Dpo3014 programming manual

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From simple websites to large scale e-commerce portals, our web developers excel at creating highly efficient websites. These are just a few of the many ways our web development company stands out from the competition. The following users thanked this post: dzseki. I cannot get these to work and my IDA skills are too bad to figure out what is happening. As I said in the other thread, there should also be a debug console avalible that is accessible through TCPIP but I cannot figure out how to connect to it Jwalling Supporter Posts: Country: This is work?

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JPG The ideal way would be to find out how the key is generated for the Mhz upgrade, because the scope's firmware definitely knows what to do when upgrading Maybe some similar routines as for the MDO?? Marchello Contributor Posts: 26 Country:. Is it possible to hack MSO? Worked fine, and bandwidth did improve, although it doesnt seem to meet the risetime spec. Chapter 3 Methodology This chapter describes how the project was carried out, focusing especially on the process that was used to obtain measurements.

An empirical approach was used to characterize the channel. The methodology was based on making measurements of the channel in various scenarios, and using the collected data to represent the channel as a two-port network via Z-parameters. In order to calculate Z-parameters, the magnitude and phase of voltages and currents on either coil are needed.

To collect the necessary data, a custom measurement setup based on an oscilloscope was arranged, which was controlled by a PC running Matlab scripts. An LCR meter can measure the self inductances and mutual inductance of the system, as well as the resistances of either coils, but there does not seem to be a straightforward way to measure the mutual resistance, meaning that the real part of Z12 and Z21 are not captured with this method.

Using an oscilloscope with measurement probes allows for currents and voltages to be measured directly over the transmitting and receiving coils, enabling the calculation of Z-parameters directly from these quantities. In order for inductive power transfer to occur, a time varying current needs to be delivered to the primary coil. A sinusoidal signal is generated by a function generator and fed to a PA.

The PA is connected in series to the primary transmitting coil and the resonance capacitor. On the receiving side, the secondary receiving coil is connected in series to a resonance capacitor. The current is measured using a current measurement board, which leads the current to a connected resistive load. Figure 3. As the function generator is unable to generate large power outputs, a PA was needed.

The function generator can be controlled from a PC, allowing for the input to be changed dynamically during measurements. The PA has a power output limit of 90 VA and a voltage input limit of 4 V peak-to-peak, making the maximum voltage output 40 V peak-to-peak. At high frequencies and power levels the PA distorts the signal, as described in Figure 3.

This distortion becomes very apparent when the output voltage is close to 40 V and high frequencies are used. Simultaneous capture allows for phase shifts between each pair of the quantities to be recorded. An oscilloscope with four analog input ports was chosen to do the measurements. Calibration was performed in order for the analog inputs to be scaled correctly. The calibration was done by measuring the voltage and current over a known resistance with a known voltage input and making sure the measured values match the expected ones by adjusting the scaling for each probe on the oscilloscope.

As data was analyzed, it was found that the real part of Z-parameters are very sensitive to measurement error, and require high accuracy equipment to be measured properly. Methodology 19 3. The measurements were made at kHz and kHz, as this thesis focuses on the frequency range from kHz, which will be discussed further in Section 3. The mutual inductance between the coils can be calculated by measuring the equivalent inductance of the two coils when they are connected in series, such as they are aiding or opposing each other [16], as shown in Figure 3.

When the coils are aiding each other, the inductance measured by the LCR meter is higher than that of either coil separately, whereas when the coils are opposing each other, the measured inductance is lower than that of either coil.

They have a spiral structure with dimensions and characteristics described in Table 3. Each coil has a layer of ferrite attached to it, as can be seen in a picture of one of the coils in Figure 3. The purpose of the ferrite is to improve the coupling between the coils, and the attached ferrite is of Ni-Zn type. The lateral distance could be changed between 0 mm and around 35 mm. The vertical spacers that were used had a thickness of 1. The minimum vertical distance is achieved by putting the upper coil directly on the black plastic layer below it.

The possible vertical distances between the coils were 1. The initial distance is set by the upper coil being attached to the "default position" of the transparent plastic layer shown in Figure 3. Their respective size and shape can be found in Table 3. Methodology 21 Figure 3. The simulations allow for the calculations of currents, voltages and phase relationships using the FHA model.

Additionally the simulations were used as a reference for comparison with measurement data. An example showing the result of a simulation of the current through a resistive load connected to the secondary side can be seen in Figure 3. From 80 kHz to kHz measurements were made every 2. In the range from kHz to kHz measurements were made every Because of hardware limitations, data could not be collected for the higher powers for every operating scenario.

Frequen- cies far from resonance, as well as low coupling factor, require large input voltages in order to reach the higher power, beyond the 40 V limit of the PA. The following tables shows the vertical and lateral distances used with their corresponding coupling factors.

For each lateral distance, the vertical distance of 2 mm is used. The vertical dis- tance is measured from surface to surface between the coils, and the lateral distance from center to center, as illustrated in Figure 3. Vertical Distance k 1. Methodology 25 Figure 3. To achieve this, a custom software was developed in Matlab. The software was made to control the A function generator as well as the Tektronix oscilloscopes. For a given set of frequencies, the software would ramp up the voltage at the coil system input until a target power level was reached.

Once reached, the oscilloscope would make a measurement and the data would be saved. The voltage would then be further increased until all targeted power levels were reached, after which the process would be repeated for the next frequency point.

Each measurement made by the oscilloscope would result in a waveform cap- ture, consisting of a collection of data points showing the magnitude of each mea- sured quantity over a number of cycles. The result from a frequency sweep would be a set of waveform captures, one for each measured quantity and power level, over the target range of frequencies.