBmV
42.5 dBmV
Feeder cable 0.500 PIII, 0.4 dB/100 ft Drop
cable 6-series, 1.22 dB/100 ft
12Coax Distribution Design Assumptions
- Coax Drop loss (_at_30MHz)
- Total Loss (Coax Combiner), typical max 10dB
- Distribution coax tap port loss
- Typical 21dB
- Maximum 26 dB
- Operating window is 15 to 20 dB
- Reference carrier input level
- 18dBmV
Used to calculate RF power headroom Derived from
system and industry plant design data
Taken from system plant design guide
Selected to insure a balance between operating
headroom and sufficient carrier to ingress
13Why do we run Plant and Drop RF levels as high
as possible?
- To Keep signal above plant noise ( Fairly easy)
- Thermal noise is not really a problem in reverse
plant if it is balanced properly - To keep signal above drop ingress
- (not as easy)
- The drop plant is much harder to keep a handle
on. As a rule of thumb the higher the return RF
level is the fewer ingress problems you will
have. - Coaxial plant C/N should be about 45 to 55 dB
14Thermal Noise
- Characteristic of all active components
- Optoelectronics
- Upstream amplifiers
- In-home devices
- Improper network alignment or defective equipment
can cause high levels of thermal noiseas can
improper upstream combiningwhich will degrade
carrier-to-noise ratio
15Thermal Noise
Good carrier-to-noise ratio (50 dB)
Poor carrier-to-noise ratio (12 to 15 dB)
16RF Ingress
- Upstream spectrum is shared with over-the-air
users - Short-wave broadcasts
- Citizens band (CB) radio
- Amateur (ham) radio
- Ship and aeronautical communications
- Government communications
- RF signals can enter network through cable
shielding defect
17RF Ingress
- CB radio operator had installed his own cable
outlets
18Upstream Over-The-Air Spectrum, 5-30 MHz
Source NTIA (http//www.ntia.doc.gov/osmhome/allo
chrt.pdf)
19Impulse Noise
- Most upstream data transmission errors caused by
bursts of impulse noise - Fast rise time, short duration
- Most less than 10 microseconds duration
- Significant energy content over most of upstream
spectrum - Common sources
- Vehicle ignitions, neon signs, lightning, power
line switching transients, electric motors,
electronic switches, household appliances
20Impulse Noise
- Impulse noise from arc welder in machine shop
21Reverse Laser drive and performance
22What is NPR?
- NPR Noise Power Ratio
- Is means of easily characterizing an optical
links linearity and noise contribution - NPR and CNR are related, but not the same
23DFB Laser NPR Response
NPR ?CNR Along Right-hand Side
NPR CNR Along Left-hand Side
- 7dB Optical Link
- 37MHz Loading
24 FP NPR Curves
- The NPR curve changes over temperature
- FP NPR curves shown over temperature range of -40
to 140 F
25 FP and DFB NPR Curves
- FP and DFB NPR curves at room temperature.
26Adding Carriers to the Return Path
HSD
Business Services
VOD
VOIP
27Per Carrier Power vs. Composite Power
- As you add more carriers to the return path the
composite power to the laser increases. - To maintain a specific amount of composite power
into the transmitter the carrier power must be
reduced. - When modulation schemes are changed the composite
power into the transmitter changes. - The higher the order of modulation the more peak
energy the channel contains.
28Per Carrier Power vs. Composite Power
29Per Carrier Power vs. Composite Power
30Changing Modulation Type
31Changing Modulation Type
32Determining Power Levels
- Power per Hz
- Power per Hz total power - 10log(total
bandwidth in Hz) - Channel power from power per Hz
- Channel power power per Hz 10log(channel
bandwidth in Hz)
33Power Levels
- Example Calculate the power per Hz for a
manufacturers 45 dBmV maximum laser input power
specification in the 5-40 MHz reverse spectrum
(35 MHz bandwidth) - Power per Hz Total power - 10log(total
bandwidth in Hz) - Power per Hz 45 dBmV - 10log(35,000,000)
- Power per Hz -30.44 dBmV per Hz
- -30.44 dBmV per hertz represents the maximum
power into the laser allocated over 35 MHz - Now lets calcluate what a 2MHz wide QPSK carrier
would need to be to equate to that level.
