EEM.scmA Satellite Communications A Part 3 Link planning / budgetting -Professor Barry G Evans- Autumn2004 © University of Surrey SatComms A - part 3 - B G Evans 3.1 Link budget & system planning Autumn2004 © University of Surrey SatComms A - part 3 - B G Evans 3.2 Mobile System Autumn2004 © University of Surrey SatComms A - part 3 - B G Evans 3.3 Performance • (i) QoS – b.e.r. – 10-4 if speech – 10-6 – 10-8 data (extra coding) • (ii) Availability – 95% – Channel conditions Autumn2004 © University of Surrey SatComms A - part 3 - B G Evans 3.4 Basic Transmission Autumn2004 © University of Surrey SatComms A - part 3 - B G Evans 3.5 Carrier Transmission Budget -Antenna GainThe antenna gain is defined as the ratio of the power per unit solid angle received/radiated by the antenna in a given direction to the power per unit solid angle received/radiated by an isotropic antenna supplied with the same power. Autumn2004 © University of Surrey SatComms A - part 3 - B G Evans 3.6 Basic Transmission Autumn2004 © University of Surrey SatComms A - part 3 - B G Evans 3.7 Basic Transmission Autumn2004 © University of Surrey SatComms A - part 3 - B G Evans 3.8 Antenna radiation pattern Antenna radiation pattern = gain variations as a function of the angle relative to boresight Autumn2004 © University of Surrey SatComms A - part 3 - B G Evans 3.9 Transmitted power in a given direction Autumn2004 © University of Surrey SatComms A - part 3 - B G Evans 3.10 Predicted coverage areas for the HOTBIRD satellites (a) Superbeam (b) Widebeam (courtesy of EUTELSAT) Autumn2004 © University of Surrey SatComms A - part 3 - B G Evans 3.11 Effective isotropically radiated power (EIRP) Autumn2004 © University of Surrey SatComms A - part 3 - B G Evans 3.12 Exercise (1) - Carrier Transmission Budget • Given – Power fed to antenna: PT = 10W – Antenna gain (at boresight): GTmax = 40dB – Distance: R = 36000km (earth to geostationary satellite • Calculate – Transmitter EIRP in dB(W) – Flux density at receiver in dB(W/m2) Autumn2004 © University of Surrey SatComms A - part 3 - B G Evans 3.13 Down Path Autumn2004 © University of Surrey SatComms A - part 3 - B G Evans 3.14 GEO - Geometry Autumn2004 © University of Surrey SatComms A - part 3 - B G Evans 3.15 Earth station from the geostationary orbit • • Satellite – Height h above the equator – Sub-satellite point, longitude ΦS Earth station – Latitude E, longitude ΦE – Relative longitude satellite = (ΦE – ΦS) = ΦES Autumn2004 © University of Surrey SatComms A - part 3 - B G Evans 3.16 Exercise (2) – Carrier Transmission Budget • Given – Uplink frequency = 14GHz – Eart station • Power fed to the antenna: PT=100W • Antenna diameter: D=4 (efficiency =0.6) • Location: Bercenay (France) Latitude = 48º13’07”N Longitude = 03º53’13”E – Satellite • Receiving antenna gain at boresight: GRmax=40dB • Location: 7ºE (EUTELSAT 1-F2) • Calculate – EIRP of earth station – Free space loss – Received power Autumn2004 © University of Surrey SatComms A - part 3 - B G Evans 3.17 Noise in an Earth Station G/T Ref rf Ta if Tf TD/L IPA LNA TLNA DEMOD TIPA Lo BASEBAND QoS (BER) DOWN CONV C/NOD Ts – Noise comes from: • • • • Pa Ta= picked up by antenna from outside ( kB=effective noise) Tf= lossy feeder TLNA, TIPA= amplifiers in receiver chain TD/C= down converter – Refer all noise to a reference plane into the LNA Autumn2004 © University of Surrey SatComms A - part 3 - B G Evans 3.18 Noise in a Payload G/T Ref CD Cu D/C C/Nou eirps • Noise comes from: – Antenna received noise –earth + galaxy – Feeder lossy noise (nb.290K) – Equipment noise –amps / D/C etc. added in same way as for earth station. Autumn2004 © University of Surrey SatComms A - part 3 - B G Evans 3.19 Autumn2004 © University of Surrey SatComms A - part 3 - B G Evans 3.20 