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DPScope SE User Manual

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1. T Cursors f CH1 CH2 Levels Frequency Spectrum Setup Position Level Acquisition CH1 CH2 Trig h mh amp continuous single shot Ho Avg t T Log to file 4 Horizontal Vertical Trigger Mode I R it Oscilloscope 0 5 me div CH1 Vn Source F Auto CHI Ext F 20 kS asec Trig d i Datalogger ile 2 Widiv Polarity Fising 7 Falling 5 C a The left side of the display is mostly taken up by the waveform display To the right and on the bottom you can see that the controls are grouped in several functional blocks we will explain each of them in more detail later Mode Selects the main functionality oscilloscope datalogger or logic analyzer Display Determines how the acquired data is to be displayed Acquisition Main control of acquisition process Position Level Sets the voltage offset for each channel and the trigger threshold level Vertical Controls the input amplification attenuation for each of the two input channels Horizontal Controls the time base sampling speed and delay Trigger Defines the trigger source On the bottom there is a status line that displays the cursor information right now the cursors are turned off so it is empty which you can use to make measurements on the displayed waveforms e g to determine the signal amplitude or frequency On the top of the screen you find
2. DPScope SE After a few seconds the DPScope SE program should appear on the screen If the program cannot find and connect to the DPScope SE you will get a popup see below that you need to confirm in order to continue The software will still start after that but of course you will not be able to run the acquisition In this case close the software unplug the oscilloscope plug it in again you may want to try a different USB port if that does not help and launch the software again This problem is very unlikely to happen More likely is that you simply haven attached the scope to your computer DPScope SE Could not find any instrument attached to the computer Please make sure the unit is turned on and connected to the computer The DPScope SE should always be attached to a USB port directly at the computer or through a powered USB hub Unpowered USB hubs tend to have excessive supply voltage drop which needs to be compensated for and which will reduce the scopes maximum voltage range If in doubt you can check the actual USB supply voltage by selecting Utilities gt Check USB Supply The nominal value is 5V but in reality can be as low as 4 3V The minimum required screen resolution for the DPScope SE software is 800x600 pixels 3 The Main Screen After startup the screen should look as shown below File Utilities Help 4 Display n cH ga Oer M Lines 3 I bold mey S coe M O REF i Dots D Logic Channels Persist
3. not in datalogger mode or logic analyzer mode 6 1 5 Log to File This function is only available in datalogger mode It allows you to write all the captured samples directly into a file This way you can record signals of arbitrary time spans and with an arbitrary number of sample points no longer restricted to the DPScope SEG 200 points per channel record length 6 2 Display Display Moc See o er M Hnes bold if CH2 Bo El Dats E Persist Cursors f B Levels Frequency Spectrum Setup 6 2 1 CH1 CH2 Turns the display of scope channel 1 and 2 on or off respectively Note that this does not affect the signal capture itself meaning e g you can still trigger on CH1 even when it isn displayed 6 2 2 REF1 REF2 Turns the display of reference waveform 1 and 2 on or off respectively To copy the currently displayed waveform CH1 or CH2 respectively into the respective reference waveform you use the appropriate gt buttons Reference waveforms are very helpful e g to judge small signal changes by comparing the stored waveform to the displayed waveform Another important application is when you want to compare more that two signals one example would be an SPI bus consisting of clock data and chip select In this case you can first set up the DPScope SE so CH1 looks at the chip select and CH2 looks at the clock signal and it triggers on the falling edge of the chip select signal Capture both sign
4. 50 point mid level or falling edges if there aren two rising edges on the screen e Frequency 1 period e Duty cycle time spent above 50 during one period relative to the length of the period duty_cycle pos width period e Pos width time spent above 50 during one period e Neg width time spent below 50 during one period 6 9 2 DMM Display Measurement Update rate 2 per sec While the automated measurement panel is convenient sometimes you may want to observe only a specific value This could be e g to trim the frequency or the amplitude of an oscillator Chances are you do this at some distance from the screen so it is important that the display is large enough to be observable without being right in front of the computer This is the purpose for the DMM Display window DMM stands for Digital Multimeter because this mode has very similar functionality to such an instrument There you can select a single measurement out of all the measurements available in the main measurement panel on one channel which will then show up in very large digits The update rate lets you select how often the value will get updated if the acquisition rate is slow then of course the update rate will be slower than selected but it will never be faster This makes the numbers easier to read since they don jump around wildly 6 9 3 Check USB Supply Measures and displays the actual supply voltage from the USB port This enables
