Tag Archive | "oscillator"

Kit Review – Altronics Pocket Oscillator

Introduction

In this review we examine the Pocket Oscillator Kit from Tronixlabs, based on an design from (the now defunct) February and March 1989 editions of Electronics Australia magazine – and manufactured by Altronics. The purpose of this oscillator is to give you a high quality, portable square or sine wave generator that can be used to test audio equipment, speaker response, fool about with oscilloscopes (!), and so on. The prototype basic specifications are as follows:

  • Frequency range: 41~1082 Hz and 735 Hz~18.1 kHz
  • Output: 1.27V RMS sine, 1.45V peak square
  • Load: 1.0V RMS sine into 330 Ω
  • Distortion: 0.16% THD at 1 kHz

Assembly

The kit is packaged in typical form, without any surprises:

Altronics K2544

In the usual Altronics fashion, the instructions are accompanied with a neat “electronics reference sheet” which covers many useful topics such as resistor colour codes, various formulae, PCB track widths, pinouts and more. The kit instructions are based on the original magazine article and include a small addendum which isn’t any problem.

Unlike some kits, everything is included to create a finished product (except for the IC socket):

Altronics K2544 parts

… including a nice enclosure which has the control instructions screen-printed on the lid…

Altronics K2544 enclosure

However at this point I think the definition of a “pocket” is the same used by Sir Clive Sinclair when he had those pocket televisions. At this time I won’t use the enclosure as my drill press is in storage, however look forward to fitting the kit within at a later point. The PCB has a neat solder mask and silk screen:

Altronics K2544 PCB top

Altronics K2544 PCB bottom

Assembly was pretty straight forward, the original design has tried to minimise PCB real-estate, so all the resistors are mounted vertically. The signal diodes take this a step further – each pair needs to be soldered together:

Altronics K2544 diodes

… then the pair is also mounted vertically:

Altronics K2544 diodes mounted

However it all works in the end. The rest of the circuit went together well, and we used our own IC socket for the opamp:

Altronics K2544 assembled PCB

From this point you need to wire up the power, switches and potentiometers:

Altronics K2544 assembly

… and consider mounting the whole lot in the enclosure (or before assembly!):

Altronics K2544 lid

However as mentioned earlier, I just went for the open octopus method for time being:

Altronics K2544 finished

How it works

The oscillator is based around the Texas Instruments TL064 opamp, and due to copyright I can’t give you the schematic. For complete details on the oscillator, either purchase the kit or locate the February and March 1989 edition of Electronics Australia magazine. However the waveforms from the oscillator looked good (as far as they can on a DSO):

Altronics Pocket Audio Oscillator K2544 sine wave output

Altronics Pocket Audio Oscillator K2544 sine wave output

Altronics Pocket Audio Oscillator K2544 square wave output

Altronics Pocket Audio Oscillator K2544 square wave output

Conclusion

The oscillator works well, however the PCB layout could have been a little lot easier on the end-user. It’s time for a redesign, possibly put all the contacts for external switches around the perimeter – and allow space for the diodes to lay normally. Nevertheless – this is a neat kit, and still quite popular after all these years. For the price you get a few hours of kit fun and a useful piece of test equipment. So if you’re into audio or experimenting, check it out. Full-sized images are available on flickr.

Finally, check out tronixlabs.com – which along with being Australia’s #1 Adafruit distributor, also offers a growing range and great value for supported hobbyist electronics from Altronics, DFRobot, Freetronics, Jaycar, Seeedstudio and much much more.

visit tronixlabs.com

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 altronics, K2544, kit, kit review, tronixstuffComments (2)

Rapid stripboard prototyping made easy with Lochmaster

Introduction

As a beginner in the world of electronics, sooner or later you’ll want to make a more permanent project than what can be constructed on the solderless breadboard. It’s easy to say “make your own PCBs” – however this can introduce a steep learning curve, not to mention the cost and time involved in waiting for PCBs to arrive – and hoping they’re correct. Thus for many people a happy medium is transferring prototype circuits over to stripboard – it’s really cheap (check ebay), you can keep various sizes on hand, and it’s quick.

However planning more complex circuits can be difficult – so it would be much easier with the use of a software design tool. Which brings us to the subject of our review – the Lochmaster v4.0 software from Abacom. It’s an incredibly easy to use developer’s tool for strip board projects. No more loose pieces of graph paper, soldering parts “one row too far over”, or lost design plans – you can now design stripboard projects efficiently and with ease.