Autumn2004 © University of Surrey SatComms A - part 3 - B G Evans 3.21 Noise Characterisation (1) Autumn2004 © University of Surrey SatComms A - part 3 - B G Evans 3.22 Noise Characterisation (2) Autumn2004 © University of Surrey SatComms A - part 3 - B G Evans 3.23 Noise contribution of an attenuator Autumn2004 © University of Surrey SatComms A - part 3 - B G Evans 3.24 Earth-station system G/T and noise temp. Ref Ta Tf TLNA LdB LNA GLNA TLNA TIPA TIPA TD/C IPA D/C GIPA g LNA LD/C TD/C 1 ( 1 )Tf l g LNA xg IPA 1 xTa l TIPA T DC Ts Ta (1 - )Tf TLNA ... gLNA gLNA x gIPA LdB 10log(l), α 1 l GdB 10log(g) Gain of antenna at reference (Ga - L)dB G Autumn2004 © University of Surrey T (Ga L) 10Log(Ts)d B/K SatComms A - part 3 - B G Evans 3.25 Earth station antenna noise temperature Examples (clear sky conditions) Autumn2004 © University of Surrey SatComms A - part 3 - B G Evans 3.26 Exercise (3) - Noise Contribution Budget • • • • Operating frequency = 12 GHz LNA: TLNA = 150K, GLNA = 50dB MIXER: TMX = 850K, GMX = -10dB IF AMP: TIF = 400K, GIF = 30dB • Calculate – Receiver effective input noise temperature TR – Receiver noise figure Autumn2004 © University of Surrey SatComms A - part 3 - B G Evans 3.27 Exercise (4) - G/T of C-band earth station • • • • • • • • • • Dish=15m, n=70% Ta=30K Tf=290K Loss f=0.5dB TLNA=35K GLNA=30dB FIPA=3dB GIPA=20dB TD/C=1000K Loss D/C=-10dB Feeder LNA IPA D/C if • Calculate the earth station G/T – What are the advantages of trading off dish size and LNA temp.? Autumn2004 © University of Surrey SatComms A - part 3 - B G Evans 3.28 Propagation -Effects to be considered• Radio noise • Ionospheric effects – Absorption – Total electron content effects (group delay, refraction, polarisation rotation) – Scintillation • Tropospheric effects – Attenuation by rain – Depolarisation – Refraction effects • Shadowing and multipath effects Autumn2004 © University of Surrey SatComms A - part 3 - B G Evans 3.29 Clear Sky Noise Temperature • Any ATTENUATION process which involves energy absorption is associated with THERMAL NOISE GENERATION from the medium • Absorption by atmospheric gases is frequency dependent, hence clear sky noise temperature exhibits similar variations with frequency Autumn2004 © University of Surrey SatComms A - part 3 - B G Evans 3.30 Attenuation by atmospheric gases • See CCIR Rep.719 for a detailed description of practical techniques of calculation for LAG. The following curve displays AAG(E) versus frequency; E is the elevation angle. Autumn2004 © University of Surrey SatComms A - part 3 - B G Evans 3.31 Noise temperature of the sun Autumn2004 © University of Surrey SatComms A - part 3 - B G Evans 3.32 Ionospheric effects Autumn2004 © University of Surrey SatComms A - part 3 - B G Evans 3.33 Attenuation due to rain, etc. • • • • Mist Clouds Snow Ice Autumn2004 © University of Surrey SatComms A - part 3 - B G Evans 3.34 Autumn2004 © University of Surrey SatComms A - part 3 - B G Evans 3.35 References for calculation methodology • Course notes or chapter 8 of the book • ITU-R PN 618-3 splant path rain induced attenuation and depolarisation and scintillatin (available from lending libraries or ITU, Geneva) Autumn2004 © University of Surrey SatComms A - part 3 - B G Evans 3.36 Attenuation due to precipitation and clouds Relevant techniques described in CCIR (see rep.563, 564, 721, 723) Autumn2004 © University of Surrey SatComms A - part 3 - B G Evans 3.37 Autumn2004 © University of Surrey SatComms A - part 3 - B G Evans 3.38 Autumn2004 © University of Surrey SatComms A - part 3 - B G Evans 3.39 Maps of rainfall contours (1/3) Contours of RAINFALL RATE R₀․₀₁ (mm/h) exceeded for 0.01% OF AN AVERAGE YEAR: Autumn2004 © University of Surrey SatComms A - part 3 - B G Evans 3.40 Maps of rainfall contours (2/3) Contours of RAINFALL RATE R₀․₀₁ (mm/h) exceeded for 0.01% OF AN AVERAGE YEAR: Autumn2004 © University of Surrey SatComms A - part 3 - B G Evans 3.41 Maps of rainfall contours (3/3) Contours of RAINFALL RATE R₀․₀₁ (mm/h) exceeded for 0.01% OF AN AVERAGE YEAR: Autumn2004 © University of Surrey SatComms A - part 3 - B G Evans 3.42 Nomogram for determination of specific attenuation with circular polarization use the arithmetic mean of attenuation with horizontal and vertical polarization Autumn2004 © University of Surrey SatComms A - part 3 - B G Evans 3.43 Typical values of rain attenuation Comments: 30/20 GHz systems face a problem, especially in tropical regions where rainfall rate is very high during small percentage of time. Performance objective must be achieved when rain occurs. The link will probably be over dimensioned during most of the time (margin). Autumn2004 © University of Surrey SatComms A - part 3 - B G Evans 3.44 Autumn2004 © University of Surrey SatComms A - part 3 - B G Evans 3.45 Autumn2004 © University of Surrey SatComms A - part 3 - B G Evans 3.46 Autumn2004 © University of Surrey SatComms A - part 3 - B G Evans 3.47 Autumn2004 © University of Surrey SatComms A - part 3 - B G Evans 3.48 DEPOLARISATION • Rain and ice cause this due to shape of particles – Need to know shape and orientation of particles – Linear and circular POLN different – Circular POLN is worst case – Can form a model linking depolarisation (XPD) and attenuation Autumn2004 © University of Surrey SatComms A - part 3 - B G Evans 3.49 Autumn2004 © University of Surrey SatComms A - part 3 - B G Evans 3.50 Autumn2004 © University of Surrey SatComms A - part 3 - B G Evans 3.51 Autumn2004 © University of Surrey SatComms A - part 3 - B G Evans 3.52 XPD STATISTICS Autumn2004 © University of Surrey SatComms A - part 3 - B G Evans 3.53 Raininduced XPD circular polarisation (for 1% worsth month) CO-POLAR ATTENUATION dB Autumn2004 © University of Surrey SatComms A - part 3 - B G Evans 3.54 Other tropospheric effects • Snow – Dry snow –ok (little effect) – Wet snow –as bad as rain – Problem if snow builds up on antenna • Atmospheric absorption – Gas and particle absorption (worse at low elevation angles) Autumn2004 © University of Surrey SatComms A - part 3 - B G Evans 3.55 Noise Contribution Budget -Satellite Antenna Noise Temperature-(1) Autumn2004 © University of Surrey SatComms A - part 3 - B G Evans 3.56 Noise Contribution Budget -Satellite Antenna Noise Temperature-(2) Autumn2004 © University of Surrey SatComms A - part 3 - B G Evans 3.57 Influence of Rain Autumn2004 © University of Surrey SatComms A - part 3 - B G Evans 3.58 Noise Autumn2004 © University of Surrey SatComms A - part 3 - B G Evans 3.59 Exercise (5.a) - Carrier Transmission Budget • • • • • Ta=50K, =0.9, Tf=290k Pointing loss = 0.7dB Atmospheric loss = 0.3dB Rain loss = 3dB for 99% lime Rain temp = 275K • Calculate the G/T of the earth station under worst weather conditions • Calculate the down link C/No • Calculate the down link C/N if the link bandwidth is 100KHz • Complete the link budget sheet Autumn2004 © University of Surrey SatComms A - part 3 - B G Evans 3.60 Exercise (5.b) – Link budget sheet • Link budget sheet – Downlink Satellite EIRP dBW Pointing loss dB Atmospheric loss dB Rain loss (99%) dB Free space loss dB Gain E/S dB Downlink carrier dBW E/S noise temp. dB-K E/S G/T dB/K Boltzmann constant -228.6 dBW/Hz/K Downlink noise density (NOD) dBW/Hz C/NOD dB-Hz Autumn2004 © University of Surrey SatComms A - part 3 - B G Evans 3.61 Autumn2004 © University of Surrey SatComms A - part 3 - B G Evans 3.62 Autumn2004 © University of Surrey SatComms A - part 3 - B G Evans 3.63 Autumn2004 © University of Surrey SatComms A - part 3 - B G Evans 3.64 Autumn2004 © University