5. a quick check if the port voltage is close enough to its nominal value 5 Volts 1 the actual value can be as low as 4 3V 6 10 Help Menu 6 10 1 About Here you can find version and build of your software and of the scopeG firmware the latter only if there is actually a scope connected please always include this information when submitting bug reports or support requests The panel also shows the support contact info Version 1 0 2 Build 207 2 02 05 Scope Firmware Version nra C 2012 by Wolfgang Machen Email supportidpscope com Web http nwn dpscope com 7 Appendix Probe Calibration As long as you use simple cables or 1 1 probes you do not need to perform any compensation since the DPScope SE is compensated for them by design This is different with 1 10 probes some adjustment may be necessary to obtain correct waveform display and maximum bandwidth To perform this compensation connect the probe to the DPScope SE and hook it up to a square wave signal frequency about 1 KHz This could e g be a function generator set to produce a square wave or a pin on a microcontroller that gets toggled 2000 times per second Make sure the scope probe is set to 1 10 attenuation not 1 1 Display the signal on the screen Trigger turned on so the waveform is stable Adjust the vertical scaling and offset so the signal spans about half the display height Adjust the timebase soyou see roughly two periods of the calibrat
6. a single channel Then it waits for the next trigger and captures a second sample on this channel and so on For each sample it waits for a slightly longer time after the trigger this delay can be controlled in increments much finer down to 500ns or half a us than the smallest real time sample interval 20 us That way assuming the waveform is repetitive with respect to the trigger the sample points of subsequent acquisitions will lie in regular intervals along the repetitive waveform Plotting them together suitable shifted by the respective added delay versus the trigger produces a picture of the signal with finer resolution than possible with real time sampling The DPScope SE acquires first CH1 in this fashion then CH2 then CH1 again and so on The main advantage is that you can resolve the signal in much finer increments up to 2 MSamples sec or equivalent time sample intervals of just 500 nanoseconds than possible with real time sampling There are a number of tradeoffs connected with equivalent time sampling First there is lower acquisition speed because the DPScope SE only acquires one sample per trigger event instead of a full record like in real time sampling especially noticeable at slower timebase settings and slower trigger rates Second there is the necessity that the signals be repetitive with respect to the trigger Thirdly you always need to have a trigger source with fixed timing relationship to the signal to be meas
7. appropriate channel See picture below tek DP Scope SE File Utilities Help Display CHT pee o aer Lines i bold lw CH2 3 E FEF B ters 5 Persist ss gt Cursors ff g r Levels a Frequency Spectrum Setup Position Level Acquisition CH1 CH2 Trig Stop Clear Ho Hm E f continuous f single shat No Avg Horizontal Vertical Trigger Mode ca f Oscilloscope 0 5 mevdiv cH Sovran Source of Auto f CHI f Ext F 20 k5arsec DS m Trig d 2 T CH 2 di Polarity Fising C Falling 6 8 File Menu 6 8 1 Load Setup Recalls a previously saved setup all settings like acquisition mode vertical scales time scale trigger setup etc from a file 6 8 2 Save Setup As Saves the current setup i e all settings like acquisition mode vertical scales time scale trigger setup etc to a file 6 8 3 Export Data Exports the currently displayed waveforms to a text file File format is standard CSV comma separated values format which you can open and process in Microsoft Excel or any standard text editor e g Notepad e In oscilloscope mode the file contains both scope waveforms CH1 and CH2 as well as both reference waveforms REF1 and REF2 e In Logic Analyzer mode the file contains the four digital logic channels e In datalogger mode the file contains the two analog oscilloscope channels as well as the four digital logic chan
8. div CH2 2 Vrdiv E 6 6 3 Trig d This indicator ririggeredd shows if the scope is getting trigger events Each trigger will cause it to turn green for a short amount of time If it stays green that means the scope is getting triggered at a fast rate This can be helpful e g when the signal has very little noise so it is hard to tell if the acquisition is stuck Trig is grey or if the scope is actually constantly acquiring new data but each acquisition simply looks the same as the previous one 6 6 4 Noise Reject In scope mode if there is noise on the signal and there is always some amount this can cause false triggering E g if triggering on a rising edge the signal may actually be falling at a given instant but a short little positive noise spike right when the signal has crossed the trigger threshold from above will look like a rising edge to the comparator and cause a trigger even though it is not a true positive going edge As a result the oscilloscope will effectively trigger on a falling edge instead of a rising edge To avoid this situation the DPScope SE automatically performs Noise Rejectoby requiring that the signal must remain above the threshold in the case of a rising edge trigger below for falling edge for at least one sample interval 1 10 of a division i e 5 samples If it fails to do so e g because the edge really was just a short noise spike as discussed above the trigger event will get
9. e g use a different sampling mode change the trigger polarity etc When you expect to measure the same signal again later you may want to save the complete setup to a file File gt Save Setup that can be loaded back later That way you do not have to repeat the full setup procedure over and over 5 3 Undersampling Aliasing One very common trap that many beginners but not only they fall into with digital sampling oscilloscopes is so called aliasing This effect can happen whenever the sample rate is too slow compared to the signal frequency To pick a simple example assume you have a 1 kHz sine wave that you sample with a 1kSample sec sample rate In this case each acquisition will hit the same point in the signal period just one period later each time so the displayed waveform on the screen will be a flat horizontal line i e look like DC rather than a sine wave clearly wrong If the signal frequency is a steady 1 01 kHz and the sample rate is 1 kHz each sample will be 1 100 of a period offset on the and the resulting displayed waveform will be a very convincingly looking 10 Hz sine wave this can be very misleading Incidentally this is in fact a variation of the equivalent time sampling process it is called fecoherent undersamplingoand is widely used whenever one can get sufficient sample rate to sample incoming high speed signals in real time The solution is of course to sample the waveform with a sufficiently high sa
