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AQ: Grain Storage system

A Grain Storage system usually consists of the following elements

1. A means of measuring Grain coming in and out- Usually a truck scale or a bulk weighing system. In addition some applications require measuring grain between transfers to different bins and a bulk weighing system is usually used for that.

2. A means of transferring between different operations or storage location- Conveyors, screws, buckets, pneumatic, wheel house.

3. Dust Collection

4. And Equipment for the operations that will be performed, drying, cleaning, screening, grading, sampling, roasting, steaming, packaging etc.

A system I have just completed was 24 containers + 3 buildings for storage with 76 conveyors, 3 drop-off and 3 loading points. Connection to ERP system and weigh scales to weigh trucks and send them to the correct bay. Local HMI on each bay ensured correct lorry goes to correct bay. Main conveyor runs are automatically selected. Manual option to run all conveyors to move grain around.

System used Ethernet infrastructure with hubs mounted strategically around tank farm. Also implemented soft starter with Ethernet connectivity, thus allowing easy monitoring of current consumption + for maintenance.

The future-proof design will allow customer to install level and humidity measurement in the future using the Analogue IO connected on Ethernet.

AQ: How to suppress chaotic operation in a DCM flyback at low load

I would like to share these tips with everybody.
A current mode controlled flyback converter always becomes unstable at low load due to the unavoidable leading edge current spike. It is not normally dangerous but as a design engineer I don’t like to look at it and listen to it.

Here are three useful and not patented tips.

First tip:
• Insert a low pass filter, say 1kohm + 100pF between current sense resistor and CS input in your control IC.
• Split the 1kohm in two resistors R1 to the fet and R2 to the control IC. R1 << R2.
• Insert 0,5 – 1pF between drain and the junction R1/R2. This can be made as a layer-to-layer capacitor in the PCB. It does not have to be a specific value.
• Adjust R1 until the spike in the junction in R1/R2 is cancelled.
You will see that the current spike is always proportional to the negative drain voltage step at turn-on. Once adjusted, the cancellation always follows the voltage step, and you some times achieve miracles with it. Cost = one resistor.

Second tip:
Having the low pass filter from first tip, add a small fraction of the gate driver output voltage to the current sense input, say 0,1V by inserting a large resistor from ‘Drive Out’ to ‘CS input’. The added low pass filtered step voltage will more or less conceal the current spike. You should reduce your current sense resistor accordingly. Cost = one resistor.

Third tip:
In a low power flyback, you some times just need an RC network or just an extra capacitor from drain to a DC point, either to reduce overshoot or to reduce noise. Connect the RC network or the capacitor to source, not to ground or Vcc. If you connect it to ground or Vcc, you will measure the added discharge current peak in the current sense resistor. Cost = nothing – just knowledge.

All tips can be used individually or combined => Less need for pre-load resistors on your output.

AQ: Determine coefficient of grounding

Determination of required grounding impedance is based on determination of coefficient of grounding which represents ratio of maximum phase voltage at phases which aren’t exposed by fault and line voltage of power network:

kuz=(1/(sqrt(3)))*max{|e(-j*2*π/3)+(1-z)/(2+z)|; |e(+j*2*π/3)+(1-z)/(2+z)|}
z=Z0e/Zde

where are:

kuz-coefficient of grounding,
z-ratio of equivalent zero sequence impedance viewed from angle of place of fault and equivalent direct sequence impedance viewed from angle of place of fault,
Z0e-equivalent zero sequence impedance viewed from angle of place of fault,
Zde-equivalent direct sequence impedance viewed from angle of place of fault.

So, after this explanation, you can get next conclusions:
if kuz=1 then power network is ungrounded because Z0e→∞, which is a consequence of existing more (auto) transformers with ungrounded neutral point than (auto) transformers with grounded neutral point (when kuz=1 then there aren’t (auto) transformers with grounded neutral point),
if kuz≤0,8 then power network is grounded because Z0e=Zde, which is a consequence of of existing more (auto) transformers with grounded neutral point than (auto) transformers with ungrounded neutral point.

