Home |
Search |
Today's Posts |
#27
![]() |
|||
|
|||
![]()
On 11/5/2014 8:29 PM, Jeff Liebermann wrote:
Incidentally, I don't believe using a high impedance loop and amp are good ideas. While there are benefits, my experiences from the marine radio biz convinced me that high voltage is an invitation to problems from condensation, salt fog, and PCB leakage. In other words, it works on the bench, but craps out in the field. I'll probably end up with a large high Q loop, and a separate low-Z coupling loop (i.e. a step down xformer). Not sure why you can't discuss this in the right thread of this group. I've posted my reply to your post in the loop antenna thread. First, I'm not sure what you are talking about connecting high impedance antennas to condensation and salt fog. If you are transmitting, then maybe you could get such high voltages as to attract microscopic objects, but this is a receiver design. Also, the antenna is not high impedance, just the input to the receiver. The transformer I am looking at is a high turns ratio current sensor. It spans the right frequency range and is a nice compact package easy to mount on a PCB. My main concern is lowering the Q because of the loading from the receiver input, especially with the change in impedance as reflected through the transformer. I think when I simulated it, I found the max signal strength came with a 25 or 33:1 turns ratio because with higher turns ratios the Q was spoiled enough to bring the voltage down at the receiver input. This simulation didn't include the effect of the radiation resistance, so I will need to add that in. I expect this will lower the Q as a starting point which means the affect from the receiver input loading will not be as significant, possibly making a higher turns ratio in the transformer more useful. -- Rick |
Thread Tools | Search this Thread |
Display Modes | |
|
|