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Reg
Your patience is that of a saint. H. "Reg Edwards" wrote in message ... Cec sez, My solution is to get Reg to write a new program. :-) ======================================= My patience is wearing thin. Nevertheless, once more into the breach. There's no need to write a new program. There's not even any need for an old one. Knowledge of the current distribution along a loading coil has no practical use except to assist with drawing pictures of it in books and magazines. FOR PRESENT PURPOSES THE LENGTH AND IMPEDANCE OF THE ANTENNA BELOW THE COIL IS NOT RELEVANT. IT CAN BE CONSIDERED TO BE PART OF THE GENERATOR. LET THE ANGULAR LENGTH OF THE COIL = THETA DEGREES. OTHERWISE KNOWN AS THE PHASE SHIFT. THIS IS A FIXED, IMMUTABLE QUANTITY SET BY THE PROPAGATION VELOCITY = 1 / SQRT( L * C ). THE MAGNITUDE OF THE CURRENT DISTRIBUTION ALONG THE COIL IS ALWAYS THE SAME COSINE CURVE BUT WHICH IS TRUNCATED (SLICED OFF) AT VARYING ANGULAR DEGREES AT EITHER OR BOTH ENDS. THE ANGLE AT WHICH THE TOP END IS TRUNCATED DEPENDS ON THE INPUT IMPEDANCE OF THE ANTENNA ABOVE IT. IT IS ALSO RELATED TO Zo OF THE COIL WHICH IS THE USUAL SQRT( L / C ). THE ANGLE AT WHICH THE BOTTOM END IS TRUNCATED IS ALWAYS THE TOP ANGLE MINUS THETA. IT CANNOT BE ANYTHING ELSE. THUS, WHEN THE TOP END IS OPEN CIRCUIT AND THETA = 90 DEGREES WE HAVE A COMPLETE 1/4-CYCLE OF A COSINE CURVE - A 1/4-WAVE RESONANT HELICAL ANTENNA. The foregoing applies to both short, fat coils and long, thin coils, close-wound or stretched-out. Coil resistance is the uniformly-distributed radiation resistance plus conductor resistance. For useful calculations such as Q, bandwidth, efficiency, etc., you can forget all about bewildering reflections, standing waves, forward and reflected power and use the well-known classical transmission line formulae, the everyday tools of all good engineers. The final wanted characteristic, the radiation pattern, can be found with number-crunching EZNEC-type computer programs which work in an entirely different manner. ---- Reg, G4FGQ |
#2
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H. Adam Stevens, NQ5H wrote:
Reg Your patience is that of a saint. H. "Reg Edwards" wrote in message ... Cec sez, My solution is to get Reg to write a new program. :-) ======================================= My patience is wearing thin. Nevertheless, once more into the breach. There's no need to write a new program. There's not even any need for an old one. Knowledge of the current distribution along a loading coil has no practical use except to assist with drawing pictures of it in books and magazines. FOR PRESENT PURPOSES THE LENGTH AND IMPEDANCE OF THE ANTENNA BELOW THE COIL IS NOT RELEVANT. IT CAN BE CONSIDERED TO BE PART OF THE GENERATOR. LET THE ANGULAR LENGTH OF THE COIL = THETA DEGREES. OTHERWISE KNOWN AS THE PHASE SHIFT. THIS IS A FIXED, IMMUTABLE QUANTITY SET BY THE PROPAGATION VELOCITY = 1 / SQRT( L * C ). THE MAGNITUDE OF THE CURRENT DISTRIBUTION ALONG THE COIL IS ALWAYS THE SAME COSINE CURVE BUT WHICH IS TRUNCATED (SLICED OFF) AT VARYING ANGULAR DEGREES AT EITHER OR BOTH ENDS. THE ANGLE AT WHICH THE TOP END IS TRUNCATED DEPENDS ON THE INPUT IMPEDANCE OF THE ANTENNA ABOVE IT. IT IS ALSO RELATED TO Zo OF THE COIL WHICH IS THE USUAL SQRT( L / C ). THE ANGLE AT WHICH THE BOTTOM END IS TRUNCATED IS ALWAYS THE TOP ANGLE MINUS THETA. IT CANNOT BE ANYTHING ELSE. THUS, WHEN THE TOP END IS OPEN CIRCUIT AND THETA = 90 DEGREES WE HAVE A COMPLETE 1/4-CYCLE OF A COSINE CURVE - A 1/4-WAVE RESONANT HELICAL ANTENNA. The foregoing applies to both short, fat coils and long, thin coils, close-wound or stretched-out. Coil resistance is the uniformly-distributed radiation resistance plus conductor resistance. For useful calculations such as Q, bandwidth, efficiency, etc., you can forget all about bewildering reflections, standing waves, forward and reflected power and use the well-known classical transmission line formulae, the everyday tools of all good engineers. The final wanted characteristic, the radiation pattern, can be found with number-crunching EZNEC-type computer programs which work in an entirely different manner. ---- Reg, G4FGQ If patience were money, Reg would be wearing a barrel. 73, Tom Donaly, KA6RUH |
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