Getting Started
The purpose of this board is to learn how to perform basic measurements with an oscilloscope. Most experiments can be performed with any digital storage scope. Some experiments can be performed with an analog scope.
Experiments in this project are performed using the Velleman HPS140 Handheld Pocket Scope. All experiments require basic knowledge of terms such as AC and DC voltage, current, resistance, etc...
Make sure to check YouTube as well; it features a short movie for each experiment.
Manual Downloads
- UK: See the product page on our website for the latest available translated manual.
- NL: Download de laatst beschikbare vertaalde handleiding op de product-pagina van onze website.
- FR: Consultez la fiche technique sur notre site web pour la toute dernière version de la traduction du mode d'emploi.
- D: Eine aktuelle Version der deutschen Bedienungsanleitung finden Sie auf der Produktseite unserer Website.
- ES: Para descargarse el manual del usuario en español más recientes, consulte la página del producto en nuestra web.
Warranty
This product is guaranteed against defects in components and construction from the moment it is purchased and for a period of TWO YEARS starting from the date of sale. This guarantee is only valid if the unit is submitted together with the original purchase invoice. Velleman Ltd limits its responsibility to the reparation of defects or, as Velleman components Ltd deems necessary, to the replacement or reparation of defective components. Costs and risks connected to the transport, removal or placement of the product, or any other costs directly or indirectly connected to the repair, will not be reimbursed by Velleman components Ltd. Velleman components Ltd will not be held responsible for any damages caused by the malfunctioning of a unit.
Oscilloscope Basics
What is an Oscilloscope?
While a multimeter shows an instant voltage level or an average voltage level, an oscilloscope is capable of displaying voltage levels over a period of time. Voltage is displayed vertically versus time (X-axis).
Applications
- Looking at the shape of a signal.
- Measuring the amplitude and frequency of a signal.
- Measuring the time between two events.
- Looking for anomalies such as clipping, noise, distortion, spikes, ripple, etc...
Analog vs. Digital
There are two basic types of oscilloscopes: analog and digital scopes. Each type has its typical applications, advantages, and disadvantages. The advantage of digital scopes is that they are able to capture and store events for further study. They are also more user-friendly, as they require less setup in order to show a picture of your signal. For our experiments, we will use a digital scope.
Waveforms
An oscilloscope will mainly display and measure waveforms. A wave is a pattern that repeats over time, e.g., the waves of the sea. One cycle or period of a wave is the part of the wave that repeats itself. When shown on the screen of an oscilloscope, it is called a waveform. There are many different waveforms. A couple of them will be used in our experiments:
- 1. Sine waves: A typical example: The AC power grid. [Diagram: A smooth, oscillating sine wave.]
- 2. Full-wave rectified AC: The output of a full wave diode rectifier. [Diagram: A rectified sine wave where both positive and negative halves are present, but the negative halves are flipped to be positive.]
- 3. Half-wave rectified AC: The output of a half-wave diode rectifier. [Diagram: A rectified sine wave where only the positive halves are present, with gaps where the negative halves would be.]
- 4. DC voltage: Yes, oscilloscopes can also measure DC. [Diagram: A flat horizontal line representing a constant DC voltage.]
- 5. Sawtooth waveform: In this case: ripple. [Diagram: A waveform that rises linearly and then drops sharply.]
- 6. Square wave: The board features a simple two-transistor oscillator which produces a square wave. [Diagram: A waveform that alternates between two distinct voltage levels.]
Measuring Probe
To be able to display waveforms, we need to connect the signal to the input of the oscilloscope. Similar to a multimeter, the oscilloscope uses a measurement lead, but here it is called a 'probe'.
Setting Up the Board
The board requires a 9VAC (Alternating Current) adaptor (e.g., Velleman PS905AC (230VAC)). A DC adaptor instead of an AC adaptor will not damage the board, but most experiments will not work correctly. Connect the adaptor at the left-hand side of the board and plug it in.