10. shot or repetitive capture That said the most common usage of a logic analyzer is in triggered single shot mode i e set up a trigger wait for the trigger event to happen capture one full record on all channels then stop and analyze the data lt F F OT LSS SS I pZ DPScope SE o w i a A o l ati File Utilities Help Display CH1 IEE W Lines E CI mas T bold Che E REFe Dots jw Logic ee Bl see Cursors f CH1 CH2 Leve Frequency Spectrum setup PositionfLevel Acquisition CH1 CH2 Trig j HH al al Clear f continuous f single shat No Avg Log to file Horizontal Vertical Logic Trigger Mode 10 mediv 1 kS asec Oscilloscope CH1 Hia vedie Source C Auto 1 T2C3C 4 l C Datalogger Trig d Se l f Lagic ao a o u CH2 e Polarity amp Fising Falling 5 2 Probe Vertical Gain Setup and Trigger Setup When you want to acquire a new unknown signal it is best to maximize you chances of seeing something before fine tuning your settings Choose the widest voltage range available 1 V div and set the channel offset to the center of the screen That way your visible range spans from 10V to 10V which will capture most signals you encounter For larger signal use a 1 10 probe to widen the range even further Whenever you use a new 1 10 probe first perform a probe calibration described in the DP
11. words a 110V AC signal oscillates between 156V and 156V while 220V AC ranges from 311V and 311V The latter will thus exceed the DPScope SEG input range even with a 1 10 probe There are 1 50 and 1 100 probes available that would allow to measure such signals Note The DPScope is intended for measurements on low voltages only and we explicitly decline any responsibility for damage or injury resulting from work with high voltages that is any voltage exceeding 25V peak you do this at your own risk Should you choose to perform such measurements you confirm that you have the necessary knowledge to do so and will always observe the required safety precautions 6 5 Horizontal Horizontal 10 us div 1 MSasec o E 6 5 1 Sample Rate Determines the sample rate i e how many times per second the signals are measured The available range is dependent on the acquisition mode e Normal Mode 1 sec div to 0 5 msec div 10 Sa sec to 20 kSa sec interleaved 0 2 msec div 50 kSa sec CH1 and CH2 alternating Equivalent Time Sampling Mode 0 1 msec div to 5 usec div 100 kSa sec to 2 MSa sec Frequency spectrum 0 5 Hz div to 1 kHz div 10 Sa sec to 50 kSa sec Datalogger Mode 0 5 sec div to 1 hr div Logic Analyzer Mode 1 sec div to 10 usec div 10 Sa sec to 1 MSa sec 6 5 2 Horizontal Position This slider is only active in Logic Analyzer mode because the full record 850 samples per channel is longer than what fit
12. DPScope SE User Manual Version 1 0 0 Feb 8 2012 1 Introduction The DPScope SE is a low cost microcontroller based digital oscilloscope intended for hobby and educational use If you are new to oscilloscopes we recommend the following introductory application notes created by Tektronix one of the major oscilloscope manufacturers for the professional high end market which will supply all the knowledge necessary to understand this user manual and get the most from your DPScope SE The XYZs of Oscilloscopes The ABCs of Probes You can download both documents either from the Tektronix website htip Awww tektronix com or from the DPScope SE website http www dpscope com gt DPScope SE gt Downloads lf after reading through the documentation you still have questions regarding the DPScope SE or want to provide feedback or suggestions for improvement do not hesitate to contact us atF support dpscope com 2 Software Startup After you installed the DPScope SE software see the assembly guide for details plug in you DPScope SE and wait a short time so the computer has a chance to recognize the scope The DPScope SEG power LED on the front panel should blink quickly a few times and then stay solidly on 1 this is the sign that the scope has successfully powered up The DPScope SE does not neet any special drivers since it uses the standard USB HID driver that comes with Windows Then launch the PC software Start gt DPScope SE gt
13. If set to fExt othen the scope triggers on the signal fed into the external trigger input pin labeled ATO for the trigger signal and rGofor ground The trigger threshold here is fixed at around 1 5V good for TTL 5V CMOS 3 3V CMOS and 2 5V CMOS In logic analyzer mode you can either force constant acquisition fAutod or trigger on any of the four digital input channels 1 2 3 or 4 www DPScope cor 2a 6 6 2 Rising Falling The trigger polarity further specifies the required trigger condition FRisingOmeans the signal must cross the threshold from below and rise above the threshold i e a positive slope to cause a trigger fFallingomeans the signal must cross the threshold from above i e a negative slope The pictures below show this in more detail Note that because of the noise reject feature see below you will not see the actual trigger instant because the acquisition of the sample data only starts a short moment after detection of the trigger In logic analyzer mode frisingomeans a transition from 0 logic low to 1 logic high and alling is the opposite transition from 1 to 0 One could conceptionally think of the threshold as being at 0 5 of course there is no such digital value it DP Scope SE ft DPScope SE File Utilities Help File Utilities Help Trigger Trigger SOUE e f Ext Source f Auto CHI C Ext Trig d Polarity Rising C Falling O Polarity Rising CH2 2