Fault current in grounded power networks is higher than fault current in ungrounded power networks. By other side, in case of ungrounded power networks we have overvoltages at phases which aren’t exposed by fault, so insulation of this conductors could be seriously damaged or in best case it could become older in shorter time than it is provided by design what is the main reason for grounding of power networks.
Coefficient of grounding is very important in aspect of selecting of insulation of lighting arresters and breaking power of breakers, because of two next reasons:
1. in grounded power networks insulation level is lower than insulation level in ungrounded power networks,
2. in grounded power networks value of short circuit current is higher than value of short circuit current in ungrounded power networks.

AQ: How to design an Panel required for PLC / MCC / Drive

1. The regular industrial standard size panel available with most of the panel fabricator’s.
2. Type of protection (used to say as IP).
3. Spacing depends upon the Power handled by the conductors inside Panel and the ventilation system.
4. Cable Entry / Bus bar entry may depend on the application and site condition. it may be at rear/bottom or at the top.
5. When comes to Drive, if the site condition is too hot then an industrial ac is required usually attached at the side of the panel.
6. Drive to drive required spacing (Check the manual of the drive}, since the power switching activity take place inside the drive.
7. Provide required space for the transformers and AC-choke since they create magnetic flux in ac circuits.
8. Don’t mix the Control cable, Power cable, Signal cable and Communication cable together in the cable tray… Otherwise you will be wired…
9. Keep the control on mcb/mccb/mpcb in handy location. So that its easier for operator to control it frequently and not disturbing other circuits..
10. Plc will be acquiring the top position in the panel since there is nothing to do with it once installed. Just we will be monitoring the status.
11. Don’t place the Plc nearby to the incoming or outgoing heavy power terminals..
12. Mcc panel are easy thing to do, but do the exact calculation for the ACB selection in the incomer side. Since each feeder will be designed with tolerance level.

There being a lot more than 12 guidelines to follow. What
about back-up power for the PLC? What about internal heat flow considerations
(not just does it need an AC or not)? How much space between terminal blocks
and wireway? What about separate AC and instrument grounds? What about wireway
fill? What about wire labels? What about TSP shields? What about surge
protection? In my experience, there are plenty of people that can design a
panel but if they haven’t gone to the field with it then they haven’t been able
to learn from their design mistakes.

The best thing you can do is start your design but you
really need to be guided by an experienced designer.

AQ: Right Half Plane Pole

Very few know about the Right Half Plane Pole (not a RHP-Zero) at high duty cycle in a DCM buck with current mode control. Maybe because it is not really a problem.
It is said that this instability starts above 2/3 duty cycle – I think that must be with a resistive load. If loaded with a pure current source, it starts above 50% duty cycle.

Here is a little down-to-earth explanation:
If you run a buck converter at high duty cycle but DCM, it probably works fine and is completely stable. Then imagine you suddenly open the feedback loop, leaving the peak current constant and unchanged. The duty cycle will then rush either back to 50% or to 100% if possible. You now have a system with a negative output resistance – if Voltage goes up, the output current will increase.

You can see it by drawing some triangles on a piece of paper: A steady state DCM current triangle with an up-slope longer than the down-slope and a fixed peak value. Now, if you imagine that the output voltage rises, you can draw a new triangle with the same peak current. The up-slope will be longer, the down-slope will be shorter but the sum of times will be longer than in the steady state case. The new triangle therefore has a larger area than the steady state triangle, which means a higher average output current. So higher output voltage generates higher output current if peak current is constant. Loaded with a current source, it is clear that this is an unstable system, like a flipflop, and it starts becoming unstable above 50% duty cycle.

However, when you close the feedback loop, the system is (conditionally) stable and the loop gain is normally so high at the RHP Pole frequency that it requires a huge gain reduction to make it unstable.

It’s like when you drive on your bike. A bike has two wheels and therefore can tilt to either side – it is a system with a low frequency RHPP like a flipflop. If you stand still, it will certainly tilt to the left or to the right because you have no way to adjust your balance back. But if you drive, you have a system with feedback where you can immediately correct imbalance by turning the handlebars. As we know, this system is stable unless you have drunk a lot of beers.

