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#1
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I just read one of Cebik's lessons on common mode currents and am
looking at a diagram he posts. The diagram shows I1 as the RF current on the center conductor, I2 as RF current on the inside of the braid and I3 as commond mode current on the outside of the braid. Since I have not seen my query posted anywhere, I am a bit reluctant to ask because the answer is probably very obvious. I hope I don't get chided that I an an Extra, asking a simple, fundamental question. I have studied hard most every day but without the benefit of an electrical/electronics/engineering background, it is going to take the rest of my lifetime to acquire all that I am curious about. This particular bit of confusion comes from knowing how I attach a PL-259 to the braid of coax. The OUTSIDE surface of the braid fits flush to the PL-259 shell, not the INSIDE surface of the braid where I2 is portrayed to be. Subsequently, the shell of the PL-259 gets coupled to one side of the antenna. I understand the potential for I3. And, I reasoned that the RF current could be initially placed on the inside surface of the braid at the transmitter end of the coax run. But then, back at the antenna end of the coax and PL-259 connector, I only see a dead end for the I2 current. I added a Balun component to my thinking about the issue, but the confusion did not go away. I just cannot understand how I2 gets coupled to the dipole antenna element since the coax gets coupled at the PL-259 via the outside surface of the braid. |
#2
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k1drw wrote:
I just cannot understand how I2 gets coupled to the dipole antenna element since the coax gets coupled at the PL-259 via the outside surface of the braid. It is the physics of the coaxial cable that causes I1 and I2 to be equal in magnitude and opposite in phase. The internal coax fields force that condition. At the antenna, I1 has only one choice of paths - into the antenna (if matched). But I2 has two choices - into the antenna (if matched) or down the outside of the coax. It will divide at that point according to Ohm's law most of it taking the path of least impedance. A choke increases the impedance down the outside of the coax making the antenna impedance more attractive to the current. -- 73, Cecil http://www.w5dxp.com |
#3
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Cecil:
Thank you for the quick reply and clear explanation. I now understand the coupling of rf current from inside the braid to potentially, depending on impedance, both paths. Sincere thanks..! |
#4
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You might get a little more insight from
http://eznec.com/Amateur/Articles/Baluns.pdf. Roy Lewallen, W7EL |
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