14. Position Level Acquisition CH1 CH2 Trig j HH g al al al Clear io a No Avg Log to file Horizontal vertical Trigger Mode _ w La a 3 o C Oscilloscope 05 s div J cH Jovraiv Source 0 20 Samples zec _ f Datalogger SS oe gg A al gt CH2 H2 div Polarity 9 E E E A 5 1 4 Logic Analyzer Mode Many signals you encounter are digital in nature i e they are either high or low This can greatly simplify acquisition if you are only interested in the logic state not the exact analog waveform or levels the instrument can measure signals with a comparator instead of a full blown analog to digital converter and for each sampling instant only store one bit of information per channel It can do this much faster up to 1 MSa sec real time sampling rate for the DPScope SE and store more sample on more channels up to 850 samples on 4 channels than in scope or datalogger mode Input in this mode is through the logic analyzer connector on the back of the instrument The input channels are labeled rq R and FAQ respectively You also need to connect ground labeled A to the ground of your circuit under test www DPScop cormn Otherwise this mode is very similar to the normal real time scope mode You can trigger on each of the four channels either on a rising or a falling edge or have the acquisition in free running mode and either single
15. Scope SE Assembly Guide 1 1 probes should not need any calibration because the DPScope SEG input is compensated for them by design Set the time scale to 0 5ms div 20 kSa sec so you are in real time sampling mode and triggering is not mandatory It is usually best to set the trigger to FAuUtoOmode otherwise youd have to hunt for a valid trigger level on the invisible waveform before the scope displays anything The waveform timing will not be stable that way but will move randomly in time but you will be able to see which voltage range the signal spans Using the fPersistenceddisplay mode can sometimes be helpful if looking at rare spikes where the signal amplitude is difficult to judge otherwise Once you know the range you can adjust vertical gain and offset to center the signal vertically and make it fill a good portion at least a quarter of the vertical display range To set up the trigger move it to the center of the trigger channel signal band i e the green triangle on the left should be somewhere between maximum and minimum level of the signal on CH1 and turn the trigger on Switching on the fLevelsodisplay can be helpful there as well If you are using the external trigger which is fed in through the connector on the back of the instrument pins Arofor the trigger signal and rGofor ground then the trigger level is fixed at around 1 5V good for TTL 5V CMOS 3 3V CMOS and 2 5V CMOS Now you can fine tune your setup
16. als with single shot mode and save CH2 to REF2 Now connect CH2 to the data line instead and repeat the capture You now have all three signals clock data chip select on the screen at the same time Note that if the signals are digital in nature it may be easier to use logic analyzer mode instead where you can capture up to 4 signals concurrently 6 2 3 Lines Checking this option will cause the scope to connect the captured data points with lines This makes the actual waveform much easier to see especially when there are fast changes which would make subsequent points fall on places far away on the screen Check the fBoldOcheckbox to make the lines wider e g to be able to see them at a distance 6 2 4 Dots Checking this option will cause the scope to indicate the actual sample points with small circles This can be very useful if you want to check if your sample rate is truly high enough for an accurate waveform display Either lines or dots or both must be turned on as unchecking both with result in an empty display which could be confusing to the user thus the DPScope SE enforces this automatically 6 2 5 Persist Normally the screen is cleared whenever the scope has a new acquisition is to display Checking this option will make the scope keep all waveforms on the screen until you either press rStopdand then rStart Nagain or until you press rCleard This allows you to see over which range the waveform is changing importan
17. d small periodic components e g periodic noise from the power line hidden in the main signal it is much easier to see an isolated 60 Hz component spectral line in a frequency plot than it is to see it among all the random noise riding on the signal Note that in frequency spectrum mode the scope alternates the signal capture between channels i e only captures one channel at a time It does that so it can acquire a longer data record 410 points which results in finer frequency resolution You can still freely choose which channel CH1 or externale trigger input to trigger on i e also trigger on a channel when it is not displayed It is usually easiest to first set up the waveforms in normal time domain mode and only then change to frequency spectrum mode Also in most cases frequency spectrum mode works fine in rautoo trigger mode as long as the waveform is periodic and with sample rates low enough so a few signal periods are displayed on the screen However make sure that your sample rate is at least 3 4 times your signal period otherwise aliasing will occur resulting in erroneous frequency domain pictures You can use the cursors to make measurements of frequency and relative power Note that the sample rate box changes to frequency units Hz and kHz Pressing the rSetupobutton brings up a small panel where you can modify the settings used for the conversion Linear V vs logarithmic dB scaling voltage vs power an
18. d the filter type to use The filters reduce artifacts caused by the finite length of the data set The available types from top to bottom none Hamming Hanning and Blackman result in increasingly accurate amplitudes for the price of increased spectral line width At the moment frequency spectrum mode is only available in real time sampling mode i e for sample rates up to 50 kSa sec well sufficient for audio range the sample rate must be more than twice the highest frequency of interest 1 traditionally 20 KHz for audio File Utilities Help Display m cH gg o er M Ones bold cHe M O RE o Dots a Persist Cursors J Levels pm e E N A x Fe Frequency Spectrum Setup ee Position Level Acquisition CHI CH2 Trig Stop H E sl al al al Clear f continuous f single shat No Avg m Horizontal n Vertical Trigger Mode X Oscilloscope 1 kH2div J cH a Source of Auto i CH1 een _ 50kSa sec ns T i a gt CH 2 div Polarity Rising C Falling Trig d 6 3 Mode Hode f Oscilloscope f Datalogger f Logic Analyzer 6 3 1 Oscilloscope Datalogger Logic Analyzer In oscilloscope mode the DPScope SE will always acquire a full data set 200 points per channel and store it in its internal memory before transmitting it to the computer for display This enables very fast sample rates up to 50 kSa sec real time and 2 MSamp