AQ: What causes VFD driven motor bearing current?

There are several things involved, all with varying degrees of impact.

Large machines are – generally speaking – made of pieces (segments) because the circle for the stator and/or rotor core is too large to manufacture from a single sheet. This leads to some breaks in the magnetic flux path symmetry, both in the radial (right angles to the shaft) and axial (parallel to the shaft) directions.

For the most part, the windings of large machines are formed and installed by hand. This too can lead to symmetry issues, as the current paths are not identical which in turn will create some differences in the magnetic field flux.

Output waveforms from power electronics are only approximations of true sinusoids. The presence of additional harmonics distorts the sinusoidal nature and results in changes that are not symmetric in the magnetic field strength … which in turn means a non-symmetric flux distribution.

Two other items contribute to potentially damaging bearing currents as well. One of these is the Common Mode Voltage which is present (to some degree) in all drives. Essentially this is a signal that is present at both the drive input and output … I tend to think of it as an offset. It’s not something that traditional grounding addresses, and can create an elevated potential in the shaft which then discharges through the bearing path.

A second item is not related to the presence (or absence) of drives at all; it is related to the mechanical arrangement of the process drive train. For example, a shaft that has a sliding seal (like the felt curtain on a dryer section), or one that turns a blade against a gas or liquid (like a compressor) can generate a static charge at the point of contact. If there is no means of isolating this charge to the portion of the shaft where the sliding is occurring, it can pass through to the motor shaft and thence through the motor bearings.

Lastly – the frequency of the variable frequency drive harmonics in the output waveform is significantly higher than line frequency. This requires specific accommodations for grounding as traditional methods are insufficient due to the attenuation caused by the relatively high resistance ground path.

AQ: Avoid voltage drop influence

My cable size and transformer size should give me maximum 3% on the worst 6% to 10%. If it is the single only equipment on the system then maybe you can tolerate 15%. If not, dip factor may affect sensitive equipment and lighting.

This is very annoying for office staff each time a machine starts lights are dimming. It does not matter what standard you quote I cannot accept 10%- 15% make precise calculation and add a 10% tolerance to avoid.

In most cases, this problem comes from cable under sizing so we have to settle with a Standard giving 15% Max.

Just recently I had to order a transformer and cable change for a project which was grossly undersized.
I have had to redesign the electrical portion of a conveyor and crushing system to bring the system design into compliance with applicable safety codes. The site was outdoor at a mine in Arizona where ambient temperatures reach 120F. The electrical calculation and design software did not include any derating of conductor sizes for cable spacing and density within cable trays, number of conductors per raceway, ambient temperature versus cable temperature rating, etc. Few of the cables had been increased in size to compensate for voltage drop between the power source and the respective motor or transformer loads.

Feeder cables to remote power distribution centers were too small, as voltage drop had not been incorporated in the initial design. The voltage drop should not be greater than 3%, as there will be other factors of alternating loads, system voltage, etc. that may result in an overall drop of 5%.

The electrical system had to be re-designed with larger cables, transformer, MCCS, etc, as none of the design software factors in the required deratings specified in the National Electric Code NFPA70 nor the Canadian Electric Code, which references the NEC.

AQ: Experience: Flyback

My first SMPS design was a multiple output flyback. This was in 1976, when there were no PWM controllers. So I used a 556 (1/2 osc -30 kHz, and 1/2 PWM generator) plus used a 3904 NPN where the VBE was the reference and also provided gain for the error amp function. I hap-hazardly wound the windings on a 25 mm torroid. It ranglike a tank circuit. I quickly abandoned the transformer and after a year, and many hours on the bench, I had a production-grad SMPS.
Since it went into a private aircraft weather reader system, I needed an exterier SMPS which was a buck converter. I used an LM105 linear regulator with positive feedback to make it oscillate (one of nationals ap notes). It worked, but I soon learned that the electrolytic capacitors lost all of their capacitance at -25 deg C. It later worked with military-grade capacitors.