of Surrey SatComms A - part 3 - B G Evans 3.65 Autumn2004 © University of Surrey SatComms A - part 3 - B G Evans 3.66 Autumn2004 © University of Surrey SatComms A - part 3 - B G Evans 3.67 Autumn2004 © University of Surrey SatComms A - part 3 - B G Evans 3.68 Autumn2004 © University of Surrey SatComms A - part 3 - B G Evans 3.69 Autumn2004 © University of Surrey SatComms A - part 3 - B G Evans 3.70 Autumn2004 © University of Surrey SatComms A - part 3 - B G Evans 3.71 Autumn2004 © University of Surrey SatComms A - part 3 - B G Evans 3.72 DOWNLINK Autumn2004 © University of Surrey SatComms A - part 3 - B G Evans 3.73 UPLINK Autumn2004 © University of Surrey SatComms A - part 3 - B G Evans 3.74 Up Path Autumn2004 © University of Surrey SatComms A - part 3 - B G Evans 3.75 Exercise (6) – Up-link Cu • • • • • • • • • • • • Ku-band uplink 14GHz Dish size=5m, =0.65 Distance to satellite=38,000km Uplink atmospheric loss=0.3dB Uplink pointing loss=0.7dB Uplink rain loss=3dB Tx e/s w.g. feed loss=3dB Satellite Rx antenna gain=26dBi (from Tx e/s) Satellite Tx antenna gain=25dBi (at boresight) Rx earth station AR=-2dB Satellite Tpdr gain=120dB The satellite transponder has a single carrier saturation condition • 120dB SAT eirps PFDi=-76dBW/m2, eirp sut=50dBW The transponder’s is operated at 8dB input and 5dB output back off Calculate 1. 2. 3. The uplink HPA rating if this has to operate at 6dB back off The uplink carrier at the satellite Cu The downlink carrier eirp from the satellite Autumn2004 © University of Surrey SatComms A - part 3 - B G Evans 3.76 Characteristics of intermodulation products • The order of any intermodulation product is defined as ‘(n+m) where the IMP’s are: (n f 1 m f 2) where n, m= 1,2,3,… • • When the center frequency of the amplifier is large compared to its bandwidth, odd-order intermodulation products are the only ones falling within the useful frequency band Intermodulation product power decreases with the order of the product. So only third and fifth order intermodulation products are concerned Autumn2004 © University of Surrey SatComms A - part 3 - B G Evans 3.77 Link Performance -Intermodulation noise Intermodulation products may appear at: - the output of the transmitting earth station non linear power amplifier - the output of the satellite repeater These intermodulation products can interfere with the desired carriers, and hence be considered as noise called “intermodulation noise”. With modulated carriers, the intermodulation noise is distributed over the entire frequency band. Example: Intermodulation noise spectrum for a typical TWT with 10 carriers. (6 central carriers modulated by a multiplex of 24 telephone channels, two 64 channels carriers and two 132 channels carriers) Intermodulation products can be considered as filtered white noise with constant spectral density (No)IM Autumn2004 © University of Surrey SatComms A - part 3 - B G Evans 3.78 Autumn2004 © University of Surrey SatComms A - part 3 - B G Evans 3.79 Intermodulation • (nf1 mf2), order = (n+m) • IMP’s vary (order-1)dB/dB with carrier. – E.g. 3rd – 2dB/dB 5th – 4dB/dB • Payloads –linearisers to reduce IMP’s • Ku-band transponders – TV – 3rd order important • L/S-band transponder –1000’s small mobile carriers. 