Bernie G said:
I don't have access to a sample cable right now, but all the 3 GHz low loss (low power) 75 ohm cable I've seen has been large diameter
all cables will operate to and well beyond 3GHz ( not sure why you are fixated with the 3GHz figure?
the only difference is that some cables will have greater loss at 1 to 5 GHz. So the design of the cable determines the attenuation (loss) the cable has
per 100 ft (30 metres). The loss is measured in dB. The spec's for a given cable will show a table of the losses for a range of frequencies / 30 metres
lets choose my fav cable for the 144MHz to 1300MHz (1.3GHz) LDF4-50A
this is 1/2 inch diameter ( maybe a tad more)
solid copper or sometimes copper clad aluminium, centre conductor, foam dielectric and a copper outer conductor
Freq -- dB/100m -- dB/100ft
150 ----- 2.673 ------ 0.815
450 ----- 4.749 ------ 1.447
1000 --- 7.284 ------- 2.22
1500 --- 9.093 ------ 2.771 you can see how the attenuation increases rapidly as the frequency rises.
every 3 dB of loss you halve your power ( that applies to transmit or receive signals)
I have also often used its big brother on commercial installations, LDF 5-50, 7/8 inch diameter ( close enough to 1 inch dia)
the lowest attenuation is achieved by having an all air dielectric, but this is impossible in a coaxial cable as there needs to be something to support the inner conductor in the centre of the cable. One way around this is to use a spiral of Teflon. This keeps the 2 conductors uniformly separated but still achieves a dielectric that is >80% air. See the centre coax in the pic below
for frequencies 5GHz and greater and for lengths more than a metre or so, waveguide is used. This has very low loss compared to any coax cable
Bernie G said:
Isn't it much easier to make a high frequency 50 ohm cable than a 75 ohm cable?
no, the manufacturing process is just the same
do you understand what determines the impedance of a coaxial transmission line ? ...
Coax impedance determination
The impedance of the RF coax cable is chiefly governed by the diameters of the inner and outer conductors. On top of this the dielectric constant of the material between the conductors of the RF coax cable has a bearing. The relationship needed to calculate the impedance is given simply by the formula:
Where:
Zo = Characteristic impedance in Ω
εr = Relative permeability of the dielectric
D = Inner diameter of the outer conductor
d = Diameter of the inner conductor
Note: The units of the inner and outer diameters can be anything provided they are the same, because the equation uses a ratio.
that should be εr on the bottom line ... not going to name the page it came from as I don't particularly like some of their other garbage
Wiki gives a derivation of this formula ...
Derived electrical parameters[edit]
- Characteristic impedance in ohms (Ω). Neglecting resistance per unit length for most coaxial cables, the characteristic impedance is determined from the capacitance per unit length ([PLAIN]https://upload.wikimedia.org/math/0/d/6/0d61f8370cad1d412f80b84d143e1257.png) and the inductance per unit length ([PLAIN]https://upload.wikimedia.org/math/d/2/0/d20caec3b48a1eef164cb4ca81ba2587.png). The simplified expression is ([PLAIN]https://upload.wikimedia.org/math/1/7/d/17d9d3ce2d1beb4487f2801b1e1b5046.png). Those parameters are determined from the ratio of the inner (d) and outer (D) diameters and the dielectric constant ([PLAIN]https://upload.wikimedia.org/math/c/5/0/c50b9e82e318d4c163e4b1b060f7daf5.png). The characteristic impedance is given by[7]
[PLAIN]https://upload.wikimedia.org/math/4/2/f/42f82056c01eef1ea64f5ce256b6a2c2.png[/U]
Assuming the dielectric properties of the material inside the cable do not vary appreciably over the operating range of the cable, this impedance is frequency independent above about five times the https://en.wikipedia.org/w/index.php?title=Shield_cutoff_frequency&action=edit&redlink=1 . For typical coaxial cables, the shield cutoff frequency is 600 (RG-6A) to 2,000 MHz (RG-58C).[8]
cheers
Dave