Installation

Available for all versions of Windows from XP to 8, Lochmaster is less than ten megabytes and is distributed electronically after purchase – so backup your installation file when received. Otherwise it’s a quick install, you don’t need any extra framework software and due to the size will run well on less-specified machines. Although we have screen shots in the review below, you can download a trial version – so it won’t cost you anything to check it out yourself.

Designing your circuits

Once installed, opening Lochmaster for the first time you’re presented with a blank example of stripboard ready for your components:

Lochmaster

However you can also use different types of prototyping board, such as varieties with all holes, edge connectors, mounting holes, different copper directions – or even make your own board to match a preferred style. Boar dimensions can be displayed in measurement units as well as “holes”. Then it’s a simple matter of selecting a part library from the drop-down list on the left of the window. For example, to add a 555 timer (which is an 8-pin DIL part) select the “ICs” library, click on the 8-pin enclosure and the following window appears, prompting you to fill out the appropriate details such as label, type etc:

Lochmaster 555

… then you can drop the 555 on the board. It then becomes an object which can be dragged around and placed where you need it. You can also create and modify the component libraries, and also create your own custom parts.

At that point, you might want to cut the tracks on the other side of the board. By clicking the “turn around” button the menu bar, you’re presented with the bottom of the board. Using the “add/split” button on the vertical toolbar between the library and the board, you can then virtually cut the tracks, for example:

lochmaster

You can also see the rounded circles which represent solder joints. After a few minutes we found dragging and dropping components onto the board very simple, and with the turn-around button you can easily flip sides until the placement looks good. After placing components, running the necessary links or wires is simple with the “draw jumper wire” tool. They can run in any direction, and also have corners, for example:

Lochmaster wires

You can also adjust the colours and thickness of the wires,  and of course can also be placed on the other side of the board – just flip it around and place the wires. After wiring things up and getting to the stage when you’re ready to build – you can test the connections to ensure you haven’t mis-counted holes or tracks. Using the “Test mode” tool you can click on tracks and the sections that are electrically connected to the point with the cursor are all highlighted – for example if you click on the point marked by the black arrow below, the connected tracks are highlighted:

lochmaster test

If you don’t like the 3D-rendered components, you can also work with normal 2D in colour or black and white:

lochmaster 2D

For final quality-control, you can also review the project at any time with “X-ray” view, which shows an outline of the parts on the other side, for example when looking at the bottom of the board, turning on X-ray results with:

Lochmaster xray

You can also generate component lists, which are great for documentation or simply making up a shopping list. It can be exported to .xls or text file, for example:

lochmaster list

And then you can export your project as an image (.jpg or .bmp), HPGL machine file – and print out both sides to serve as an assembly guide. There is also standalone file-viewer software, so you can share your designs with others who haven’t got the full Lochmaster software installed.

Example project

After experimenting with Lochmaster for a short while, we decided to test using it with a real project that a beginner might assemble. For example, a square wave oscillator from an old Talking Electronics magazine (click image for larger version):

square wave oscillator

Nothing too complex, but a useful tool for anyone experimenting with electronics. It’s a 555 astable with six different RC values which allows you to select from 1, 10, 100, 1 k, 10 k and 100 kHz outputs. The first step is to gather all the components together, so you know the widths and number of holes each needs on the stripboard:

lochmaster_components

The next step is to measure the board, as you can enter the dimensions via Board>Edit board layout… into Lochmaster to avoid having excess space in the design plan. Then after consulting the schematic and the single-layer PCB layout from the magazine, it’s a simple matter of placing the parts onto the virtual board after checking how the fit in on the real thing:

osciillator top

… and the flip-side:

oscillator bottom

Not a work of art – but it works.  (We didn’t fit the 100 kHz setting, as the capacitor wasn’t in stock). And that’s the neat thing – you can experiment with placement until you’re happy, then double-check connections before soldering. You might find even after some planning, that you may deviate from the plan. Fair enough, but just double-check what you’re doing. And a short while later, the results, top and bottom:

oscillator PCB top

oscillator PCB bottom

Conclusion

If you’re a beginner and don’t have the time, money and patience to design your own PCBs – Lochmaster is ideal. It’s a neater way to visualise physical circuits, as well as filing and sharing them with others.   To order your own copy, get the trial version, or if you have any questions please contact Abacom. Full-sized images of the screen-shots can be found on flickr. And if you made it this far – check out my new book “Arduino Workshop” from No Starch Press.