5th and 7th important Autumn2004 © University of Surrey SatComms A - part 3 - B G Evans 3.80 Total Link Operation (link from earth station to earth station) 1 – LINEAR OPERATION: PT‹(PT)max’ (NO)IM = O Repeater power gain GS is constant. Satellite transmitter output power is shared between: - amplified carriers - amplified input noise 2 – SATURATION REGION OPERATION: Available power from satellite repeater is limited. Output power is shared between: - amplified carriers - amplified input noise - intermodulation products Power gain value depends on operating point. Autumn2004 © University of Surrey SatComms A - part 3 - B G Evans 3.81 Total Link Budget -Non linear operation- Autumn2004 © University of Surrey SatComms A - part 3 - B G Evans 3.82 Interference Autumn2004 © University of Surrey SatComms A - part 3 - B G Evans 3.83 Interference Management (1) • Between Satellite and Terrestrial systems –limit PFD’s satellites and terrestrial Tx’s • Radio Reg’s –Appendix S7 • 1st stage – Calculate coordination contour – Calculate all Tx’s inside contour • 2nd stage – – – – If needed Detailed calc’s using all parameters Site shielding Energy dispersal etc. Autumn2004 © University of Surrey SatComms A - part 3 - B G Evans 3.84 Radio regulations (Appendix S7) EARTH STATION: MADLEY SAT: INTELSAT 5 LONGITUDE 3415 RX FREQUENCY: 4.18 GHZ - CO-ORDINATION CONTOUR - MODE 1 CONTOUR Autumn2004 © University of Surrey SatComms A - part 3 - B G Evans 3.85 Interference Autumn2004 © University of Surrey SatComms A - part 3 - B G Evans 3.86 Interference Management (2) • Between satellite networks • Radio Reg’s –Appendix S8 • Analyse noise increase ΔT6% (otherwise go to second detailed stage) S2 S1 I C E2 E1 Autumn2004 © University of Surrey SatComms A - part 3 - B G Evans 3.87 Total Link Budget -Non Linear OperationTotal noise at receiver input = uplink retransmitted noise + intermodulation noise + downlink noise: 1 – Assuming that all incoming carriers at repeater input have SAME POWER(as with controlled uplink power FDMA for instance): (C/N0)T-1 = (C/N0)U-1 + (C/N0)D-1 + (C/N0)IM-1+ (C/I0)U/D-1 2 – If incoming carriers at repeater input DO NOT HAVE SAME POWER: There is a CARRIER SUPPRESSION EFFECT: large power carriers tend to suppress small power carriers. Generally speaking: - for SMALL POWER carriers: (C/N0)T is smaller than in the case of equal power carriers. - for LARGE POWER carriers: (C/N0)T is larger than in the case of equal power carriers. Autumn2004 © University of Surrey SatComms A - part 3 - B G Evans 3.88 Exercise (7) – Link Performance SAT Downlink interference Uplink interference Uplink path • Given – – – – – – • Downlink path Uplink carrier power-to-noise power spectral density: Downlink carrier power-to-noise power spectral density: Carrier power-to-intermodulation noise power spectral density: Uplink carrier power-to-interference power spectral density: Downlink carrier power-to-interference power spectral density: Noise equivalent bandwidth of earth station receiver: (C/No)U=85dB(Hz) (C/No)D=83dB(Hz) (C/No)IM=87dB(Hz) (C/No)I,U=90dB(Hz) (C/No)I,D=90dB(Hz) BN=5MHz Calculate – Overall link carrier power-to-noise power spectral density: – Overall link carrier power-to-noise power ratio: Autumn2004 © University of Surrey SatComms A - part 3 - B G Evans (C/No)T (C/N)T 3.89 Total Link Budget -Non linear operation with interference Autumn2004 © University of Surrey SatComms A - part 3 - B G Evans 3.90 Autumn2004 © University of Surrey SatComms A - part 3 - B G Evans 3.91 Figure 6.11 Gains and losses in power of signals being relayed by satellite. The signal falls to about one hundred billion billionth of its strength (10-34) on each of its 25,000-mile journeys through space. This great loss is balanced by the grains of the antennas and amplifier Autumn2004 © University of Surrey SatComms A - part 3 - B G Evans 3.92 Setting out Link budgets Uplink EIRP Satellite C/Nou C/IM o C/IU C/ID C/ND Increase EIRP And Repeat Sat. Link Performance C/NTOT Requirements for QoS If Not 2-3 dB C/No.Req Margin Autumn2004 © University of Surrey =C/NTOT – C/NoReq SatComms A - part 3 - B G Evans 3.93 Types of Objectives • SIGNAL QUALITY OBJECTIVES: In terms of thresholds which must not be exceeded for more than a given percentage of time. • SYSTEM AVAILABILITY OBJECTIVES: Asys = (required time – down time) / required time Required time = period of time during which the user requires the link to be in condition to perform a required function Down time = cumulative time of link interruption within the required time Interruption is a period in which there is a complete or partial loss of signal, excessive noise, or a discontinuity or severe distortion of the signal. • PROPAGATION TIME: The overall link propagation time should not overstep a maximum value depending on the user’s requirement. Autumn2004 © University of Surrey SatComms A - part 3 - B G Evans 3.94 System Availability SYSTEM AVAILABILITY ASYS implies that the quality objectives be met during a given percentage of time (typically between 99 and 99.9%). This requires the link C/N0 ratio to be larger or equal to a given value for the considered percentage of time. C/N0 varies according to: - propagation effects (mainly influence of rain) - implementation losses (mainly antenna depointing or equipment failure) ASYS = ATX Asat Alink ARX where: ATX = transmitting earth station availability Asat = satellite availability Alink = link availability ARX = receiving earth station availability Autumn2004 © University of Surrey SatComms A - part 3 - B G Evans 3.95 Link Availability RAIN INDUCED attenuation and depolarization can reduce the C/N0 value, and cause link outage. A LARGER MARGIN value leads to a HIGHER LINK AVAILABILITY, as C/N0 will understep the required value during a shorter time interval. Autumn2004 © University of Surrey SatComms A - part 3 - B G Evans 3.96 Cost of System Availability System cost increases rapidly with system availability: CUSTOMER SHOULD NOT ASK FOR TIGHT SPECIFICATIONS, UNLESS STRICTLY NEEDED. Autumn2004 © University of Surrey SatComms A - part 3 - B G Evans 3.97 Digital Transmission Techniques -System Model- PERFORMANCE: Autumn2004 © University of Surrey - BIT ERROR RATE - BANDWIDTH SatComms A - part 3 - B G Evans 3.98 Autumn2004 © University of Surrey SatComms A - part 3 - B G Evans 3.99 Autumn2004 © University of Surrey SatComms A - part 3 - B G Evans 3.100 Time Division Multiplexing Digital signals are organized in bursts by means of buffers where bits are stored and then read at a higher clock rate. Bursts are transmitted sequentially within time slots according to a time frame structure. Autumn2004 © University of Surrey SatComms A - part 3 - B G Evans 3.101 Time Division Multiplex Standards (CCITT,Rec. G702, G732, G733): Autumn2004 © University of Surrey SatComms A - part 3 - B G Evans 3.102 Data Encryption DATA ENCRYPTION entails two aspects: - confidentiality: avoid access to message by an unauthorized party. - authentication: protection against someone changing the message content. Two types of encryption techniques: - stream cipher: each bit of the plain text is combined bit per bit with the keystream, - block ciphering: the plain text is modified block per block. Autumn2004 © University of Surrey SatComms A - part 3 - B G Evans 3.103 Scrambling • At receiver side CLOCK TIMING for bit detection is extracted from DATA SYMBOL TRANSITIONS. Long data streams of 0’s and 1’s can result in the loss of data synchronization. DIGITAL DATA CSRAMBLING at transmitter side provides a data symbol transition probability close to 0.5. At receiver side DESCRAMBLING is performed to restore original data. • SCRAMBLING also removes any periodic pattern in the baseband pulse train. Hence it CANCELS any DISCRETE LINE COMPONENT in the modulated RF spectrum. This offers better protection against overstepping the permissible level of radiated power flux density: scrambling is an ENERGY DISPERSAL technique. Autumn2004 © University of Surrey SatComms A - part 3 - B G Evans 3.104 Channel encoding Autumn2004 © University