Constraints for the physical layer and RF equipment » History » Version 1
AUGER, Anne sophie, 03/23/2015 04:16 PM
1 | 1 | AUGER, Anne sophie | h1. Constraints for the physical layer and RF equipment |
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3 | 1 | AUGER, Anne sophie | h2. Constraints for the physical layer and RF equipment: |
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6 | 1 | AUGER, Anne sophie | (calcul Rb) |
7 | 1 | AUGER, Anne sophie | |
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9 | 1 | AUGER, Anne sophie | From the given allocated frequency band, the following parameters are defined: |
10 | 1 | AUGER, Anne sophie | * f : Central frequency of the emitted signal |
11 | 1 | AUGER, Anne sophie | * B: Larger of the allocated bandwidth |
12 | 1 | AUGER, Anne sophie | * EIRP: Maximum power that can be emitted in a given direction |
13 | 1 | AUGER, Anne sophie | |
14 | 1 | AUGER, Anne sophie | From the specifications, the following parameters are defined: |
15 | 1 | AUGER, Anne sophie | * Rb: Useful bit rate of the transmission |
16 | 1 | AUGER, Anne sophie | * R : Minimal distance for the transmission |
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18 | 1 | AUGER, Anne sophie | The value of these parameters constrain the parameters of the physical layer and the RF equipment for the design of the system. |
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21 | 1 | AUGER, Anne sophie | h3. Physical layer: |
22 | 1 | AUGER, Anne sophie | |
23 | 1 | AUGER, Anne sophie | The study of the physical layer will be limited to the choice of the modulation, the coding and the shaping filter. We will consider a SRRC filter (Square Root Raised Cosine) for the shaping filter as it is commonly used in telecommunication systems for its good performances. |
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25 | 1 | AUGER, Anne sophie | Then, the parameters of the physical layer are: |
26 | 1 | AUGER, Anne sophie | * M : Modulation (M=4 : QPSK, M=8 : 8PSK etc) |
27 | 1 | AUGER, Anne sophie | * rho : Coding rate (rho <1) |
28 | 1 | AUGER, Anne sophie | * alpha : roll-off of the SRRC filter |
29 | 1 | AUGER, Anne sophie | |
30 | 1 | AUGER, Anne sophie | In fact all these parameters are linked through the spectral efficiency T of the system, which is fixed by B and Rb: |
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32 | 1 | AUGER, Anne sophie | T= cst et T= |
33 | 1 | AUGER, Anne sophie | |
34 | 1 | AUGER, Anne sophie | Then, the parameters of the physical have to comply with the following relation: |
35 | 1 | AUGER, Anne sophie | |
36 | 1 | AUGER, Anne sophie | T>cst |
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40 | 1 | AUGER, Anne sophie | h3. Link budget: |
41 | 1 | AUGER, Anne sophie | |
42 | 1 | AUGER, Anne sophie | Here is the expression of the link budget: |
43 | 1 | AUGER, Anne sophie | |
44 | 1 | AUGER, Anne sophie | (link budget) |
45 | 1 | AUGER, Anne sophie | |
46 | 1 | AUGER, Anne sophie | We can notice that all the parameters are already known, except: |
47 | 1 | AUGER, Anne sophie | * (G/T): Figure of merit of the receiver (ISAE antenna) |
48 | 1 | AUGER, Anne sophie | * Lmarg: Margin on the link budget to take into account all the perturbations (antenna |
49 | 1 | AUGER, Anne sophie | depointing, atmosphere attenuation, interferences, non-ideal demodulator …) |
50 | 1 | AUGER, Anne sophie | |
51 | 1 | AUGER, Anne sophie | Lmarg being only linked to physical parameters, we don’t have any influence on it. Then, it has to be evaluated but it is not really a parameter of the design. |
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53 | 1 | AUGER, Anne sophie | Power amplifier |
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56 | 1 | AUGER, Anne sophie | h2. Conclusion: |
57 | 1 | AUGER, Anne sophie | |
58 | 1 | AUGER, Anne sophie | From these considerations, our aim will be to: |
59 | 1 | AUGER, Anne sophie | * Choose the modulation and the coding (according to the shaping filter) |
60 | 1 | AUGER, Anne sophie | * Compute the gain of the receiving antenna |
61 | 1 | AUGER, Anne sophie | * Propose some technical solution for the receiving antenna |
62 | 1 | AUGER, Anne sophie | |
63 | 1 | AUGER, Anne sophie | We will also develop tools to visualize the influence of the bandwidth, EIRP, useful bit rate and distance on the system design. |
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65 | 1 | AUGER, Anne sophie | The aircraft antenna will be considered able to fulfil the required antenna pattern, but we will not discuss about technical solutions for this antenna, as it can be really tricky. |