Home |
Search |
Today's Posts |
#10
![]() |
|||
|
|||
![]()
Owen Duffy wrote in
: .... If I take a half wave folded dipole immersed in some environment where the ambient noise temperature is T, and attach a load directly to the feedpoint, the load power will be maximum when it is about 300 ohms rather than about 75 ohms, and the noise power density due to ambient noise would be K*T*300 W/Hz rather than K*T*75 W/Hz. If Rr is the (virtual) resistance due to coupling of the antenna with distant space, then surely this example suggests that Rr is 300 rather than 75 ohms. (If I performed the same experiment with a plain half wave dipole, the load power will be maximum when it is about 75 ohms, and the noise power density due to ambient noise would be K*T*75 W/Hz.) Sorry, that is plainly wrong. Clarity struck whilst having breakfast, the received power of a matched system should be independent of R. Noise power density is simply K*T W/Hz. There is no R term. The text should read... If I take a half wave folded dipole immersed in some environment where the ambient noise temperature is T, and attach a load directly to the feedpoint, the load power (due to ambient noise) will be maximum when it is about 300 ohms rather than about 75 ohms. If Rr is the (virtual) resistance due to coupling of the antenna with distant space, then surely this example suggests that Rr is 300 rather than 75 ohms. My apologies. Owen |
Thread Tools | Search this Thread |
Display Modes | |
|
|
![]() |
||||
Thread | Forum | |||
Radiation Resistance | Antenna | |||
Radiation Resistance & Efficiency | Antenna | |||
Measuring radiation resistance | Homebrew | |||
Measuring radiation resistance | Antenna | |||
Measuring radiation resistance | Homebrew |