of Surrey SatComms A - part 3 - B G Evans 3.105 Decoding gain Autumn2004 © University of Surrey SatComms A - part 3 - B G Evans 3.106 Digital Speech Interpolation (DSI) • A talker has an activity factor which is less than 1. By INSERTING BITS from another channel INTO PAUSES of a given channel, DSI compresses a number m of voice channels into a SMALLER number n of satellite channels. Autumn2004 © University of Surrey SatComms A - part 3 - B G Evans 3.107 Performance objectives • Quality objectives for telephony (CCIR Rec.522) DIGITAL TRANSMISSION – a) b) c) • Quality objectives for data transfer (CCIR Rec.614) – • The BIT ERROR RATE (BER) should not exceed: 10-6, 10-minute mean value, for more than 20% of any month 10-4, 1-minute mean value, for more than 0.3% of any month c) 10-3, 1-second mean value, for more than 0.01% of any year for 64 kbit/s channels as part of ISDN: The BIT ERROR RATE (BER) should NOT EXCEED: a) 10-7, for more than 10% of any month b) 10-6, for more than 2% of any month c) 10-3, for more than 0.03% of any month No standard yet for bit rates in excess of 64 kbit/s. Likely 10-9 to 10-12. Autumn2004 © University of Surrey SatComms A - part 3 - B G Evans 3.108 Noise performance • Problems – Additive white Gaussian noise – Co-channel interference • Frequency re-use – Adjacent channel interference • From other signals – Intersymbol interference • Due to band limiting – Phase noise • From carrier recovery Autumn2004 © University of Surrey SatComms A - part 3 - B G Evans 3.109 Autumn2004 © University of Surrey SatComms A - part 3 - B G Evans 3.110 Which modulation? ASK FSK BER PSK minimum power from satellite Eb/No • Power limited satellite use B/QPSK • Mobiles need OQPSK/MSK to avoid non linear amp problems • Bandwidth limited satellite –16 QAM etc. Autumn2004 © University of Surrey SatComms A - part 3 - B G Evans 3.111 Digital transmission techniques M-PSK modulation Autumn2004 © University of Surrey SatComms A - part 3 - B G Evans 3.112 Carrier-to-noise power ratio at demodulator input The noise equivalent bandwidth BN of their receiver is assumed to be matched to the modulated carrier bandwidth B Autumn2004 © University of Surrey SatComms A - part 3 - B G Evans 3.113 BPSK QPSK 1 +/2 01 11 Vn=AWGN VR DECN VR 0 10 -/2 2 x errors Bw=1/2 BPSK Result same 00 Prob(Error) = BER SIGNAL AWGN 1 BER erfc Eb No 2 BER Rs= Rb/2 Rs= Rb • Autumn2004 © University of Surrey 1 erfc Eb No 2 QPSK is half bandwidth of BPSK • PSD in QPSK is 3dB higher SatComms A - part 3 - B G Evans 3.114 Theoretical Bit Error Probability (BEP) Autumn2004 © University of Surrey SatComms A - part 3 - B G Evans 3.115 Bit Error Probability (BEP) Useful values Autumn2004 © University of Surrey SatComms A - part 3 - B G Evans 3.116 Theoretical Bit Error Probability(BEP) Autumn2004 © University of Surrey SatComms A - part 3 - B G Evans 3.117 Carrier & Bit Error Probability (cont’d) Autumn2004 © University of Surrey SatComms A - part 3 - B G Evans 3.118 Demodulation of digital signals CONCLUSION Autumn2004 © University of Surrey SatComms A - part 3 - B G Evans 3.119 M-PSK modulation Power spectral density Autumn2004 © University of Surrey SatComms A - part 3 - B G Evans 3.120 Matched filtering Autumn2004 © University of Surrey SatComms A - part 3 - B G Evans 3.121 Autumn2004 © University of Surrey SatComms A - part 3 - B G Evans 3.122 Autumn2004 © University of Surrey SatComms A - part 3 - B G Evans 3.123 Bit Rates and Bandwidth • Example PCM coder Rb =1/2 FEC coder Rc QPSK MOD Rs – What is Rb, Rc and Rs? – If filtering is Rc, =0.5, what is the bandwidth? Autumn2004 © University of Surrey SatComms A - part 3 - B G Evans 3.124 Spectral efficiency Autumn2004 © University of Surrey SatComms A - part 3 - B G Evans 3.125 Exercise (8) – Digital Transmission