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On Nov 21, 5:18*pm, Wimpie wrote:
On 21 nov, 16:44, Art Unwin wrote: On Nov 21, 5:38*am, Wimpie wrote: On 21 nov, 04:47, Steve wrote: I've seen several programs that will help you calculate the precise dimensions of a single-turn loop, given the composition of the radiating element, its thickness, and so on. However, none of these programs are written to cover the case of a two or more-turn loop. Does anyone know of a program that will offer guidance in the construction of a two or more-turn loop? Thanks, Steve Hello Steve, You probably did some loop calculations and found that in a transmit case the voltage across the tuning capacitor is very high (and bandwidth is limited). Also for small loops, most input power is lost as heat due to copper resistance. When you make a two turn loop, the radiation resistance will increase with factor 4. So with half the current through the loop, the radiated power is same (as for a single turn loop). *When the 2 turns of the loop are relative close together, the inductance increases with factor 4, hence the reactance. The current has been halved, but because of the reactance, the voltage across the tuning capacitance will be 2 times the value for the single turn loop with higher probability on corona effects. *An advantage can be an almost 4 times smaller tuning capacitor. One may expect that the loss resistance due to heat of a two-turn inductor will be twice as high (w.r.t. single turn case). This is not true; the loss resistance will be more then twice as high because of proximity effect. The current will not equally distribute along the circumference of the tube/wire. *So the efficiency of the loop will be less then twice as high (w.r.t. single turn case). When the turns are far apart (with respect to wire/tube diameter), inductance will not be 4 times higher and proximity effect will be less. You will get better performance than the single turn loop made of same diameter tube/wire. The result will be the same as when you place the two turns in parallel. Inductance will decrease somewhat (hence lower voltage across capacitor), AC resistance also, hence radiation efficiency). There is an "however". When you make a single turn loop from flat strip that has the same width as the length of your two-turn loop, you will notice: *1. reduced AC resistance (because of the significantly larger circumference of the flat strip with respect to a thin round tube, 2. inductance will decrease (H field lines have to take a longer path around the wide strip), 3. radiation resistance will not change with respect to a single turn loop from wire/tube. This results in higher efficiency and increased bandwidth. * The overall result will be better then for your two-turn loop. I think that is the reason why most programs are for single turn loops. So for the transmit case, given fixed diameter of your loop, the larger the copper surface (=length*circumference), the better the efficiency. *Best thing to enhance conductor surface is to use very wide flat strip (high wind load), or multiple wires (with some spacing in between) in parallel (limited wind load). Off course for the receive-only case, a multi turn loop can be helpful as you can use a smaller tuning capacitor. Best regards, Wim PA3DJSwww.tetech.nl In case of PM, don't forget to remove abc. Seems to me you are recommending the "?slinky" ! Is that correct? Art Sorry Art, I am not talking about a slinky. I am just talking about a multi turn (2 turns) loop where overall wire length is 0.25 lambda so you can assume that current in wire is constant along the length. It must be tuned by external capacitance. Regarding the strip. When you take a 3.14m long 20cm wide thin copper strip and make a loop of it (1m diameter), it will have a better efficiency then when you take 6.28m *copper tubing with Dtube=2cm and make a two-turn loop (Dloop=1m, turns 18 cm apart). In the strip case, the current has more circumference to flow (40cm) instead of 6.28cm for the copper tubing. *AC resistance of copper tubing will be about 10 times higher. Off course, current in two-turn loop will be half (for same radiated power), but still heat losses will be 10*0.5^2=2.5 times higher (for the two-turn loop). When both loops have good efficiency (so radiation resistance dominates), the strip loop will have better bandwidth as flux path is longer and therefore results in less inductance. I hope this clarifies my posting. Best regards, Wim PA3DJS Please remove abc in case of PM. I think I am missing something Wim. A slinky has a strip winding that is edge wound which provides the largest disparity between the inside radius and the outside radius. On one of the top transmitters the inductance winding is such that the inner radius is close to the outside radius. Naturally the different pitch of the windings is very different as is the inter coil capacitance. As Roy stated charges accumulate on sharp edges which I see as correct but I cannot see how that alteres the diference all that much as the same clearance is required So in the final analysis for less inductance which form is which., the longer inductance or the shorter inductance on the assumption that the number of turns are similara nd I can acceptt your word for it? I referred to a slinky purely to emphasize the importance of reverse windings so that lumped loadings applied are cancelled. Actually the modern slinky is not contra wound for some reason but I assume that is for the novelty movement reasons for children and not because of radiation reasons. The slinky patent is now defunct if that matters and iI am assuming that the fed would be centre fed. Thank you so much for responding Best regards Art |
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