19. ed in V div Volts per division or mV div Millivolts per division so e g at 2V div each vertical unit interval between two horizontal dashed grid lines corresponds to 2 Volts 6 4 2 Probe Attenuation The probe attenuation settings 106checkboxes do not have any bearing on the actual amplifier setup but rather tells the scope software how it must scale the measured data on the screen A 1 10 probe reduces the signal by a factor of 10 which allows you to measure much larger signals than would be possible with a 1 1 probe The option to use 1 10 probes is only available in the upper range settings 0 5 1 and 2 V div in the lower ranges they would not make sense anyway since you could simply use a 1 1 probe and change the gain setting accordingly Important Warning While the scope can display signals between 240V and 240V with a 1 10 probe which reduces these signals to a range between 24 and 24V you must exercise extreme caution when working with such large signals e As arule of thumb anything that exceeds 20V is potentially dangerous If you accidentally touch the source you can seriously hurt yourself or even die e To avoid damage to yourself the DPScope SE or your computer always verify that the probe is truly set to 1 10 mode before contacting the circuit e Note that AC voltages e g line voltage have peak values that exceed the rated effective RMS voltage value by a factor of sqrt 2 or about 40 In other
20. form display is somewhere in the middle of the CH1 waveform the red waveform That waveform should now be stable assuming you waveform is periodic Try switching between rising and falling edge trigger Now change the sample rate in the Horizontal control display and see how the waveform changes itd like Zooming in and out on the waveform timing In the Display control box turn the waveforms on and of by clicking on the appropriate checkbox you can still trigger on a waveform even when it is not displayed Change the display style to points and or infinite persistence Congratulations you have just measured your first signal with the DPScope SE 5 General Remarks The DPScope SE is a digital storage oscilloscope refer to the XYZs of Oscilloscopeomentioned in the introduction if you are unsure what that is based on a Microchip PIC18F14K50 microcontroller Most of the oscilloscope functionality is actually integrated in this single chip analog to digital converters sample logic trigger logic and threshold generation memory logic analyzer USB interface Only the analog frontend input amplifier attenuator consists of external components 5 1 Acquisition Modes The DPScope SEG acquisition engine has four different modes again refer to the XYZ of Oscilloscopesodocument for further details 5 1 1 Normal Mode Acquisition is started by a trigger event or automatically right after the previous acquisition if the trigger m
21. ged signal 6 1 3 Continuous Single Shot Selects whether the DPScope SE shall continuously acquire new waveforms or only acquire once and then stop Continuous acquisition is useful for repetitive waveforms when you want to have a real timedimage of the signal and to see if or how the signal changes over time Single shot capture is useful e g for event that happen only once e g a sudden pulse or when you want a steady picture to take measurements on 6 1 4 Averaging Selects how many waveforms to average over 1 2 5 10 20 50 or 100 Averaging reduces random noise on the waveform resulting in a much cleaner picture that allows you to see small details that may otherwise be hidden under the noise For averaging to make sense you need to have a basically Stable repetitive waveform so you will need to turn the trigger on i e auto mode wond work because the sample timing would be asynchronous to the signal period Note that the averaging process used is not a simple arithmetic average over the given number of samples instead it uses exponential weighing i e earlier acquisitions have less weight than the more recent ones This is the digital equivalent to an analog R C low pass filter but unlike a filter in your signal path it will not degrade your signal bandwidth or rise time it will just filter out fast changes from one capture to the next but not fast changes along the waveform Averaging is only available in scope mode
22. he end of the previous acquisition happens so you may wait close to a second before the screen refreshes just once In this case it is usually better to display the sampled data as it comes in This is what the Datalogger mode often also called Roll Mode is for The scope acquires the signals continuously and plots the samples on the screen right away The waveform scrolls to the left and the new points get added to the right similar to how a classic datalogger would draw curves on a moving band of paper from a roll that where the Roll Mode has its name from There is no trigger available in this mode since we do not want to wait for a trigger event anyway But you can log the captured data into a text file on your hard drive so unlike the other three modes you can capture data sets of arbitrary length only limited by the free space on your hard drive Clearly this mode only makes sense for relatively slowly varying signals so the sample rate is limited to 20 samples per second timebase 0 5 sec div or slower Since sampling speed is slow and the scope can transmit the data as It comes in i e does not have to store full records in its small internal memory you can not only measure and display the analog signals on the scope inputs but also the four digital logic analyzer inputs at the same time Display m cH ggg o er M bres i bold M cH2 B RE pas _ f W Logic Channels S gt a A Cursors f amp i Levels F Eo