Once powered, the LEDs (LD2 & LD3) should blink alternately. The board is now ready to perform experiments.
Experiment 1: Measuring AC Voltage
Connection Layout
Connection Summary
GND clip: 2
Probe tip: 1
Purpose
The purpose of this experiment is to display and measure AC voltage. In this particular case, we will measure the AC voltage supplied to the board.
How To
- Turn on the HPS140 Handheld Pocket Scope (refer to the HPS140 manual for instructions).
- Place the probe switch "x1/x10" to 'x1'.
The unit always starts up in 'auto-setup' mode. You can tell that it is in auto-setup mode because the readouts for Volts/div and Time/div are displayed in 'reverse video' (white characters on dark background). Thanks to the auto-setup mode, the unit automatically sets V/div and time/div for you. In the lower right-hand corner, the RMS value of the supplied AC voltage is displayed. More about auto-setup is covered in the next experiment.
What We See
- Select 'AC coupling' (refer to the HPS140 manual for instructions).
- Set time/div to 5ms/div.
- Set volts/div to 10V/div.
Note: The readout in the bottom right-hand corner displays the RMS value of the measured AC voltage. Different readouts are available (refer to the HPS140 manual for instructions). Note: If you live in an area where the AC grid frequency is 60Hz instead of 50Hz (e.g., US), the image may slightly vary.
Experiment 2: Adjustable AC Voltage (Advantages of the Auto-Setup Function)
Connection Layout
Connection Summary
GND clip: 2
Probe tip: 3
Purpose
The purpose of this experiment is to show the advantages of the auto-setup function to measure AC voltage.
How To
- Turn on the HPS140 Handheld Pocket Scope (refer to the HPS140 manual for instructions).
- Place the probe switch "x1/x10" to 'x1'.
Trimmer RV1 allows us to adjust the output voltage on test point 3 between 0V and the full input voltage. Turn RV1 fully anti-clockwise (0V output). The trace on our oscilloscope screen remains a flat line, as there is no input voltage.
Next, set V/div to 50mV/div (refer to the HPS140 manual for instructions).
Slightly turn RV1 clockwise until a sine wave is displayed on the screen. You only need to turn it slightly before the signal appears. If the signal goes 'off-screen', turn RV1 anti-clockwise until the signal is correctly displayed. In the lower right-hand corner, you can read the current RMS value of the AC voltage measured, e.g., 100mV (0.1V).
Turn RV1 a little further clockwise. The signal goes off-screen, and the Vrms readout displays an error, because the unit is no longer capable of calculating the correct Vrms.
How can we display the current signal correctly again? Increase the V/div setting to 0.1V/div. As you will see, the signal fits the screen again.
If you turn RV1 clockwise again, the signal will go off-screen again. Changing V/div to 0.2V/div once again restores the display.
You can continue this process until RV1 is turned fully clockwise. In that case, we will measure the full input voltage, which we also measured in Experiment 1.
Is there a better way of measuring unknown voltages? Yes, there is, by using the 'auto-setup' function. Keep pressing any of the arrow keys until V/div and time/div are displayed in reverse video. The trace immediately adjusts for optimal viewing. Now you can adjust the voltage from 0 to max. by turning RV1. At any time, the trace will be displayed correctly and it will not go off-screen. At the lower right-hand corner, the current Vrms will be correctly displayed.
Experiment 3: Measuring AC Grid Frequency and Period
Connection Layout
Connection Summary
GND clip: 2
Probe tip: 3
Purpose
The purpose of this experiment is to demonstrate the use of the markers to perform on-screen measurement of frequency and period.
How To
- Turn on the HPS140 Handheld Pocket Scope (refer to the HPS140 manual for instructions).
- Place the probe switch "x1/x10" to 'x1'.
Press the lower right button; this will freeze the screen and turn on the markers. The upper right button allows us to toggle between the different markers.