In the meanwhile 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? And join our friendly Google Group – dedicated to the projects and related items on this website. Sign up – it’s free, helpful to each other –  and we can all learn something.

[Note – Lochmaster software license was a promotional consideration from Abacom]

Posted in lochmaster, software review, stripboard, tronixstuff, tutorial, veroboardComments (1)

Various 555 Timer circuits

Hello readers

The purpose of this article is to follow on from our explanation of the 555 timer IC by demonstrating some simple yet interesting, noisy and plain annoying uses of the 555. They are by no means that complex, and intended to help move theory into practice.

Button de-bouncer

De-bouncer? How does one bounce a button in the first place? Many years ago I bounced a button on the arcade Sonic the Hedgehog – hit it so hard it popped out and bounced over the table… But seriously, when working with digital logic circuits, you may need to use  a momentary button to accept user input. For example, to pulse a trigger or so on. However with some buttons, they are not all that they seem to be. You press them once, but they can register multiple contacts – i.e. register two or more ‘presses’ for what seems like only one press. This could possibly cause trouble, so we can use a 555 timer monostable circuit to solver the problem. In our de-bounce example, when the button is pressed, the output is kept at high for around half a second. Here is the schematic:

555debouncesch

What we have is a basic monostable timer circuit. For my example the output delay (t) is to be half a second. The formula for t is: t=1.1xR1xC1. The closest resistor I had at hand was 2k ohms, so to find the required value for C1, the formula is rearranged into: C1=t/(1.1xR1). Substituting the values for t and R1 gives a value of C1 as 227.274 uF. So for C1 we have used a 220 uF capacitor.

Now for a visual demonstration of the de-bouncer at work. In the following video clip, the oscilloscope is displaying the button level on the lower channel, and the output level on the upper channel. The button level when open is high, as the 555 requires a low pulse to activate. The output level is normally low. You can see when the button is pressed that the button level momentarily drops to low, and then the output level goes high for around half a second:

Make some noise

As we know the 555 can oscillate at frequencies from less than 1Hz to around 500 kHz. The human ear can theoretically hear sounds between (approximately) 20 and 20 kHz. So if we create an astable timing circuit with an output frequency that falls within the range of the human ear, and connect that output to a small speaker – a range of tones can be emitted.

The circuit required is a standard 555 astable, with the output signal heading through a small 8 ohm 0.25 watt speaker and a 4.7 uF electrolytic capacitor to ground. The capacitor stops any DC current flowing to ground, without this we will overload the current-handling ability of the 555. (I couldn’t help myself by trying it without the capacitor – pulled 550 mA from the 555 before it stopped working…). To choose the values of R1 and C1 to emit out required frequency, the following formula is used: f (frequency) = 1.4 / {(R1 + [2 x R2]) x C1}. To cover the range required, a 100k ohm trimpot was used for R1. Here is the resulting schematic:

noisemakersch

The input voltage can fall within the specification of the 555, however for optimum results a supply of between 5 and 9 volts DC should be used. In the following demonstration, we used a 9V supply. The purpose of the video is to learn the relationship between the tones and their frequencies. You can see the frequency on my old counter and hopefully hear the result:

Our next example is to create a  siren effect, using two 555 circuits – one for a low frequency and one for a high frequency. To determine the value for R1 for the low and high frequency, I used the previous circuit and chose two tones that were quite different, and measured the resistance of the trimpot (R1) at those frequencies. My R1 value for the ‘low’ tone is 82k ohm and 36k ohm for the ‘high’ frequency.

The switching between low and high frequency will be handled by a 4047 multivibrator – the Q and Q outputs will control NPN transistors. The transistors are used as switches to allow current to flow from the supply to the 555 high or low tone circuit. We use this method as the 4047 is not able to source enough current to drive the 555 circuits. Here is the schematic:

555siren

Don’t forget to connect pin 14 of the 4047 to supply voltage. This circuit has been tested with a supply voltage between 5 and 12 volts. As the supply voltage increases, so does the amplitude of the square wave emanating from the 555 output pins, which in turn in creases the volume of the siren. At 5 volts, the entire circuit drew only 20 milliamps. Speaking of which, you can listen to a recording of the output here. If you wish to alter the time for each tone, adjust the value of what is the 47k ohm resistor on pins 2 and 3 of the 4047.

