I really love learning things, and recently I've finally been removing a long-standing thorn in my side - the fact that I don't really understand radio frequency electronics and the propagation of radio waves.

I've tried to fix this a few times in the past, but the resources I'd read never seemed to quite explain the whole picture - and I couldn't see how to piece the things they explained together into one coherent understanding of the electromagnetic world; they were clearly only shedding light on little corners of a totality that still remained mysterious to me.

Well, there are still gaps in my understanding... but I've made some progress, and in the hope that I can help others struggling with the same confusions as I was, I'd like to share my way of understanding it all.

One thing that bothered me was that explanations of transmission-line behaviour seemed to flip between talking about instantaneous voltages and currents at some point in the line, sampling the analogue signal traveling down the line - or talking about an RMS average voltage or current, and thereby causing me to struggle to make sense of what they were saying. But I think I now get transmission lines to some extent (although I'm still hazy on wave guides, because I've not gotten around to looking into them yet). And I was never quite sure what the impedance of a whole transmission line really meant, regardless of its length. If I had a transmission line and put a resistor over the end of it, and hooked it up to a battery and an ammeter, I knew that the current flowing would depend on the total resistance of the line and the resistor at the end - which would depend on the length of the line, as its resistance would be in ohms per meter. So what the heck was this impedance thing about? How did impedance mismatches cause reflections?

So, here's how I think about transmission lines now. The "DC model" of hooking a battery up to one end of a line and reading the current that flows into it is, of course, perfectly true - we can set the circuit up and test it; the reason it doesn't contradict with this weird parallel world of impedances is that the DC model is a steady state model of the system. When you first connect that battery to the line, current is going to start flowing into it, crawling along at a sizeable fraction of the speed of light; but until that current has reached the end, flowed through the terminating resistor, and flowed all the way back, it can't possibly have communicated any information about the total resistance of the line and its terminating resistor... So how much current initially flows from the battery, and why? Of course, the line can be thought of as two series of tiny inductors (with resistors in series, if we assume the inductors are perfect) with tiny capacitors connecting the two conductors, due to the inherent inductance of the wire and the inherent capacitance of the gap between them; you can imagine that the current from the battery has to charge the capacitors through the inductors for the voltage/current surge to propagate down the line. But what made "impedance" really click for me was going back to the basics of Ohm's Law and seeing it as a ratio of voltage to current. At any point along that transmission line, a certain instantaneous current will be flowing - and there will be a certain instantaneous voltage between the two conductors at that point; and the voltage divided by the current is the impedance.

So, if a 12 volt voltage source is connected suddenly to a 50 ohm impedance cable, an instantaneous current of 0.24 amps (12̣̣̣̣÷50) will flow. Now, as Kirchoff's current law tells us, the currents flowing into a node must sum to zero; so with the imaginary node at any point on the transmission line connecting two halves of it, the input current must equal the output current (although some current may be lost to resistive heating or leakage, that's not relevant in this case). So what happens when there's a change in impedance at some point in the transmission line? The current must remain the same, but the impedance changes - so the voltage must change, to make Ohm's Law still hold. If my 50 ohm cable is connected to a 75 ohm cable, that 0.24 amps flows into it and changes into a voltage of 18 volts (0.24×75). Which is why high impedance transmission lines are less lossy; a transmitter putting a watt of power down such a line (with proper impedance matching) will push out a higher voltage with less current that one putting a watt of power into a low impedance line - and resistive losses in the cable are worse for higher currents.

How about the reflections when impedance changes? I'm still a little hazy on this, but I think it's something along the lines of this: imagine a point just where the impedance changes in our example of moving from a 50 ohm cable to a 75 ohm one. A current is flowing into that point, but the voltage is higher after that point than before - which is going to create a current traveling back the other way. Where I'm hazy on is how this happens at junctions where the impedance falls (is it to do with the fact that the current flows alternately backwards and forwards, so the junction is traversed by current in both directions anyway, and the phases where the current travels from low to high impedance are what create the reflections? If so, isn't that a kind of rectifying action, that will create harmonics and intermodulation? But what is the "direction" of a signal traveling along a line, anyway? If we froze the signal in time, we'd just see a sine wave of voltage and a sine wave of current along the transmission line - if we restart time, how does it "know" what direction to propagate in? Something to do with the relative phase of the voltage and current waves?) So, yeah, I've a little more to learn there.

But this model of impedance does explain a lot. I wondered why the angles of the radials of a ground-plane monopole antenna affected impedance, but now it makes sense - the end of the transmission line basically spreads out to become a dipole, or a monopole and its ground plane; the electrical field of the traveling signal has to cross a larger region of space, so it makes sense that the voltage required to do so might vary depending on the amount of space crossed. All the mysterious constants, like the fact that a dipole trimmed to 0.48 times the wavelength has an impedance of 70 ohms are really down to the electromagnetic stretchiness of space: the impedance is the voltage required to push one amp along a transmission line (a dipole antenna just being an oddly-shaped transmission line, handing the signal over to the even weirder transmission line that is free space itself), and that is a function of the permittivity and permeability of that space.

