Speaking of tubes: Introducing the Grid Dip Meter

+Jonah Miller is currently working on a multi-part series of articles on how computers work. In one of the installmetns he mentioned the good old triode vacuum tube with a cathode, plate, and grid. That brings up the subject of today's post, the grid dip meter, (GDM). If you wandered over here from the ham radio practice tests[1], and you want the shortest answer possible, then click here, or scroll down the page. If you want more information, read on:

The grid Dip meter schematic is shown in picture 1.

The main purpose of the circuit, at least for amateur radio operators, is to determine the resonant frequency of some other circuit or device, (like an antenna). Let's say you've built you're latest radio and you'd like to get all the power you can from the driving finals, into the antenna. To do that, you'd like to make sure that the antenna resonates at the same frequency you'd like to send and receive at. If the antenna resonates at a little bit lower frequency, you can always trim it's length, or if it oscillates at a little bit higher frequency, you can always make a longer one. To find out which I need to do, I'll use my grid dip meter to determine the antenna's resonant frequency.

The basic grid dip meter's circuit consists of a Colpitts oscillator with the inductor, L1, of the LC feedback loop exposed and protruding from the device, (see picture 2), it's the coil on the far left edge of the picture.

To determine my antenna's resonant frequency, I'll attach a small coil to the middle of it, (I tend to only use dipoles because I'm lazy). Next, I'll place the exposed coil of the grid dip meter near the coil attached to my antenna. Then, I'll tune the oscillator's operating frequency until I see the reading on the meter on the front face of the apparatus, which is denoted by G in the schematic, dip, (hence the name).

So,why does the current being supplied to the grid of the Colpitt's oscillator dip? At the resonant frequency of the device being measured, the magnetic field from the inductor begins to drive the coil on the device under test. In this case, the antenna radiates that energy away. The current that was driving the grid is now reduced in an amount related to the amount of energy that went into the device under test, (the antenna). Pretty cool!

The Answer to the Ham Radio License Exam Question
You want the two coils to be as loosely coupled as possible. If they are tightly coupled, (located very close to one another), then the inductance in the coil attached to the device under test will effect the resonant frequency of the GDM. The end result will be that the resonant frequency won't be the actual resonant frequency of the device under test, it will be an odd munge of the device and the GDM circuit. On the flip side, you don't want to couple too loosely either, or the grid current simply won't dip.

A Year and a Month Ago

Radiating Superconductors, Arduinos, and Data Acquisition
http://copaseticflow.blogspot.com/2012/06/radiating-superconductors-arduinos-and.html

LabBook 2014_05_26 Superconductor Quenching Magnet Chilling Supply and Leak Detector Testing
http://copaseticflow.blogspot.com/2014/05/labbook-20140526-superconductor.html

References:

1. http://copaseticflows.appspot.com/hamtest

2. Jonah Miller's Post on Logic Circuits
http://www.thephysicsmill.com/2014/06/22/boolean-cirucit-logic/

Cool Math Tricks: Deriving the Divergence, (Del or Nabla) into New (Cylindrical) Coordinate Systems

Now available as a Kindle ebook for 99 cents ! Get a spiffy ebook, and fund more physics The following is a pretty lengthy procedure, but converting the divergence, (nabla, del) operator between coordinate systems comes up pretty often. While there are tables for converting between common coordinate systems , there seem to be fewer explanations of the procedure for deriving the conversion, so here goes! What do we actually want? To convert the Cartesian nabla to the nabla for another coordinate system, say… cylindrical coordinates. What we’ll need: 1. The Cartesian Nabla: 2. A set of equations relating the Cartesian coordinates to cylindrical coordinates: 3. A set of equations relating the Cartesian basis vectors to the basis vectors of the new coordinate system: How to do it: Use the chain rule for differentiation to convert the derivatives with respect to the Cartesian variables to derivatives with respect to the cylindrical variables. The chain ...

The Alcubierre Warp Drive Tophat Function and Open Science with Sage

I transferred yesterday's Mathematica file with the Alcubierre warp drive[2] line element and space curvature calculations to the +Sage Mathematical Software System today, (the files been added to the public repository [3]). If you haven't used Sage before, it's a Python based software package that's similar in functionality to Mathematica. Oh, and it' free. I also worked a little more on understanding the theory, but frankly, I made far more progress with the software than the theory. What follows will be a little more of the Alcubierre theory, plus, a cool Sage interactive demo of one of the Alcubierre functions[1], as well as a bit about my first experience with using Sage. Theory The theory is fun, but it's moving slowly. Here's the chalk board from this morning's discussion Alcubierre setup the derivation using something called the 3+1 formalism which means we consider space to be flat, (in this case), slices that are labelled ...

The Valentine's Day Magnetic Monopole

There's an assymetry to the form of the two Maxwell's equations shown in picture 1. While the divergence of the electric field is proportional to the electric charge density at a given point, the divergence of the magnetic field is equal to zero. This is typically explained in the following way. While we know that electrons, the fundamental electric charge carriers exist, evidence seems to indicate that magnetic monopoles, the particles that would carry magnetic 'charge', either don't exist, or, the energies required to create them are so high that they are exceedingly rare. That doesn't stop us from looking for them though! Keeping with the theme of Fairbank[1] and his academic progeny over the semester break, today's post is about the discovery of a magnetic monopole candidate event by one of the Fairbank's graduate students, Blas Cabrera[2]. Cabrera was utilizing a loop type of magnetic monopole detector. Its operation is in...

Copasetic Flow

Search This Blog