MORE ABOUT OBLONGS 2

by Slobodan Bukvic, YU7XL, yu7xl@nadlanu. com

 

In the last Dubus issue, I described a super oblong antenna for 1296 MHz. Now, I am going to describe two models of oblong for 432 MHz.

As I previously said, thinner element wire gives better antenna performance. I have found that by comparing different models I made. Higher gain, better side lobe suppression, and much wider range of frequency are always seen with thin elements, if the boom is long enough. This is, unfortunately, just in theoretical. In practice, the losses due to material resistance increases as element diameter gets smaller. Bellow a certain diameter, the losses become too high, and all benefits in theoretical performance are lost.

I have made a better design for 1296 MHz, than I previously described. The same number of elements, and approximately same boom length gives even 0,5 dB more gain and G/T. However, the losses are so high, that this antenna is worse in reality.

We could also talk about antenna temperature. Higher losses involve higher temperature, and the situation is quite comparable with dish antenna and its D/f ratio. Therefore, the higher gain antenna (with higher loss) could be better for transmitting purposes, but not for receive.

I do not intend to elaborate too much about this. My simple idea is: the better G/T ratio, the better antenna. That phylosophy has already been proven by YU7EF with hid yagi antenna. This means: low temperature and low losses, combined with bigger bandwidth and better G/T, though gain is sacrificed a little.

Let me mention the sky and earth temperatures are much lower on 432 compares to 144 MHz. Therefore, we adopt an average Tsky to be 15 Kelvin and Tearth 290 Kelvin. Derived from this, good antenna temperature is much more important on 432 MHz than it is on 144 MHz.

I have made nearly a hundred models of oblong for 432 MHz, trying to discover the best ratio between oblong element height and width, and found the best value of the element height h=0,05 to 0,1 wavelengths. I also discovered that the best oblongs can be achieved for the boomlength in the range of 10 to 20 wavelengths. In this area, the oblong is much better than the yagi! Here is the proof. The table shows performances of the original EF7032 yagi made by YU7EF versus my Q7032XL oblong. The oblong has got  a better G/T of nearly 1 dB! It is modelled on the basis of EF7032, though only the boomlengths are kept the same, in order to make comparison easier.

Note: YU7EF yagis are probably the best in the world at the moment.

For comparison, the results of the original YU7EF yagi versus my Q7032XL oblong are shown in table 1::

Antenna

Boomlength (mm)

Material

Gain (dBi)

TA (◦K)

G/T (dB)

 

Q7032XL

 

8670

No loss

20,55

18,0

+7,81

Silver

20,51

21,8

+7,13

Aluminum

20,48

23,4

+6,80

 

EF7032-5

 

8670

No loss

19,92

20,0

+6,91

Silver

19,87

23,3

+6,19

Aluminum

19,84

25,2

+5,83

Remarks: Same segmentation density used. Same frequency: 432,200 MHz

Table 1: YU7EF yagi versus Q7032 oblong

 

Super oblong antenna for 432 MHz  - Q7034XL

Now, let us see the 34 element oblong antenna Q7034XL for 432 MHz. Later one more oblong antenna for 432 MHz (shorte, for moderate requeats) will be described. I made this model following the already shownm shorter model Q7032XL, Its elements are made of aluminium rods of 5 mm diameter. Some can decide that silver plated rods can be worth of effort, because the difference is approx 0,3 dB in G/T for silver. The total boom length is 9385 milimetres. The impedance value is exactly 50±j0 Ohms on the center frequency of 432,300 MHz, and the bandwidth for SWR=1,5 is 430,170 to 433,380 MHz. The other parameters are given in the following tables:

 

Performance Data: (No loss condition)

TYPE

ELE

L (mm)

G (dBi)

F/B (dB)

F/Sh (dBi)

F/Sv (dBi)

Hor (◦)

Ver (◦)

Temp (◦K)

G/T (dB)

ΔF * (MHz)

Q7034XL

34

9385

20,81

25,24

20,91

19,95

18,6

18,8

17,5

+8,38

3,25

* ΔF given for SWR=1,5

 

 

Performances: (Losses included)

Element material

G (dBi)

Temp (◦K)

G/T (dB)