There are 4 markers: two horizontal and two vertical. The horizontal markers allow us to measure the amplitude of a displayed signal (i.e., how many volts there are between both markers). The vertical markers allow us to measure time between the two markers. In order to measure the frequency of a periodic signal, we can use the vertical markers and isolate one period of the signal.
Press the upper right button repeatedly to select vertical marker 1. Next, use the arrow keys to position marker 1 on the sine wave as shown.
Press the upper right button again to select vertical marker 2. Use the arrow keys to position this marker at the exact same location but further to the right of the screen.
You have now selected one period or cycle of the displayed waveform. In the lower right corner, the unit displays the time between the two markers. In most cases, this will be 20ms (16.66ms). The value displayed is called the period of a waveform, i.e., the time before it repeats itself.
Now for the frequency (= the number of periods per second). Press and hold the upper right-hand button until the menu appears.
When the menu appears, release the button and press it again a number of times until 'time mark' is displayed in reverse video. Next, press any arrow key once to change the mode from 'time mark' to 'freq mark'. Release all buttons and wait until the unit exits the menu.
Look in the lower right corner. The readout now displays frequency. In most cases, this will be 50Hz (60Hz).
Good to know: The AC power grid frequency in most parts of the world is 50Hz. The US, Japan, and some parts of Central and South America have 60Hz power.
Experiment 4: Rectified AC, Single Phase
Connection Layout
Connection Summary
GND clip: 4
Probe tip: 5
Purpose
The purpose of this experiment is to show what single-phase rectified AC looks like on a scope screen.
How To
- Turn on the HPS140 Handheld Pocket Scope (refer to the HPS140 manual for instructions).
- Place the probe switch "x1/x10" to 'x1'.
- Make sure to flip SW1 to the correct position (for single-phase rectification).
Select 5ms/div and 4V/div.
The display will show a signal similar to this one:
A Little Theory
With a single diode, we can convert an AC voltage to a DC voltage. As a diode only conducts the current in one way, only one half of the waveform can pass. The other half, with inverted polarity, is blocked. As you can see on the screen, the trace shows 'interruptions' where the voltage is 0. This is the part of the AC voltage that is blocked by the diode. If you move the probe clip from test point 5 to test point 1, you remove the diode from the circuit, and the display shows the complete waveform again.
Good to know: Should the rectifier diode be defective, then you will see either the complete waveform (if the diode is shorted) or no waveform at all (if the diode is open-circuit).
Experiment 5: Rectified AC, Dual Phase
Connection Layout
Connection Summary
GND clip: 4
Probe tip: 5
Purpose
The purpose of this experiment is to show what dual-phase rectified AC looks like on a scope screen and to show the difference with single-phase rectified AC.
How To
- Turn on the HPS140 Handheld Pocket Scope (refer to the HPS140 manual for instructions).
- Place the probe switch "x1/x10" to 'x1'.
Select 5ms/div and 4V/div.
As the switch is still set to single-phase rectification, the display will show the same trace as with Experiment 4.
Now, check what happens when you flip the switch from single phase to dual phase rectification. Flip the switch back and forward to clearly see the difference between both settings.
A Little Theory
As you can see, the 'interruptions' we have noticed with single-phase rectification are gone. As opposed to single-phase rectification, both halves of the sine wave are used. Instead of a single diode, we use 4 diodes to make a 'diode bridge'.
Exercise
In Experiment 3, we learned how to measure the frequency of a repeating waveform. Can you measure the period and frequency of both the single-phase and dual-phase rectified signal?
(Answer: 10ms/100Hz or 8.33ms/120Hz)
Experiment 6: Smoothed Versus Unsmoothed DC (Ripple)
Connection Layout
Connection Summary
GND clip: 4
Probe tip: 6
Purpose
The purpose of this experiment is to show what smoothed and unsmoothed DC looks like on a scope screen and how a scope can help you to determine the quality of your DC supply.
