Tag Archive | "inductance"

Kit review – High Accuracy LC Meter

Hello readers

Time for another kit review. Lately one of my goals has been to make life easier and in doing so having some decent test equipment. One challenge of meeting that goal is (naturally) keeping the cost of things down to a reasonable level. Unfortunately my eyesight is not the best so I cannot read small capacitor markings – which makes a capacitance meter necessary. Although I have that function within my multimeter, it is often required to read resistors in the same work session.

Thus the reason for this kit review – the High Precision LC Meter kit. The details were originally published in the May 2008 issue of Australia’s Silicon Chip magazine. The meter specifications are:

  • Capacitance – 0.1pF to over 800 nF with four-digit resolution;
  • Inductance – 10 nH to over 70 mH with four-digit resolution;
  • Accuracy of better than +/- 1% of the reading;
  • Automatic range selection, however only non-polarised capacitors can be measured.

The power drain is quite low,  between 8 (measurement) and 17 milliamps (calibration). Using a fresh 9V alkaline battery you should realise around fifty to sixty hours of continuous use. At this point some of you may be wondering if it is cheaper to purchase an LC meter or make your own. A quick search found the BK Precision 875B LCR meter with the same C range and a worse L range for over twice the price of the kit. Although we don’t have resistance measurement in our kit, if you are building this you already have a multimeter. So not bad value at all. And you can say you built it 🙂

Speaking of building, assembly time was just under two hours, and the kit itself is very well produced. The packaging was the typical retail bag:

retailkitss

The first thing that grabs your attention is the housing. It is a genuine, made in the US Hammond enclosure – and has all the required holes and LCD area punched out, so you don’t need to do any drilling at all:

hammondcasess

The enclosure has nice non-slip rubberised edging (the grey area) and also allows for a 9V battery to be housed securely. The team at Altronics have done a great job in redesigning the kit for this enclosure, much more attractive than the magazine version. The PCB is solder-masked and silk-screened to fine standard:

pcbss2

There are two small boards to cut and file off from the main PCB. We will examine them later in the article. All required parts for completion were included, and it is good to see 1% resistors and an IC socket for the microcontroller:

partsss1

At first I was a little disappointed to not have a backlit LCD module, however considering the meter is to be battery operated (however there is a DC socket for a plugpack) and you wouldn’t really be using this in the dark, a backlight wouldn’t be necessary. Construction was easy enough, the layout on the PCB is well labelled, and plenty of space between pins. Lately I have started using a lead-former, and can highly recommend the use of one:

leadformerss

Assembly was quite simple, just start with the lower profile components:

assemble1ss

 

… then mount the LCD and the larger components:

assemble2ss

… the switches and others – and we’re done:

finishedsolderingss

The only problem at this point was the PCB holes for the selector switch, one hole was around 1mm from where it needed to be. Instead of drilling out the hole, it was easier to just bend up the legs of the switch and keep going:

switchlegsss

At this stage one has to cut out two supports from the enclosure, which can be done easily. Then insert the PCB and solder to the sockets and power (9V battery snap). Initial testing was successful (after adjusting the LCD contrast…

inittestss

If you look at the area of PCB between the battery and the left-hand screw there are eight pins – these are four pairs of inputs used to help calibrate and check operation of the meter. For example, by placing a jumper over a pair you can display the oscillator frequency at various stages:

calibrationss

Furthermore, those links can also be used to fine-tune the meter. For example one can increase or decrease the scaling factor and the settings are then stored in the EEPROM within the microcontroller. However my example seemed ok from the start, so it was time to seal up the enclosure and get testing. Starting with a ceramic capacitor, the lowest value in stock:

3p9pfss

Spot-on. That was a good start, however trying to bend the leads to match the binding posts was somewhat inconvenient, so I cut up some leads and fitted crocodile clips on the end. The meter’s zero button allows you to reset the measurement back to zero after attaching the leads, so stray capacitance can be taken into account.

Next, time to check the measurement with something more accurate, a 1% tolerance silvered-mica 100 picofarad capacitor:

99pfss

Again, the meter came through right on specification. My apologies to those looking for inductor tests – I don’t have any in stock to try out. If you are really curious I could be persuaded to order some in, however as the capacitance measurement has been successful I am confident the inductance measurement would also fall within the meter’s specifications.

As shown earlier, there were two smaller PCBs included:

pcbadaptorsss

The top PCB is a shorting bar used to help zero the inductance reading, and the lower PCB is used to help measure smaller capacitors and also SMD units. A nice finishing touch that adds value to the meter. The only optional extra to consider would be a set of short leads with clips or probes to make measurement physically easier.