23. ion signal On the probe there is typically a small screw either at the probe head itself or at a small block at the connector end that you use to adjust the probe compensation Since this is a trimmer capacitor you should use a non metal plastic or wood screwdriver to adjust it a piece of metal can detune the setting when it is close which would make it hard to adjust accurately Refer to the picture below as to how the waveform shall look like after calibration wrong overcompensated correct wrong undercompensated
24. le sec in equivalent time because there is no limitation from the transmission speed between scope and computer The downside is that the record length is limited to about 200 points per channels and for very slow sample rates the time between subsequent transfers becomes larger because it takes a while to capture 200 points at a slow rate Datalogger roll mode on the other hand is limited to relatively slow sample rates 20 samples sec maximum which corresponds to 0 5 sec div but you can have the DPScope SE the captured data directly into a text file and thus have virtually unlimited storage It also allows to log the four digital channels together with the two scope channels In Logic Analyzer mode you can capture the digital states on four channels connected to the logic analyzer header at the back side of the instrument with sample rates up to 1 MSa sec Other than that it works very similar to oscilloscope mode You can change modes only when the acquisition is stopped 6 4 Vertical Vertical CH1 2 div CH2 2 Vediv 6 4 1 Scale The vertical gain boxes set the input amplifier gain so you can look at very small Millivolts as well as quite large several Volts signals The maximum signal range in the 2V div setting that can be displayed is from 24V to 24V Never apply signals exceeding this range to the scope input doing so risks damage to the DPScope SE as well as to your computer The scaling is display
25. mple rate So if in doubt change the sample rate and see if the waveform behaves mormallyo e g when doubling the sample rate the displayed frequency of the signal should not change And as a general guideline when working with an unknown signal always start looking at it with maximum sample rate and only then change it to something slower 6 Description of User Controls 6 1 Acquisition Acquisition Pn Clear f continuous f single shot No Avg 6 1 1 Run Stop Starts and stops the acquisition process data is captured if trigger event occurs and displayed on the screen If frcontinuousdis selected the acquisition will repeat until you press the button labeld fStopowhile acquisition is in progress is pressed In case of single shotoacquisition the scope acquires and displays only one record and then stops if fNo Avg no averaging is selected otherwise it will acquire the given number of records to average over and then stop This means that if you want to do a true single shot capture you need to set the averaging to ANo Avga In datalogger roll mode single shot and averaging is not available in this case this button simply starts and stops the continuous acquisition 6 1 2 Clear Clears deletes the currently stored traces One typical use is when averaging is selected and the measured waveform has changed as this clears out the old information so the waveform only consists of an average of the new chan
26. nels e In datalogger roll mode it is usually more useful to select Log to filedinstead because this will write all the data to the file while Export Datadonly writes the latest screen interval 6 8 4 Exit Closes the DPScope SE application 6 9 Utilities Menu 6 9 1 Measurements While it is possible to make measurements on the waveforms using the cursors the DPScope SE also offers a faster and much more convenient method Fully automated measurements Selecting Utilities gt Measurements brings up the Measurement panel Here you can select on which channel s CH1 and or CH2 the software shall take the measurements and also which measurements to take The values get updated after every acquisition If you have already acquired the signal and only afterwards bring up the Measurements panel simply press Update Valuesoto perform the calculation based on the currently displayed waveforms Do not change vertical or horizontal settings like gain or offset between the acquisition and the calculation The following measurements are available Level low high midlevel DC mean amplitude and AC RMS Timing rise time fall time period frequency duty cycle positive width negative width You can turn the waveform annotations on and off for each channel If turned on and the channel is displayed they will show the low mid and high level that the software uses This can be a valuable tool to troubleshoot your results p
27. ode is fAutod and samples digitizes the signal in real time This is very similar to how a classic analog oscilloscope operates Real time acquisition means the acquisition is very fast up to approx 20 records per second on a sufficiently fast computer and you can capture single shot events Note that the acquisition rate will decrease for slow sample rates slower than about 5 kSamples sec or 2 ms div because it takes some time to simply capture each full record if only a few samples are taken per second Also since this mode uses an interrupt generated by the internal hardware comparator the timing is very tight i e reaction to the trigger event is almost instantaneous resulting in very low jitter against the trigger in practice that means there is very little horizontal timing rwiggledof the displayed waveform This mode has two limitations First the maximum sample rate is 20 kSa sec 20000 samples per second if acquiring both channels because the controller has to digitize and store the data as fast as it comes in The main limitation here is the speed of the built in analog to digital converter it can go up to about 50 kSa sec and is shared between the two scope channels For up to 20 kSa sec on two channels the acquisition is interleaved i e the scope acquires one sample on CH1 then one on CH2 then one on CH1 again and so on at 40 kSa sec so each channel gets digitized at 20 kSa sec At 50 kSa sec the acquisition is pe