A Little Theory
In the previous experiments, we have used one or more diodes to convert an AC voltage into a DC voltage. The result was OK, but far from perfect. Why? Because it was still far from the flat line one would expect when measuring a perfect DC voltage. It is clear that our rectified AC voltage needs 'smoothing'. This can be done with an electrolytic capacitor (see diagram of this board).
How To
- Place the probe switch "x1/x10" to 'x1'.
- Make sure to flip SW1 to the correct position (for single-phase rectification).
- Turn on the HPS140 Handheld Pocket Scope. It will start-up in auto-setup mode as always.
Watch the screen closely. You will notice that the trace is almost flat, so the capacitor is doing a good job at smoothing our rectified AC voltage. Yet, it still wobbles a bit.
If you flip the switch from single-phase to dual-phase rectification, the wobbling will be reduced.
Why is this? Basically, the capacitor acts as a temporary storage device. It provides power to the rest of the circuit during the 'interruption' of the waveform (remember, single-phase rectification?). With dual-phase rectification, this interruption is not present, so the capacitor has less work to do. The remaining 'wobble' of the waveform is called 'ripple'. One of the key features of a good DC supply is low ripple.
Can we measure this amount of ripple? Yes, we can; a scope is the ideal tool for ripple measurement.
Flip SW1 back to single-phase rectification.
Default, your scope starts up with 'DC-coupling' selected. Change that to 'AC-coupling' (refer to the manual for how-to instructions).
Now, the scope will only show the AC part of the signal; the DC part will be blocked. Make sure it is still in 'auto-setup' mode.
If you look at the screen below and your scope screen, you will see a kind of 'sawtooth' waveform; this is the 'ripple' voltage that rides on top of your DC voltage. During the rising edge, the power supply charges the capacitor; during the falling edge, the capacitor supplies current to the circuit.
If more current is drawn from the supply, the ripple will be higher, as the capacitor will be drained more, so it will not be able to keep the output as steady as it would with a small load.
How can we reduce the ripple? Try flipping SW1 for single-phase to dual-phase rectification and watch the screen. Check the lower right-hand corner. It displays the RMS ripple voltage. Flip the switch back and forward. It is clear that ripple is reduced when dual-phase rectification is used.
Good to know: Use 1000µF per ampère, so e.g., if you design a 2A power supply, you need a smoothing capacitor of at least 2000µF (2200µF is the closest value that is suited for your purpose).
Experiment 7: DC Measurement
Connection Layout
Connection Summary
GND clip: 4
Probe tip: 6
Purpose
The purpose of this experiment is to show that a scope is also suited to measure DC voltages. In general, scopes are used to measure AC voltages. For DC voltages, a multimeter is fine. However, if you don't have a multimeter at hand, you can still perform DC measurements with a scope.
MAKE SURE THE SCOPE IS SET UP CORRECTLY FOR DC MEASUREMENTS
How To
- Place the probe switch "x1/x10" to 'x1'.
- Turn on the HPS140 Handheld Pocket Scope; it will turn on in 'auto-set' mode. 'Auto setup' will also work for DC measurements.
There are 3 important settings that need to be performed for correct DC measurement:
- DC input coupling
- DC readout
- DC reference
DC Input Coupling
Input coupling needs to be set to DC (DC). When set to AC, the scope will block any DC signal, so we won't be able to perform DC measurements. At start-up, the unit is automatically set to DC coupling.
DC Readout
Next, we will set the readout in the bottom right-hand corner to DC. Press and hold the upper right-hand button until the menu appears. Release the button and press it again a number of times until the 'readout' setting is highlighted (123 appears in the lower left-hand corner). Next, press any of the arrow keys repeatedly until Vdc is displayed. Wait for the unit to return to the scope screen.
It now displays the measured DC voltage in the lower right-hand corner.
DC Reference
To set the DC reference, set the input coupling to GND and wait a couple of seconds, until the DC readout in the lower right-hand corner displays '0.0mV'.
If the settings have been performed correctly, your scope will now show a flat trace above the centre of the screen and the readout in the bottom right-hand corner will show the measured DC voltage.
