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The array spacing is L = sqrt( N * A / FF ). The array contains N^3^ thinsats, the array Edge is (N-1)^L^, the array mass M is 0.003kg*N^3^, the array power is approximately P = 3W*N^3^, and the main lobe ground spot diameter Gspot at 10,000 km and 4mm (38 GHz) wavelength is approximately Gspot = 40000 m^2^/(N-1)*L : The array spacing is L = sqrt( N * A / FF ). The array contains N^3^ thinsats, the array Edge is (N-1)*L, the array mass M is 0.003kg*N^3^, the array power is approximately P = 3W*N^3^, and the main lobe ground spot diameter Gspot at 10,000 km and 4mm (38 GHz) wavelength is approximately Gspot ≈ 1.22*distance*λ/D ≈ 50000 m^2^/(N-1)*L :
Line 15: Line 15:
|| 10 || 1000 || 3 || 3kW || 1.10 || 10 || 4000 ||
|| 20 || 8000 || 24 || 24kW || 1.55 || 29 || 1380 ||
|| 32 || 32768 || 98 || 98kW || 1.96 || 61 || 660 ||
|| 50 || 125000 || 375 || 375kW || 2.44 || 120 || 330 ||
|| 64 || 262144 || 786 || 786KW || 2.77 || 180 || 220 ||
|| 100 || 1000000 || 3000 || 3.0MW || 3.46 || 340 || 120 ||
|| 128 || 2.1M || 6300 || 6.3MW || 3.92 || 500 ||  80 ||
|| 10 || 1000 || 3 || 3kW || 1.10 || 10 || 5000 ||
|| 20 || 8000 || 24 || 24kW || 1.55 || 29 || 1720 ||
|| 32 || 32768 || 98 || 98kW || 1.96 || 61 || 820 ||
|| 50 || 125000 || 375 || 375kW || 2.44 || 120 || 420 ||
|| 64 || 262144 || 786 || 786KW || 2.77 || 180 || 280 ||
|| 100 || 1000000 || 3000 || 3.0MW || 3.46 || 340 || 150 ||
|| 128 || 2.1M || 6300 || 6.3MW || 3.92 || 500 || 100 ||
Line 25: Line 25:
|| 10 || 1000 || 3 || 3kW || 4.9 || 44 ||  900 ||
|| 20 || 8000 || 24 || 24kW || 6.9 || 130 || 300 ||
|| 32 || 32768 || 98 || 98kW || 8.8 || 270 || 150 ||
|| 50 || 125000 || 375 || 375kW || 11.0 || 540 || 75 ||
|| 64 || 262144 || 786 || 786KW || 12.4 || 780 || 51 ||
|| 100 || 1000000 || 3000 || 3.0MW || 15.5 || 1530 || 26 ||
|| 128 || 2.1M || 6300 || 6.3MW || 17.5 || 2200 || 18 ||
|| 10 || 1000 || 3 || 3kW || 4.9 || 44 || 1000 ||
|| 20 || 8000 || 24 || 24kW || 6.9 || 130 || 380 ||
|| 32 || 32768 || 98 || 98kW || 8.8 || 270 || 190 ||
|| 50 || 125000 || 375 || 375kW || 11.0 || 540 || 93 ||
|| 64 || 262144 || 786 || 786KW || 12.4 || 780 || 64 ||
|| 100 || 1000000 || 3000 || 3.0MW || 15.5 || 1530 || 33 ||
|| 128 || 2.1M || 6300 || 6.3MW || 17.5 || 2200 || 23 ||

Because of the depth of the array, and the distortions caused by apogee skew, the ground spot will be compressed northeast and southwest and stretched northwest to southeast.

Array Fill

Thinsats should be in continuous sunlight for maximum radio and computational power. If one thinsat shades or partially occludes the other, the result will be a loss of power, and nonuniform temperature changes. Thinsats will need to actively and cooperatively move to keep from shading each other.

The sun is 1,391,980 km in diameter, and 149,600,000 km away (on average). Its angular size is 9.3E-3 radians, or 0.53 degrees. A thinsat sized disk 20cm in diameter casts a black shadow up to 22 meters behind it, with a shaded penumbra in a narrow 0.53 degree cone widening to infinity. The penumbra cone is a meter wide 107 meters behind a thinsat, and 10 meters wide 1070 meters behind. However, the amount of shading diminishes with distance, too, though more thinsats in the front will contribute their shadows, too. Suffice it to say that thinsats in the back of the array will get somewhat less light, on average, than those in the front, and the amount of light will have ripples in it. For that reason, we cannot pack an array too densely.

The three dimensional spacing functions used in deployment will require a lot of research to optimize; they must also be compatible with a dither function that smears out grating lobes. There are some great opportunities for research here, and I hope the best functions will be developed for the public domain. However, mathematical functions are difficult to patent, and hopefully there will be an infinite number of suitable patterns, so the patent trolls will need to spend an infinite amount of filing fees to cover all of them.

We can characterize these functions by a "fill factor". Assuming a thinsat area of A = 0.024 m2, and a three dimensional array of N x N x N or N3 thinsats, and a spacing of L, then the fill factor is defined as FF = N3*A/(N*L)2 = N*A/L2. For larger arrays, with many overlapping penumbras in the back, the average illumination in the back is (1-FF), and the temperature of the thinsats will be proportional to the 4th root of that. So if the average thinsat temperature is 330K under normal conditions, it might be 310K in the back of the array with a fill factor of 0.2, and 322K with a fill factor of 0.05 . We can probably survive a fill factor of 0.2, though we must manage thermals carefully and avoid full shading.

The array spacing is L = sqrt( N * A / FF ). The array contains N3 thinsats, the array Edge is (N-1)*L, the array mass M is 0.003kg*N3, the array power is approximately P = 3W*N3, and the main lobe ground spot diameter Gspot at 10,000 km and 4mm (38 GHz) wavelength is approximately Gspot ≈ 1.22*distance*λ/D ≈ 50000 m2/(N-1)*L :

Fill factor FF=0.2, Thinsat area A=0.024

N

N3

M(kg)

P

L (m)

Edge (m)

Gspot (m)

10

1000

3

3kW

1.10

10

5000

20

8000

24

24kW

1.55

29

1720

32

32768

98

98kW

1.96

61

820

50

125000

375

375kW

2.44

120

420

64

262144

786

786KW

2.77

180

280

100

1000000

3000

3.0MW

3.46

340

150

128

2.1M

6300

6.3MW

3.92

500

100

Fill factor FF=0.01, Thinsat area A=0.024

N

N3

M(kg)

P

L (m)

Edge (m)

Gspot (m)

10

1000

3

3kW

4.9

44

1000

20

8000

24

24kW

6.9

130

380

32

32768

98

98kW

8.8

270

190

50

125000

375

375kW

11.0

540

93

64

262144

786

786KW

12.4

780

64

100

1000000

3000

3.0MW

15.5

1530

33

128

2.1M

6300

6.3MW

17.5

2200

23

Because of the depth of the array, and the distortions caused by apogee skew, the ground spot will be compressed northeast and southwest and stretched northwest to southeast.

MORE LATER

ArrayFill (last edited 2021-06-18 19:10:16 by KeithLofstrom)