In the meanwhile 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? And join our friendly Google Group – dedicated to the projects and related items on this website. Sign up – it’s free, helpful to each other –  and we can all learn something.

Posted in 4047, 555, arduino, COM-09273, education, learning electronics, lesson, tutorialComments (0)

Part review – Linear Technology LTC6991 “Timerblox” low frequency oscillator

Hello Readers

Time for a new component review – the Linear Technology LTC6991 low frequency oscillator. This is part of Linear‘s Timerblox series of tiny timing devices. The full range is described on their web site. It is available in DFN or SOT-23 (below)  packaging. Our example for today:

The graph paper in the image is 5mm square, so the IC itself is tiny yet worthwhile challenge. Although reading the data sheet may convince you it is a difficult part to use, it is actually quite simple. This article will give you the “simple way”. Once again I have lashed out and will hand-solder an SMD onto a SOT-23 board:

Messy, but it works. Moving along…

My reason for examining the LTC6991 was as a lower-power substitute to using a 555 timer to create a square wave at various frequencies. Normally I wouldn’t give two hoots about the current draw, as everything on my bench is powered from a lab supply.

However when designing things for external use, they are usually powered by a battery of some sort or solar – so the less current drawn the better. The bog-standard TI NE555 has a current draw (with output high) of between two and five milliamps (at 5V). Which doesn’t sound like much – but our 6991 is around 100 to 170 microamps at 5V. These figures are for the respective timers without an output load. You can source up to 20mA from the output of the 6991, and when doing so will naturally increase the current load – but still it will be less than our triple-nickel.

The LTC6991 offers a period range of 1 millisecond to 9.5 hours; which translates to a frequency range of 29.1 microhertz to 977 Hz, with a maximum frequency error or <1.5%. Only one to three external resistors are required to setup your timing requirements. For a more detailed explanation, please see the data sheet.pdf. The duty cycle defaults to 50% however this can be altered by using the IC in voltage-controlled period mode.

Linear have made using the IC very easy by providing an Excel spreadsheet you can use to make your required calculations, available from this page. For example, to create a 1 Hz oscillator, we enter our figures in as such:

and the macro returns the following details:

xls2

Very convenient – a schematic, the required resistors, and example timing diagram. I recreated this example, however not having the exact values in stock caused a slight increase in frequency – with Rset at 750k,  Rdiv1 at 910k and Rdiv2 at 180k my frequency was 3.1 Hz. Therefore to match the accuracy of the LTC6991 you need to ensure a your external components are close to spec and a very low tolerance. It produces a good square-wave:

sqw1hzss

If you cannot use the exact resistor values recommended, use resistors in series or parallel to achieve the desired values. Don’t forget to measure them in real life if possible to ensure your accuracy does not suffer.

Pin one (RST) can be left floating for nomal oscillation, when high it resets the IC and forces output (pin six) low. As you can see, it is very simple to use especially with the provided spreadsheet. The required formulae are also provided in the data sheet if you wish to do your own calculations. Pulse width can be controlled with a fourth resistor Rpw, and is explained on page sixteen of the data sheet.

Although physically it may be difficult to use as it is SMD, the power requirements and the ability to generate such a wide range of oscillations with so few external parts makes the LTC6991 an attractive proposition.

The LTC6991 and the Timerblox series are new to market and should be available from the usual suppliers in the very near future such as RS and element-14.

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. Please subscribe using one of the methods at the top-right of this web page to receive updates on new posts. Or join our Google Group.

[Note – The LTC6991was a personally-ordered sample unit from Linear and reviewed without notification]

Posted in education, LTC6991, part review, tutorialComments (4)

Education – the RC circuit

Hello readers

Today we continue down the path of analog electronics theory by stopping by for an introductory look at the RC circuit. That’s R for resistor, and C for capacitor. As we know from previous articles, resistors can resist or limit the flow of current in a circuit, and a capacitor stores electric current for use in the future. And – when used together – these two simple components can be used for many interesting applications such as timing and creating oscillators of various frequencies.

How is this so? Please consider the following simple circuit:

rccircuit

 

When the switch is in position A, current flows through R1 and into the capacitor C1 until it is fully charged. During this charging process, the voltage across the capacitor will change, starting from zero until fully charged, at which point the voltage will be the same as if the capacitor had been replaced by a break in the circuit – in this case 6V. Fair enough. But how long will the capacitor take to reach this state? Well the time taken is a function of several things – including the value of the resistor (R1) as it limits the flow of current; and the size of the capacitor – which determines how much charge can be stored.