Techniques satellite transponder bandwidth B=36MHz PT=10W EIRP=40dB(W) GT=30dB Free space loss L=200dB G/T=14dB(K-1) receiver bandwidth BIF • C/No = EIRP x 1/L x G/T x 1/k Given – Type of modulation: coherent QPSK (spectral efficiency r = 1.5 bits/s.Hz) – Received information bit rate: Rb = 36 Mbit/s – Required BER = 10-5 • Calculate required value of C/No and bandwidth: – 1. Without coding – 2. With coding (code rate = 3/4) – Could you use a smaller code rate (for instance 2/3 or 1/2)? Autumn2004 © University of Surrey SatComms A - part 3 - B G Evans 3.126 Power/Bandwidth trade off and coding • • • Power and bandwidth limitations are complimentary A transponder has finite bandwidth BT and hence traffic limit = BT/BC (BC = channel spacing) Bandwidth limit case A transponder has fixed power so can only support ‘n’ channels at a given QoS (ber) – Traffic limit (PTPD-Pc)=10log(n) • (Pc=power per channel) Power limit case Coding allows trade-off between bandwidth and power to optimise throughput B Rb 1 Eb Eb Power No nc No c Autumn2004 © University of Surrey SatComms A - part 3 - B G Evans 3.127 Autumn2004 © University of Surrey SatComms A - part 3 - B G Evans 3.128 Exercise (9) – Overall Link Budget • The attached link budget has been calculated for a 9.6 kb/s email service for a VSAT into a hub. The modulation used is BPSK and the coding gives a coding gain of 4dB. The desired quality of service is a BER of 10-6. • The hub available has the following parameters: – – – – – – Antenna diameter Efficiency = Feeder loss Skynoise = LNA temp Rain temp = 65% = 50K = = 4m 0.5dB 75K 275K • Fill in the missing components of the budget. Autumn2004 © University of Surrey SatComms A - part 3 - B G Evans 3.129 Exercise (9) cont’d Autumn2004 © University of Surrey SatComms A - part 3 - B G Evans 3.130 Autumn2004 © University of Surrey SatComms A - part 3 - B G Evans 3.131 Exercise A – Earth Station • An INTELSAT-A (4/6 GHz) earth-station is required to transmit two IDR carriers (eirp = 65 dBW/carrier). The specification of the station is: – G/T >35 dB/K at 5° elevation – 2 carrier IDR, intermodulation eirp is not to exceed 10dBW/4kHz. • A list of major available equipment is shown in Table next page. • The earth-station waveguide feed loss is 0.5dB on receive and 3dB on transmit. All components beyond the LNA can be neglected for noise calculation purposes and all antennas have a 70% efficiency. The output back-offs of HPAs can be taken as 10dB for multicarrier operation and the IMP eirp is given by; • E12 = 2E1 + E2 – 2(GTX – LTX) + D - SF • Where: – (GTX – LTX) is the effective atenna gain at the HPA flange. – D = (-2.PSAT – 28 + 2 x BOo)dBW2. – SF (Spreading Factor) = 20 dBW/4kHz. • Calculate the minimum cost earth-station configuration to meet the specification. Autumn2004 © University of Surrey SatComms A - part 3 - B G Evans 3.132 Exercise A – Earth Station (cont.) • List of equipment Equipment Antenna 13.0 m 15.5 m 18.0 m Cost (£k) Noise Temp 30 K 25 K 20 K HPA 125 W 400 W 700 W 160 200 300 50 60 80 LNA 33 K 55 K 80 K Autumn2004 © University of Surrey SatComms A - part 3 - B G Evans 30 6 3 3.133 Exercise B – Payload • Figure A shows a 20/30 GHz payload with specification – – – • G/T 16.5 dB/K eirp 50 dBW C/I3 20 dB The input power at the antenna receive terminals is –111 dBW. There is an input feeder loss of 1dB at a temperature of 75K. i. ii. iii. iv. Determine the noise specification for the payload. 20 GHz LNAs of gain 10, 13 and 20 dB with noise figure of 3, 4 and 5 dB respectively are available. Determine the LNA configuration to be used. Estimate whether the noise specification is achievable. Describe how you would check the linearity specification. Autumn2004 © University of Surrey SatComms A - part 3 - B G Evans 3.134