This model also explains how impedance matching transformers work. A `1:2` turn ratio transformer will transform `X` volts and `Y` amps on the "left" into `2*X` volts and `Y/2` amps on the "right"; as the impedance is `V/I`, that means it converts `R` ohms on the left into `R*4` ohms on the right, simply through changing the voltages and currents. A `1:N` turn ratio transformer makes a `1:N^2` change in impedance.

Antennas with multiple elements are confusing, but I'm not sure anybody really understands them - as far as I can tell, the design process is almost always to mock it up in a finite-element computer simulation or build a prototype and tweak the design until the desired parameters are obtained experimentally; the mutual interactions between the elements (not to mention ground, support structures, and the transmission line feeding the antenna) are just too complicated to analyse.

I really don't get why there's a near field and a far field (or that funny one in between that, I think, is just a mixture of the two). Does the antenna both far and near fields at once, and the near field is stronger but doesn't spread out far, so the far field is negligible when close to the antenna? Or does the antenna create a near fields, which "decays into" the far field as it spreads out? Nothing I've found seems to explain.

I'm not very clear on why a balanced transmission line that's shorted at one end and open at the other end has varying impedance along its length, and can be used for impedance matching, but it doesn't create reflections from the ends.

But, I can understand how to run a cable to a dipole or monopole antenna, manage the impedance transitions, and make it radiate efficiently. That's progress!

## National Poetry Day UK 2018(by sarah)

Today is National Poetry Day - so I shall be spending the day on various social media sites and blogs sharing all the stuff from the archives - namely the writing exercises and write ups on interesting writers.

Where you can find me:

Where you can read my poetry:

Where you can find writing exercises:

Poetry is a pretty big thing for me - I never thought it was going to be, I kind of thought the whole thing wasn't for me. I like what I like and that has little to do with the academic studies of the poetic form. I like poems in different styles from different times and cultures and so on. I find people being elitist and pretentious about it all... annoying and ignorant.

That is one of the reasons that I have backed the local poetry festivals the way I have - they offered spaces for voices that were rarely heard and the internet also helped.

This month I am lucky in that I am hosting events at the Gloucester Poetry Society and I am taking part in a Slam over in Cheltenham (still not sure about the competition part of the slam culture but I like the events over all and the people I see there - they are fun and diverse).

I've been going through my poetry and trying to decide how best to move forward with it all - I have singularly failed to actually submit work once again but thanks to people chasing me I am in a couple of pamphlets which are to be release later this month I believe.

I have several collections that were stalled with head injury and what not which I should really revisit and sort out and I have a few more zines that are pretty much ready to go!

But I also want to produce more books with other people - I liked WigglyPet Press's involvement with last years poetry anthology but it has now been out for a year so I feel that it is time for me to publish something new!

At the moment I am thinking of something themed around space, the cosmos, exploration and the unknown but I have not decided on the format yet!

## October Events and Stuff!(by sarah)

September was frantic and wonderful - the Gloucester History Festival was amazing and has started me down the paths of several new and exciting things for the future! And I have a lot of events photos and sketchtember pictures to share with you all.

But for now it is October the 1st 2018 and this new month hold even more in it that September did! Namely The Cheltenham Literature Festival, Gloucester Poetry Festival and Frightmare Halloween Festival! I am involved in parts of all three of these over lapping festivals - wish me luck!

And then as my fun/de-stress there is Inktober - a drawing challenge that was one of the major factors in me actually producing the art work for Love: A Stranger Dream.

And then there is GothNoWriMo which is a writing challenge and shall see me writing yet more of the Punk Universe (which I will be releasing parts of properly next year!).

So here are the current confirmed dates!

Sat 6th Oct 7 pm Frightmare Preview Night at Overfarm Gloucester - ticketed event (prices vary)

Tues 9th Oct 7pm Operation Beehive in Swindon part of the Gloucester Poetry Festival and a Gloucester take over of the regular Ooh Beehive Night

Thurs 11th Oct 7:30 pm - Hammer and Tongues All Star Poetry Slam in Cheltenham, part of the Cheltenham Literary Festival at The Bottle of Sauce tickets are free and can be booked here

Fri 12th - Sat 13th Oct Young Gods showcase at Elmbridge Primary School 6:30 pm Jean and Mary's Drama group

Fri 12th - Sat 13th Oct Frightmare Scare Attraction Over Farm Gloucester from 7 pm

Sun 14th Oct 2-4 pm Poetry hosted by Sarah at the Gloucester Waterstones part of the Gloucester Poetry Festival - free event including goody bags as part of Books Are My Bag

Tues 16th Oct 2-4 Book Wyrms at Gloucester Library a poetry event with guest poets hosted by Sarah - part of the Gloucester Poetry Society and free event

Fri 19th - Sat 21st Oct Frightmare

Sun 21st 2-4 pm Poetry at Gloucester Waterstones as part of the Gloucester Poetry Society hosted by Sarah

Wed 24th Oct 2-4pm Book Wyrms free poetry event at Gloucester Library part of the Gloucester Poetry Festival hosted by Sarah

Wed 24th - Sat 31st Oct Frightmare Halloween Festival at OverFarm Gloucester

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