If we know these two values, we can calculate the time constant of the circuit. The time constant is denoted by the character zeta (lower-case Greek Z).

The time constant is the time taken (in seconds) by the capacitor C that is fed from a resistor R to charge to a certain level. The capacitor will charge to 63% of the final voltage in one time constant, 85% in two time constants, and 100% in five time constants. If you graphed the % charge against time constant, the result is exponential. That is:

Now enough theory – let’s put this RC circuit to practice to see the voltage change across the capacitor as it charges. The resistor R1 will be 20k ohm, the capacitor 1000 uF.

Our time constant will be R x C which will be 20000 ohms x 0.001 farads, which equals 20 (seconds).  Notice the unit conversion – you need to go back to ohms and farads not micro-, pico- or nanofarads. So our example will take 20 seconds to reach 63% of final voltage, and 100 seconds to reach almost full voltage. This is assuming the values of the resistor and capacitor are accurate. The capacitor will have to be taken on face value as I can’t measure it with my equipment, and don’t have the data sheet to know the tolerance. The resistor measured at 19.84 k ohms, and the battery measured 6.27 volts. Therefore our real time constant should be around 19.84 seconds, give or take.

First of all, here is a shot of the little oscilloscope measuring the change in voltage over the capacitor with respect to time. The vertical scale is 1v/division:

And here is the multimeter measuring the voltage next to a stopwatch. (crude yet effective, no?)

The two videos were not the most accurate, as it was difficult to synchronise the stopwatch and start the circuit, but I hope you could see the exponential relationship between time and voltage.

What about discharging? Using the circuit above, if we moved the switch to B after charging the capacitor –  and R2 was also 20k ohm – how long would it take to discharge the capacitor? Exactly the same as charging it! So one time constant to discharge 63% and so on. So you can take the graph from above and invert it as such:

How can we make use of an RC circuit?

I’m glad you asked. Consider the following circuit:

pic23

When power is applied, the capacitor starts to charge, and in doing so allows current to flow to the emitter of the transistor, which turns on the LED. However as the capacitor charges, less current passes to the base of the transistor, eventually turning it off. Therefore you can calculate time constants and experiment to create an off timer. However, a preferable way would be to make use of a 555 timer. For example, an RC combination is used to set the pulse length used in astable timing applications, for example using R1, R2 and C1:

555astable

(For more information on the 555 timer, please read this article)

Another use of the RC circuit is oscillating. Due to varying capacitor values due to tolerance, you most likely cannot make precision frequency generators, but you can still have some fun and make useful things. Here is a classic oscillator example – an astable multivibrator:

multivib1

What is going on here? Here it is in action:

and here is one side being measured on the little scope:

We have two RC circuits, each controlling a transistor. When power is applied, there is no way to determine which side will start first, as this depends on the latent charge in the capacitors and the exact values of the resistors and capacitors. So to start let’s assume the left transistor (Q1) and LED are on; and the right transistor (Q2) and LED are off. The voltage at collector of Q1 will be close to zero as it is on. And the voltage at the base of Q2 will also be close to zero as C2 will initially be discharged. But C2 will now start charging via R4 and base of Q1 to around 5.4V (remember the 0.6v loss over the base-emitter junction of a transistor). While this is happening, C1 starts charging through R2. Once the voltage difference reaches 0.6V over the capacitor, Q2 is turned on.

But when Q2 is on, the voltage at the collector drops to zero, and C2 is charged, so it pulls the voltage at the base of Q1 to -5.4v, turning it off and the left LED. C1 starts charging via R1, and C2 starts charging via R3 until it reaches 0.6v. Then Q1 turns on, bringing the base of Q2 down to -5.4V – switching it off. And the whole process repeats itself. Argh. Now you can see why Arduino is so popular.

Time for a laugh – here is the result of too much current through a trimpot:

So there you have it – the RC circuit. Part of the magic of analogue electronics! And if you made it this far – check out my new book “Arduino Workshop” from No Starch Press.

In the meanwhile 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? And join our friendly Google Group – dedicated to the projects and related items on this website. Sign up – it’s free, helpful to each other –  and we can all learn something.

Posted in education, learning electronics, lesson, multivibrator, RC circuit, tutorialComments (12)


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