34Determining Digital Power Levels
- Example Calculate allocated channel power for a
2 MHz wide QPSK digitally modulated signal
carried in the reverse path of the previous
example. - Channel power power per Hz 10log(channel
bandwidth in Hz) - Channel power -30.44 10log(2,000,000)
- Channel power 32.57 dBmV
35Setting the Transmitter Window
- RF input levels into a return laser determine the
CNR of the return path. - Higher input better CNR
- Lower input worse CNR
- Too much level and the laser clips.
- Too little level and the noise performance is
inadequate - Must find a balance, or, set the window the
return laser must operate in - Not only with one carrier but all the energy that
in in the return path. - The return laser does not see only one or two
carriers it sees the all of the energy
(carriers) that in on the return path that is
sent to it.
36NPR Response Corrected for Optical Budget
Left side moves down 1dB
- Moving from 7 to 8dB Optical Link
- 37MHz Loading
37NPR Response Corrected for Bandwidth
Right side moves out 6.2dB for 9MHz Noise
Bandwidth
- 8dB Optical Link
- Change from 37 to 9MHz Noise Power Loading
38Signal Clipping
- RF ingress and impulse noise may cause signal
clipping - Can effect Composite power into return laser
- Excessive signals from in-home devices such as
pay-per-view converters also may cause signal
clipping - Clipping occurs in upstream amplifiers and fiber
optics equipment - FP Upstream lasers most susceptible
- Energy that can cause clipping found mostly from
5 MHz to 15 MHz range - Signals at all other frequencies are affected by
cross-compression - Cross-compression affects all upstream
frequencies - Can reduce data throughput (TCP/IP controlled
resend)
39Signal Clipping
- To avoid clipping setup return laser operational
window to recommended level - Do not adjust levels at the node once setup is
accomplished - Dont change the pad to get more RF level in the
Headend. - Dont change the pad to get better CNR at the
return RX. - Set it and Leave it.
40Optical Receivers
- Receiver input padding
- To ease the use of a wide verity of optical
receivers each with unique input power limits it
is common practice to pad the receiver input
power levels to a common sweet-spot range,
typically -7 to -8 dBm. - Receiver output level
- The receiver RF gain is adjusted to yield a
reference output level per carrier (e.g. 38 dBmV)
41Return RX Setup
- Rule of Thumb
- Do not optically attenuate the return path so all
the optical inputs are the same as the lowest. - The lower the optical input power the lower the
CNR of the receiver. - Attenuate RF internally or externally of the
device - Must have enough level so that the CMTS or other
devices receiving the signals from the return
path operate acceptably. - There can be excessive passive loss from the
output of the optical receiver to the terminating
device. - 8-way splitter/combiner 10.2 dB typical
- 4-way splitter/combiner 6.8 dB typical
- Typical input into terminating device.
- CMTS 0 dBmV
- DNCS - -3 to 27 dBmV
42Return RX Setup
- On analog returns from the node the less optical
power into a receiver the less RF you will have
on the output. - The RF levels on the output of the return
receivers should be set with internal or external
RF attenuation such that with the X level that is
placed into the forward test point on the node X
level will exist on the output of all receivers. - To much optical power can cause intermodulation
in the receiver - Typical maximum input -3 dBm newer receivers are
good to 0 dBm - Use optical attenuators on extremely short paths
or where to much optical power exists into a
receiver. Most new reverse transmitters have
higher optical output than older models - To little optical power can cause CNR problems
with that return path. - If combined with other node return receiver
outputs noise issues due to more paths can occur.
43Final C/N numbers and how they change
44Zero Point cross over Optical and Coaxial plant
are at same C/N
45Zero Point cross over Optical and Coaxial plant
are at same C/N
46C/N power adds (gets worse) faster as Coaxial C/N
and Optical C/N approach each other The zero
point is when both fiber and coaxial C/N are the
same valueDo you see the 3 db point?
Zero Point cross over Optical and Coaxial plant
are at same C/N
10 dB change here degrades C/N by 3 db
10 dB change here degrades C/N by 7 db
47Headend Combining and Other Issues
48Headend Combining
- Combining ratios (node to application Rx)
- 41, required a 6dB increase in minimum CNR and
NPR - 21, requires a 3dB increase in minimum CNR and
NPR - 11, no minimum CNR change required (this one for
16 QAM use) - Ratio planning
- 41, desirable for applications with low
subscriber densities or take-rates (e.g. VoIP,
commercial services), FPs are challenged - 21, suitable for maturing applications with
higher subscriber take-rates (e.g. HSD), FPs are
OK for lower bandwidths - 11, suitable for mature high subscriber density
and take-rate applications (e.g. HSD), FPs can
work if plant clean - Combining may vary by application!