28. rc Waveform Measurements _ Level iv V CH 7 Low 7 High 7 Mid 7 DCMean wW Amplitude 9 80 9 80 W AC RMS 3 39 W 3 40 Time Rise Time Fall Time Pernod Frequency Duty Cycle Pos Width Neg idth 4 J m p 4 z J m a Select All Important notes wa T T E E i cu T lt cu i uw e In order for the timing measurements to work at least one full signal period needs to be displayed on the screen e The time measurements employ linear interpolation between the actual samples to improve resolution and accuracy of the results e Averaging can significantly improve the accuracy especially for the level measurements e Measurements slow down the acquisition process somewhat Turn them off close the measurement panel for maximum screen update rate Short description of each measurement Low lowest value minimum on the screen High highest value on the screen Mid Midpoint between low and high mid low high 2 DC mean average voltage level calculated over all points on the screen Amplitude difference between high and low amplitude high low AC RMS RMS value calculated with the mid level taken as the reference Rise time time to rise from 10 to 90 of the swing low 0 high 100 e Fall time time to fall from 90 to 10 of the swing low 0 high 100 e Period time between subsequent rising edges crossings of the
29. rformed as in an alternating fashion i e after the first trigger only CH1 is captured full record 200 points at 50 kSa sec then at the second trigger event CH2 is digitized again full record Second since the trigger initiates the capture process you can only look at things that happen after the trigger unless you can supply a suitable pre trigger signal to CH1 or external trigger that precedes the signal to be captured on CH1 or CH2 by some margin ba DPScope SE File Utilities Help Display m cH ggg m Reri M bres bold lw CH2 DERS Dots a Persist Cursors tf E Levels Frequency Spectrum Setup Position Level Acquisition CHI CH2 Trig Stop H E sl al al al Clear f continuous f single shat No Avg Horizontal Yertical Trigger Mode a Le i Le r f Oscilloscope 05 m div J cH Jovraiv source f Auto cf CHI i Ext HES 20 kSa sec I T E T Trig d gt CH2 H1 div Polarity Rising Falling oO E E a 5 1 2 Equivalent Time Sampling Mode This mode works similar to Normal Mode in the sense that the acquisition is initiated by the trigger event so again you can only look at things that happen some time after the trigger But other than Normal Mode in Equivalent Time Sampling Mode the scope makes no attempt to sample the signals in a single sweep Instead it waits a defined time after the trigger event and then just captures a single sample on
30. s conveniently on the screen 200 samples 6 6 Trigger Logic Trigger Oscilloscope mode Logic Analyzer mode Trigger Logic Trigger Source f Auto f CH1 Ext source f Auto 1 f 2 3 4 Polari fe Fis Falli ro bee olan ot Fising alling C Polarity Ri mg C Falling C This panel changes somewhat between oscilloscope mode and logic analyzer mode to account for the difference in available trigger sources 6 6 1 Auto CH1 Ext and Auto 1 2 3 4 The Auto CH1 Ext radio buttons let you select what the DPScope SE shall trigger on A trigger is basically a condition that determines when the oscilloscope starts the data acquisition For a repetitive signal you use this to obtain a steady picture of the signals For a one time signal it allows you to have the scope wait until the event of interest occurs before it starts to capture the signals If set to Muto the DPScope SE will be free running constantly collecting data and not wait for any special event before capturing data This is useful when you want to look at an unknown signal because you will always see something on the screen the scope will not wait and not display anything just because some trigger condition is not fulfilled If set to FCH1 Othe scope will use the signal on scope CH1 as the input to its trigger circuitry In this case you can use the trigger threshold slider see explanation of the Position Levelsoframe to determine the trigger threshold level
31. suppressed and the DPScope SE will keep waiting for a trigger Note that the absolute duration required depends on the sample rate time base setting This makes sense since at slow sample rates on usually isn interested in changes and doesn want to trigger on things that are too short to observe anyway This feature is especially valuable for slowly varying signals Note however that if your signal period becomes too short the noise reject feature may prevent the DPScope SE from triggering at all In this case increase the sample rate so the period becomes a larger fraction of the screen width For fast sample rates the minimum duration Is actually a bit longer than one sample interval because the processing overhead is no longer negligible 6 7 Levels PositionfLevel CH1 CH2 Trig HH ETETE 6 7 1 CH1 CH2 Channel Positions Sets the channel offset for input channel 1 and 2 respectively This lets you control where ground zero Volts is displayed on the vertical axis First this expands the available voltage range for a given vertical resolution e g at 0 1 V div you could for example cover the range fro OV to 1 2V 12 vertical divisions are visible or alternatively from 1 2V to OV A second use for the offset is to move the two waveforms CH1 and CH2 apart on the screen so they are easier to discern even though in reality they cover similar voltage ranges e g 0 to 5V The zero position for each channel is indica
32. t cases are measurement of peak to peak noise or timing jitter This is also a great tool to capture rare glitches sudden waveform aberrations that you may miss otherwise because without persist mode they may disappear from the screen again so quickly that you cand see them When persist mode is turned on however even a single such event with remain easily visible Finally this mode is useful to generate so called eye diagramsoof digital data streams 6 2 6 Levels Turns level markers on and off while the levels CH1 and CH2 offsets and the trigger threshold are also indicated with colored triangle markers on the left edge of the waveform display sometimes it is helpful to have rulers across the whole screen 6 2 7 Cursors CH1 CH2 Turns the measurement cursors on and off respectively and selects which channel CH1 or CH2 they refer to The cursors are the solid horizontal and vertical lines in the waveform display which appear whenever you check the rCursorsoOcheckbox You can move them with the slider bars on top bottom and left right of the waveform display There current level and time positions as well as the difference in their positions are shown in the status line on the bottom of the scope window Cursors dY 11 609 WY 5 456 Y 6 151 Y dt 3 572 ms T1 dt 280 0 Hz gt Because the voltage scales can be different between CH1 and CH2 you need to select which of these two waveforms the cursors shall refer to The
