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Magnetic Levitation |
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Levitation
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Levitator Simulation Using PSPICEWhat if you wanted to analyze this circuit using engineering CAD (computer aided design) tools? Many engineering students and some working engineers have access to PSPICE and other commercial tools. You can gather a great deal of insight into this circuit, and easily experiment with changes. I am using Allegro Design Entry CIS v10.3.0.p001, produced by Cadence Design Systems. This tool integrates schematic capture with PSPICE simulation and other tools. I provide all my files, in the hope you can use them to do your own analysis. Levitator Package DownloadDownload levitator package here Although my package was produced by Allegro tools, the netlist and PSPICE files are text-based industry standard format. You can import selected files into many other implementations of PSPICE. Please note the inputs to U3 are swapped, so it becomes a non-inverting amplifier. This makes the graphs more natural and a bit easier to read since they're right-side-up. It is not a problem during analysis because the Signal and Reference points are symmetric. However, it is a departure from the real-world schematic and, if you closed the loop in PSPICE, it would not function properly. DC Operating PointAll stages are dc-coupled. This is required for any controller that must govern the absolute position of an object in space. So it is useful to know the default operating point of every node. This analysis also tells you the maximum coil current and power dissipation in various components. The result of the bias point calculation from Allegro is:
Let's look at the stages one by one, calculate the gain, and compare them to the original design. DC Sweep: Gain of Difference AmplifierIf we connect a small dc voltage source to the input signal's resistor divider, then we can examine the circuit behavior over the entire operating range. This is called a dc sweep. The results from Allegro to compare the difference amplifier (U3) to input voltage (Vx): From the linear data points above (and using the waveform cursor), we can calculate the first
stage gain: This is a bit higher than calculated gain of 9, but it seems reasonable. DC Sweep: Gain of Phase Lead NetworkNow let's see the gain (attentuation) introduced by the phase lead network. We can use the same Vx input voltage, and study the signal strength at the junction of R7 and R8: The total gain after the phase lead network is Gain = 3.2267 / 2.5 = 1.291. We can isolate the
gain (attentuation) of the phase lead network by dividing by the first stage's gain, which yields: This is a good match with the calculated gain of 0.128. DC Sweep: Gain of Output AmplifierIn a similar fashion, we can use the "dc sweep" function for the output stage gain
alone: This is a good match with the calculated gain of 247. DC Sweep: Coil Current versus Sensor VoltageNow that we've seen all the individual stages, let's see how the coil current depends on the sensor voltage. This is an excellent "paper test" of the overall dc-coupled design. This also provides the end-to-end gain figure, which might be useful for analyzing the closed-loop control circuit. The results from Allegro for coil current versus input sensor voltage:
AC Frequency ResponseWe will set up the AC sweep for the levitator, to get the phase and magnitude of sinusoidal waveforms over a range of frequencies. This will tell us the coil current's frequency response. We do this by replacing Vx (dc power) with VAC for a small-signal sweep. The tools calculate the bias point, and the AC sweep is performed on a linearized model. This approach can only be used to find the small-signal gain and frequency response. Items such as voltage swing, clipping, and saturation must be obtained from the transient simulation, or by using the operating point information. The Bode plot of small signal gain is:
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Last Update 2008-11-30
©1998-2023 Barry Hansen |