Combining ratio, QAM index bandwidth drives
laser type selection!
49Changes to the Return PathLong Loop AGC
502-Way Applications Design Assumptions
- Supported Applications
- Number of upstream carriers
- Noise bandwidth per carrier
- QAM index (type of QAM) per carrier
- Client Device (CPE)
- Transmitter maximum output (dBmV)
- Auxiliary return amplifier gain (if required)
- Terminal Server
- Target per-carrier input power level (dBmV)
- CPE power management enabled
- Absolute minimum required CNR
Used to calculate RF payload bandwidth
Used to establish minimum low and high power NPR
Used to calculate RF power headroom
Used in X-Factor setup process
Used to select NPR targets. CableLabs specs 25dB
for DOCSIS _at_ 16QAM
51Setting up the Return Path
- Finding the X Level
- Determining the Return Transmitter Window
- Padding the Transmitter
- Return Receiver Setup
- Distribution out of the Return Receiver
- Padding the inputs to the Headend Equipment
52Setting Upstream Signal Levels
- X level or Reference level
- The easiest way to set upstream signal levels is
to establish what is called the X level. - This is a headend upstream signal level that is
the result of providing the proper level at the
input to the last reverse amplifier (the first
amplifier or node out of the headend). - To establish the X level, go to the first
downstream amplifier or node location out of the
headend. - Here you should inject a signal into that
locations reverse amplifier module input at a
level known to be correct. - This will result in a signal at the headend that
is measured and defined as the X level. - Assuming your system was designed for unity gain
operation, when you go to the next amplifier
location and inject the proper amplitude test
signal there, the resulting signal at the headend
will be the same as the original X level. - If it is not, you can make necessary adjustments
and install the proper output attenuator and
equalizer to achieve the correct upstream input
level at the first amplifier location, which will
give you the desired headend X level.
53X Level work Template
54Return Path at the Network Layer
55Changes to the Return Network
- ANY CHANGES TO THE RETURN PATH FROM THE SUBSRIBER
TO THE HEADEND CAN EFFECT ITS PERFORMANCE - Planned
- Segmentation of Return
- Changes in HE or Node
- Moving to higher order modulation such as 16 QAM
from QPSK - Un-Planned
- Bad tap
- Optronics Failure
- Ingress
- Technician Laser RF input level changes in the
field
56Conclusions
- Return system is a loop
- Changes anywhere in the loop can effect the
performance of the network - Modem outputs can vary from manufacturer to
manufacturer - Once the return laser is setup DONT TOUCH IT
- Changing the drive levels can effect the window
of operation of the laser - Work as a team to diagnose system problems
57Critical Factors Recap
- Key laser transmitter selection drivers
- QAM type establishes minimum CNR and NPR
- Combining adds to minimum CNR and NPR
- Bandwidth establishes laser response (NPR
correction) - A reference level tone (18dBmV) applied at the
node must result in the application receivers
target input level (padding of Rx inputs) - Set the node up properly and do NOT change it!
- Avoid routinely solving modem output level
problems by individually inserting return path
loss at the modem (if your doing this something
else is wrong!) - CPE power management must be enabled on this
application servers and modems - Avoid performing node setups during extremes in
outdoor temperature
58References
Steve DuChene Modeling for Advanced
Services, August 2003 Bright House Networks
Engineering Hranac, R. Linear Distortions,
Part 1 Communications Technology, July
2005 www.ct-magazine.com/archives/ct/0705/0705_li
neardistortions.htm Hranac, R. Linear
Distortions, Part 2 Communications Technology,
August 2005 www.ct-magazine.com/archives/ct/0805/
0805_lineardistortions.htm Farmer, J., D.
Large, W. Ciciora and M. Adams. Modern Cable
Television Technology Video, Voice and Data
Communications, 2nd Ed., Morgan Kaufmann
Publishers 2004 Scientific Atlanta - Reverse
path laser specification sheet 750874 Rev B,
November 2003 www.scientificatlanta.com Scient
ific Atlanta Engineering Customer Support
www.scientificatlanta.com Hranac, R. Two-way
(no impairments), October 2003 www.cisco.com