33. ted on the left side of the waveform display with a colored marker red for CH1 blue for CH2 If Levels is turned on in the display control frame two dashed horizontal lines of same colors are drawn across the display as well at that vertical position See picture below To reset the zero position back to the middle of the display press the respective rkObutton 6 7 2 Trig Trigger Level This slider controls the trigger threshold If the DPScope SE is set up to trigger on CH1 a trigger event will occur whenever the signal crosses this threshold with the desired polarity rising or falling edge respectively If the trigger source is the external trigger input then this slider is not active because the threshold on the external trigger input is fixed at about 1 5V Same if the trigger mode is rAutoosince in this case the DPScope SE does not wait for a trigger event at all The zero position is indicated on the left side of the waveform display with a green marker If fLevelso is turned on in the display control frame a green dashed horizontal line is drawn across the display as well at that vertical position Usually the best approach with an unknown signal is to first display it with trigger in FAutoOmode That way although the waveform on the screen will not be stable you can at least judge the voltage range that the signal spans and set the trigger level marker somewhere within that range before setting the trigger source to the
34. the menu containing three entries File to save the displayed waveforms in numerical format and to save and restore the DPScope SEG software settings Utilities measurements DMM display and supply voltage check and Help displays general info about the software 4 First Acquisition After startup the software is set up in a way to maximize you chance to see something useful on the screen right away Both scope channels are turned on the voltage range for both is set to maximum ground levels centered on the screen continuous mode and trigger in Auto mode meaning the acquisition will run without waiting for a trigger event and so on Attach the probes to some signal source e g the toggling output of a microcontroller Press the FRuno button its caption will change to r8topd You should see a waveform on the screen Since the trigger mode is Muto most likely the waveform will not be stable but rather jump around Now play around a bit with some of the controls Don be afraid You can break the scope no matter what settings you change The worst that can happen is that you no longer acquire a waveform and or see it on the screen If you get completely stuck simply close down the DPScope SE program and start it again Move the offset sliders and see how the waveforms follow Now select fCH1 odin the trigger control menu Move the trigger level slider so the trigger level indicated by a green triangle on the left border of the wave
35. time scale is the same for both so this selection has no bearing on timing measurements i e on the vertical cursors With the cursors you can perform many different measurements on the displayed waveforms for example Levels amplitude high and low level average level overshoot and undershoot Timing period frequency delay phase rise and fall time Note that the DPScope SE also offers a set of fully automated measurements You can access them through Utilities gt Measurements peck DP Scope SE File Utilities Help 4 Horizontal 0 5 mosdiv 20 kS asec Vertical CH1 2 div r CH2 2 div Cursors dY 18 511 Y 9 242 Y 9 269 Vv w logarithmic Display f Voltage f Power f None fe Hamming C Hanning C Blackman Display m cH Bj m Reri M bres bold che M O REF pa ig a Dae Persist ar CH1 WO CH2 I Levels N A a a Frequency Spectrum Setup Position Level Acquisition CHI CH2 Trig Stop H E al al al Clear f continuous f single shat No Avg Mode ORERE f Oscilloscope m Trig d 2 Checking the Frequency Spectrum option will change the display to frequency domain The oscilloscope performs a real time FFT Fast Fourier Transform on each captured record which shows the frequency components contained in the acquired signals This is a highly useful mode to analyze periodic signals or to fin
36. ured in order to get usable waveforms otherwise subsequent partial captures will be unrelated timing wise and the composite waveform on the screen will look like random noise rather than the waveform you expect Also it is obvious that you cand make single shot acquisitions in this mode the software allows single shot mode but here it means that one full waveform consisting of many single sample captures gets acquired and then the acquisition stops Still given the high acquisition speed of the DPScope SE and the fact that most signals one encounters are repetitive anyway or can be made repetitive means these restrictions are far less serious than you might think it DPScope SE File Utilities Help Display m cH ggg o er M bres bold m cH MM O REF pa ia Persist Cursors gt Levels Frequency Spectrum Setup Position Level Acquisition CH1 CH2 Trig Stop H EE E al al al Clear f continuous f single shat No Avg Vertical Trigger Mode eed oR Source f i CHI O Est i Oscilloscope A wo ee r m B Trig d J H H Aje 4 CH1 2 div r gt CH 1 div k Polarity Rising Falling 5 1 3 Datalogger Roll Mode For very slowly varying signals it takes a long time before a full record has been acquired E g at 1 sec div timebase each acquisition 20 horizontal divisions takes 20 seconds plus the time it takes before the first trigger event after t

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