Aluminum rods

20,74

22,1

+7,30

Silver plated copper rods

20,77

20,5

+7,66

 

Dimensions:

 

Ref

De

D1

D2

D3

D4

D5

D6

D7

D8

D9

D10

D11

D12

Pos

0

162

224

340

490

690

927

1201

1500

1803

2115

2436

2756

3085

Length

314,0

292,0

284,0

262,0

259,0

254,0

250,0

244,0

239,0

235,0

231,0

229,0

226,0

223,0

 

 

D13

D14

D15

D16

D17

D18

D19

D20

D21

D22

D23

D24

D25

D26

Pos

3405

3735

4060

4393

4686

5041

5358

5685

6011

6321

6649

6937

7198

7493

Length

222,0

222,0

221,0

220,0

219,0

216,0

214,0

212,0

208,0

206,0

204,0

203,0

201,0

199,0

 

 

D27

D28

D29

D30

D31

D32

REMARKS: : - All elements made of Al wire Ǿ5 mm

                       - The height of all rectangles is 50 mm

     - All dimensions given in milimetres

Pos

7823

8119

8463

8771

9076

9385

Length

198,0

197,0

196,0

195,0

195,0

194,0

Table 2: Simulated performance data and dimensions

Diagrams:

Fig 2: 34 element oblong for 70 cm - Horizontal plane (left) and vertical plane (right) (4NEC2 simulation)

Fig 1 – SWR narrow (top) and wideband (bottom) sweep for the 34 ele 70 cm oblong antenna (4NEC2 simulation

 

 

Moderate Oblong Antena Q7023XL for 432 mhz

Now, here is an oblong antenna for “moderate” requests. Its boom is 5970 mm long, what is very suitable, because standard aluminum tubes for boom are supplied in 6 metres length. The system of 4 such antennas will provide around 25,0 dBi gain; more than enough for serious EME, and excellent for normal DX work. The central resonant frequency is 432,3 MHz, which will slightly slide down to 432,1 MHz when mounted in a system. The best stacking distance is 192 cm horizontally, and 189 cm vertically.

Performance Data: (no loss condition)

TYPE

ELE

L (mm)

G (dBi)

F/B (dB)

F/Sh (dBi)

F/Sv (dBi)

Hor (◦)

Ver (◦)

Temp (◦K)

G/T (dB)

ΔF * (MHz)

Q7023XL

23

5970

19,33

29,31

18,62

17,28

21,6

22,2

17,7

+6,86

2,7

* ΔF given for SWR=1,5

 

Performance Data: (losses included)

Element material

G (dBi)

Temp (◦K)

G/T (dB)

Aluminum rods

19,27

21,9

+5,87

Silver plated copper rods

19,29

20,3

+6,21

 

Dimensions:

 

Ref

De

D1

D2

D3

D4

D5

D6

D7

D8

D9

D10

D11

D12

Pos

0

156

218

331

486

685

932

1198

1503

1805

2119

2444

2766

3085

Length

314,0

291,0

285,0

264,0

260,0

254,0

250,0

244,0

240,0

236,0

230,0

228,0

227,0

224,0

 

 

D13

D14

D15

D16

D17

D18

D19

D20

D21

- All elements Al wire Ǿ5 mm

- The height of all rectangles is 48 mm

- All dimensions given in milimetres

Pos

3415

3744

4058

4388

4708

5032

5359

5675

597

Length

223,0

221,0

220,0

218,0

216,0

212,0

210,0

206,0

202,0

Table 3: Q7023XL oblong – Simulated performance data and dimensions

Diagrams:

Fig. 4: 23 element oblong for 70 cm –Horizontal plane (left) and vertical plane (right) (simulation)

Fig.3: SWR sweep for the 23 ele 70 cm oblong antenna

 

Read what Lionel, VE7BQH, writes about the 70cm Oblongs: „This is realy very impressive for several reasons. One, I have never seen a quad type antenna over about 4 elements ever even get close to a yagi. Two, it is the biggest single gain improvement I have seen in many, many years. A 4 bay on 70 cm would be a very reasonable standalone antenna. Please, pass along my „well done“ to YU7XL.

73, Lionel, VE7BQH