Don't forget to switch it back to 'DC coupling' again.
Exercise
If you move the probe clip to test point 7 or test point 8, you will notice that the scope will automatically adapt the V/div setting and the measured DC voltage will drop to 2/3 or 1/3 of the original value, because of the resistor divider R2/R3/R6.
What happens if you swap the probe tip and ground clip?
Probe tip to test point 4, ground clip to test point 6.
The trace jumps from above the centre of the screen to below centre, and the readout shows the same value, but negative. This is logical, as the ground clip is the ground or (-) and the probe clip is the positive of our instrument. Test point 4 is at ground level while test point 6 is positive, so we get a negative readout.
Experiment 8: Waveform with Adjustable Frequency
Connection Layout
Connection Summary
GND clip: 4
Probe tip: 9
Purpose
The purpose of this experiment is to demonstrate the use of the 'trigger'-function.
How To
- Place the probe switch "x1/x10" to 'x1'.
- Flip SW1 into the 'full wave'-position.
- Turn on the HPS140 Handheld Pocket Scope; it will turn on in 'auto-setup' mode. Select DC coupling.
- Set unit to 10ms/div and 2V/div. Adjust RV2 and RV3 in such a way that the waveform looks like the screenshot below.
The unit displays a square wave. The rising edge of the square wave is not perfectly 'square', due to the limitations of this simple two-transistor circuit. Anyway, the resulting waveform is fine for our experiment.
As you can see, the displayed waveform is perfectly stable; it does not jump from left to right. The circuit responsible for this is the triggering circuit.
How Does It Work?
Take a close look at the left-hand side of the screen, where the waveform starts. You will see a vertical line with a small 'gap'. In this gap, a 'slope'-symbol is displayed. This 'gap' determines the trigger point, the place where the scope will 'trigger' or will start drawing the waveform on the screen.
Press and hold the upper right-hand button to enter the menu. Release and press again a number of times until 'Trg Level' is highlighted. Wait until the unit quits the menu.
Now look at the bottom left-hand side of the screen; the trigger symbol is displayed.
The arrow buttons allow you to shift the trigger level up or down. Check out what happens if you move it all the way down. At a certain point, the waveform becomes unstable and starts scrolling from right to left. If you look closely, this happens when the trigger point is shifted below the bottom of the waveform. If you shift it up again, so that the trigger point is located between the bottom and the top of the waveform, it will be stable again.
It is even possible to use the trigger setting to exactly determine the point where the scope will trigger. Try moving the trigger gap up and down between the top and bottom of the waveform. The waveform will shift horizontally in such a way that the beginning of the trace corresponds with the trigger level.
What is the Purpose of the 'Slope'-Symbol?
Let's change the slope and see what happens. Press and hold the upper right button to enter the menu. Release the button and press it a number of times until 'Slope' is highlighted. Wait for the unit to exit the menu. Now look at the bottom left-hand side of the screen; the slope symbol is displayed. Press any arrow key to toggle between rising and falling slope. Take a look at the waveform and see what happens.
So, the slope setting also determines where the scope will trigger. This can be on the rising or on the falling slope of the signal.
Conclusion
Trigger- and slope settings allow us to get a stable signal and make it easier for us to study parts of a complex signal.
We encourage you to further experiment with your oscilloscope. Try looking at various signals from all kinds of sources. Just make sure that you respect the maximum input voltage of your scope (100Vp with probe set to x1). If in doubt, begin by setting the probe to x10. We do not encourage you to perform measurements on 'live' equipment, i.e., equipment that is connected to the power grid, without a transformer. These circuits are unsafe. Examples of unsafe circuits are: some household appliances, old TV sets, dimmer circuits, switch mode power supplies, etc. Battery-operated equipment is usually safe.
Glossary
Definitions
- AC voltage: (AC: Alternating Current) With AC, the flow of the current periodically reverses, as opposed to DC, where the current flows in one direction. An AC source does not have a polarity.
