Receiving antenna design » History » Version 17

SCHNEIDER, Joris, 03/23/2017 08:56 PM

1 17 SCHNEIDER, Joris
+*Previous :*+ [[Receiving antenna choice]]
2 17 SCHNEIDER, Joris
3 1 SCHNEIDER, Joris
h1. Receiving antenna design
4 2 SCHNEIDER, Joris
5 3 SCHNEIDER, Joris
As we have seen in the previous section, the double cross antenna is composed of two crossed pairs of equidistant dipoles spaced a quarter wavelength and offset 30° to the azimuth. Each dipole has a length of half a wavelength. You can see the resulting general antenna appearance below.
6 3 SCHNEIDER, Joris
7 3 SCHNEIDER, Joris
p=. 
8 5 SCHNEIDER, Joris
!{width:30%}DoubleCrossAntenna2.PNG!
9 3 SCHNEIDER, Joris
10 2 SCHNEIDER, Joris
h2. Dimensions
11 2 SCHNEIDER, Joris
12 6 SCHNEIDER, Joris
To specify the dimensions, we need to calculate the received wavelength. We calculated it for NOAA 19 (137.1MHz) and NOAA 18 (137.915MHz) to see if there is a noticeable difference on the needed dimension:
13 6 SCHNEIDER, Joris
14 6 SCHNEIDER, Joris
p=. 
15 7 SCHNEIDER, Joris
!{width:30%}Wavelength.PNG!
16 6 SCHNEIDER, Joris
17 6 SCHNEIDER, Joris
Where:
18 6 SCHNEIDER, Joris
•	λ is the wavelength (m)
19 6 SCHNEIDER, Joris
•	c is the speed of the light (m/s)
20 6 SCHNEIDER, Joris
•	f is the frequency of the received signal (Hz)
21 6 SCHNEIDER, Joris
22 6 SCHNEIDER, Joris
As the difference is very small, the antenna can be used for any NOAA satellite.
23 6 SCHNEIDER, Joris
24 6 SCHNEIDER, Joris
We can deduce the dipole length and the distance between the dipoles which is respectively half a wavelength and a quarter wavelength: 
25 6 SCHNEIDER, Joris
26 6 SCHNEIDER, Joris
p=. 
27 7 SCHNEIDER, Joris
!{width:30%}Length.PNG!
28 6 SCHNEIDER, Joris
29 6 SCHNEIDER, Joris
In compliance with these results we can model our antenna:  
30 6 SCHNEIDER, Joris
31 6 SCHNEIDER, Joris
p=. 
32 8 SCHNEIDER, Joris
!{width:70%}AntennaDesign.PNG!
33 10 SCHNEIDER, Joris
!{width:50%}AntennaDesign2.PNG!
34 6 SCHNEIDER, Joris
35 16 SCHNEIDER, Joris
The use of each component may change depending on the availability on the market
36 16 SCHNEIDER, Joris
37 2 SCHNEIDER, Joris
h2. Polarization
38 12 SCHNEIDER, Joris
39 12 SCHNEIDER, Joris
To achieve the right-hand circular polarization, the pairs are fed in phase, but one of the pairs is fed out of phase with respect to the other pair by 90°. In this project, the pair of dipoles North-South is 90° earlier than the pair West-East. 
40 12 SCHNEIDER, Joris
To fed the dipoles we need coaxial cable for each dipole. We assume that we use RG58U (velocity = 0.659) cable which is very common. The type of the cable may change depending on the availability on the market. The two cables plug at North and South should have the same length and the ones at West and East should one quarter longer. This results in the phase shift of 90° needed for the polarization.
41 12 SCHNEIDER, Joris
42 12 SCHNEIDER, Joris
p=. 
43 15 SCHNEIDER, Joris
!{width:40%}Polarization.PNG!
44 12 SCHNEIDER, Joris
45 12 SCHNEIDER, Joris
The screening braids of the North and South dipole are connected, in the same way that the ones of the East and West dipoles. The cores of the North and East dipoles are put together and linked to the mesh of the coaxial cable of the receiver. On the other hand, the cores of the South and West one are linked with the core of coaxial cable of the receiver. All the properties regarding the cables can be summarized on the picture below.
46 12 SCHNEIDER, Joris
47 12 SCHNEIDER, Joris
p=. 
48 14 SCHNEIDER, Joris
!{width:70%}Polarization2.PNG!
49 17 SCHNEIDER, Joris
50 17 SCHNEIDER, Joris
+*Next :*+ [[Receiving antenna building]]