When reading this kit review it may appear to be somewhat positive and not critical at all. However it really is a  good instrument, considering the accuracy, price, and enjoyment from doing it yourself. It was interesting, easy to build, and will be very useful now and in the future. So if you are in the market for an LC meter, and don’t mind some work – you should add this kit to your checklist for consideration. It is available from our store – Tronixlabs.com

 

visit tronixlabs.com

… which along with being Australia’s #1 Adafruit distributor, also offers a growing range and Australia’s best value for supported hobbyist electronics from DFRobot, Freetronics, Seeedstudio and much much more.

As always, have fun and keep checking into tronixstuff.com. Why not follow things on twitterGoogle+, subscribe  for email updates or RSS using the links on the right-hand column, or join our forum – dedicated to the projects and related items on this website.

Posted in K2533, kit review, LC meter, test equipment, tronixlabsComments (18)

Introduction to the Inductor

Hello everyone!

Today we are going to explore the use of the Inductor. This is a continuation from the series of articles on alternating current. An inductor is a component that can resist changes in AC current, and store energy in a magnetic field from a current that passes through it. A changing current (AC) causes a changing magnetic field which induces a voltage that opposes the current produced by the magnetic field. This is known as the inductance.  One could think of an inductor as an AC resistor. But first of all, what is an inductor comprised of?

In simple terms an inductor is a coil of wire, wrapped around a core. The core forms a support for the coil of wire – such as ceramic cores, or in some cases can affect the properties of the magnetic field depending on the chemical composition of the core. These may include cores formed from ferrite (usually zinc and manganese, or zinc and nickel) or powdered iron (which has a tiny air gap allowing the core to store a higher level of magnetic flux (the measure of magnetic field strength)allowing a higher level of DC current to flow through before becoming saturated.

So, the amount of inductance is influenced by several factors – the core material (as above), the size and shape of the core, as well as the number of turns of wire in the coil and its shape. The unit of inductance is the henry (H), however common values are usually in the millihenry (mH) or microhenry (uH) range.

Furthermore, there is an amount of DC resistance due to the properties of the coil wire, however this is usually negligible and kept to a minimum. For example, looking at a data sheet for a typical line of inductors – inductors.pdf – the DC resistance of a 10uH inductor is a maximum of 0.05 ohms. With inductors of higher values, the DC resistance will need to be taken account of. But more about that later.

This is the usual symbol for an inductor in a schematic:

However this may also be used:

And here is a variety of inductors in the flesh:

10microhenryss

radial ferrite core, generally for PCB use, handles around 1.5 amperes

radial leaded, very low resistance, handles around 2.5 amperes

ferrite core, convenient for through-hole PCB

phenolic core

toroidal – handles large currents ~10 amperes depending on model

surface-mount, can still handle around 500 mA

All of the pictured inductors have an inductance of 10 uH. Now let’s examine how inductors work with alternating current. Consider the following circuit:

1

 

Just like capacitors in AC circuits, an inductor has a calculable reactance. The formula for the reactance (X, in ohms) of an inductor is:


where f is the frequency of the AC and L is the value of the inductor in Henries (remember that 1uH is 10 to the power of -6). The formula to calculate the impedance of the above circuit is:

where Z is in ohms. And finally, the formula for AC Vout is

The formula for DC Vout is the usual voltage dividing formula. In this case, as we consider the inductor to not have any resistance, DC Vout = DC Vin.

So, let’s work through an example. Our DC Vin is 12 volts, with a 2V peak to peak AC signal, at a frequency of 20 kHz. The resistor R has a value of 1 kilo ohm, and the inductor L is 10 millihenries (0.01 H). A quick check of the data sheet shows that the 10 mH inductor has a resistance that cannot be ignored – 37.4 ohms. So this must be taken into account when calculating the DC Vout. Therefore we can consider the inductor to be a 37.4 ohm resistor when calculating the DC Vout, which gives us a result of 11.56 volts DC. Substituting the other values gives us a reduced AC signal voltage of 1.24 volts peak to peak.

Another interesting fact is that there is a relationship between AC Vout and the frequency of the AC signal. In the video below, I have used a 10k ohm resistor and a 10 uH inductor in the circuit described above. The frequency counter is measuring the frequency of AC Vin, and the multimeter is measuring the AC Vout:

This is an interesting relationship and demonstrates how an inductor can resist alternating current, depending on the frequency.

Thus ends our introduction to the inductor. We will continue with the inductor in the near future. I hope you understood and can apply what we have discussed today. As always, thank you for reading and I look forward to your comments and so on. Furthermore, don’t be shy in pointing out errors or places that could use improvement, you can either leave a comment below or email me – john at tronixstuff dot com.

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Posted in education, inductor, learning electronics, lesson, test equipment, tutorialComments (0)


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