- Analog: Analog scopes use the incoming signal to deflect an electron beam, which scans from left to right on the screen. The electron beam leaves an image on the screen which represents the signal you've applied. Analog signals are continuously variable. See also 'Digital'.
- 'Auto-setup' mode: The oscilloscope automatically selects a setting for Volts/div and Time/div in such a way that one or more periods of signal are displayed correctly.
- Bandwidth: Usually expressed in MHz. It is the frequency at which an applied sine wave will be displayed at an amplitude of around 70% of its original amplitude. More expensive scopes feature a higher bandwidth. Rule of thumb: the bandwidth of an oscilloscope needs to be at least 5 times higher than the frequency of the signal applied to the input of the scope. The HPS140 bandwidth goes up to 10MHz.
- Clipping: When the 'top' or 'bottom' or both extremes of a signal are cut-off ('clipped'), e.g., because the signal cannot swing any further due to power supply limitations. An undesired property of amplifiers that are driven beyond their specs.
- DC coupling: The oscilloscope displays both the AC and the DC component of a signal.
- DC reference: DC measurement is always performed with respect to a ground level, so we need to define this ground level. If you do not set the DC reference, the readout might not be correct. In most cases, this ground level will be the center of the screen, however this is not mandatory.
- DC voltage: (DC: Direct Current) With DC, the current flows in a single direction; it does not reverse. A DC source has a polarity, (+) and (-).
- Digital: Digital scopes perform an analog to digital conversion on the incoming signal and handle all the calculations and displaying in the digital domain. Digital signals feature only two fixed levels, usually 0V and +5V. See also 'Analog'.
- Distortion: Undesired alteration of a signal due to external causes such as overloaded circuits, badly designed circuits, etc...
- Frequency (f): The number cycles of the AC waveform per second.
- Input coupling: The drawing shows a typical oscilloscope input circuit. There are 3 possible settings: AC-coupling, DC coupling, and GND. With AC-coupling, a capacitor is put in series with the input signal. This capacitor blocks any DC component of the signal and passes only AC. With DC coupling, the capacitor is bypassed, and both the AC and DC component of the signal are passed. Low frequency signals (<20Hz) should always be displayed using DC coupling. Should AC coupling be used, the internal coupling capacitor will interfere with the signal, and the displayed signal will not be correct.
- Noise: Undesired random addition to a signal.
- Period (T): Duration of one cycle of the AC waveform (= 1/f).
- Ripple: Unwanted periodic variation of a DC voltage.
- Sample rate: Usually expressed in samples or megasamples/second, sometimes in MHz. It is the number of times per second the digital oscilloscope 'looks' at the signal at the input. The more it 'looks', the better it is able to recreate a faithful image of the waveform on the screen. Theoretically, the sample rate needs to be twice the max. frequency of the applied signal; however, for best results, a sample rate of 5 times the max. frequency is recommended. The HPS140 samplerate is 40Ms/s or 40MHz.
- Sensitivity: Indicates the smallest change of the input signal that makes the trace move up or down on the screen. Usually expressed in mV. The HPS140 sensitivity is 0.1mV.
- Signal: Voltage applied to the input of the oscilloscope. The subject of your measurement.
- Sine wave: Mathematical function that represents a smooth repetitive oscillation. The waveform shown at the start of this glossary is a sine wave.
- Slope: It determines where the scope will trigger. This can be on the rising or on the falling slope of the signal.
- Spikes: Fast, short duration transients in a signal.
- Trace: 'Line' that is drawn on the screen, which represents the signal at the input.
- Vrms: The RMS voltage of an AC source represents the required DC voltage to generate the same amount of heat in a resistor as the AC source would do. For sinusoidal signals, Vrms = Vpeak / sqrt(2).
- Volts/div: Determines how many volts the signal at the input must swing for the trace to move one division.
- Waveforms: Patterns that repeat over time.
Circuit Diagram
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