I had small hills of dead MOSFETs and the directly attached controllers. When the first power MOSFETs emerged in 1979, I blew-up so many that I almost wrote them off. They had some real issues with D-S voltage overstress. They have come a long way since.

As far as very wide range flyback converter, please dig-up AN1327 on the ONSEMI website. This describes a control strategy (fixed off-time, variable on-time) and the transformer design.
The processor to that was a 3W flyback that drove 3 floating gate drive circuits and had an input range of 85 VAC to 576 VAC. It was for a 3 phase industrial motor drive. The toughest area was the transformer. To meet the isolation requirements of the UL, and IEC, it would have required a very large core, and bobbin plus a lot of tape. The PCB had the dimensions of 50 mm x 50 mm and 9 mm thick A magnetics designer named Jeff Brown from Cramerco.com is now my magnetics God. He designed me a custom core and bobbin that was 10 mm high on basically an EF15 sized core. The 3 piece bobbin met all of the spacing requirements without tape. The customer was expecting a 2 – 3 tier product offering for the different voltage ranges, but instead could offer only one. They were thrilled.

Can be done, watch your breakdown voltages, spacings and RMS currents. I found that around 17 -20 watts is about the practical limit for an EF40 core before the transformer RMS currents get too high.

AQ: Impedance analyzer

A graphical impedance analyzer with good phase resolution is a must. Some brands have all the bells and whistles, but not the phase resolution necessary to accurately measure high Q (100+) components over the instrument’s full frequency range (which should extend at least into the low megahertz). Of course the Agilent 4294A fills the performance bill, but with a $40k+ purchase bill, it also empties the budget (like similar high end new models from Wayne Kerr). Used models from Wayne Kerr work very well, and can be had for under $10K but they are very heavy and clunky with very ugly (but still useable) displays.

Perhaps the best value may be the Hioki IM3570, which works extremely well with superior phase resolution, has a very nice color touch screen display (with all the expected engineering graphing formats), is compact and lightweight, and costs around $10k new. Its only downside is that its fan is annoyingly loud and does not reduce its noise output during instrument idle.

But where should an impedance analyzer rank on the power electronics design engineer’s basic equipment list (and why)?

Beyond the basic lower cost necessities such as DMMs, bench power supplies, test leads, soldering stations, etcetera, I would rank a good impedance analyzer second only to a good oscilloscope. The impedance analyzer allows one to see all of a component’s secondary impedance characteristics and to directly compare similar components. Often overlooked is the information such an instrument can provide by examining component assemblies in situ in a circuit board assembly. Sometimes this can be very revealing of hidden, but influential layout parasitics.

Equally importantly, an impedance analyzer allows accurate SPICE models to be quickly formulated so that simulation can be used as a meaningful design tool. Transformer magnetizing and leakage inductances can be measured as well as inter-winding capacitance and frequency dependent resistive losses. From these measurements and with proper technique, a model can be formulated that nearly exactly matches the real part. Not only does this allow power circuits and control loops to be initially designed entirely by simulation (under the judicious eye of experience, of course), but it even allows one to effectively simulate the low frequency end of a design’s EMI performance.

AQ: Maximum permissible value of grounding resistance

For grounding in the US it typically goes like this: Utility transformer has one ground rod. Then from the utility to the building you typically have three phase conductors and one neutral/ground conductor landing on the main panel with the utility meter. At that point we drive a ground rod. And we bond the ground rod to the water pipes (generally). And we bond the ground rod to the building steel (generally). Water pipes are generally very well connected to ground and the building steel is a nice user ground. With all these connections you typically have a good ground reference. Now, if that utility neutral wire is bad or too small, then you can have poor reference to ground between phases (a normal sign of that is flickering lights even when the load is not changing much).

Grounding impedance of the transformer and building ground rods is mainly for voltage stabilization and under normal conditions should have nothing to do with our return ground fault current. See NEC 250.1 (5) “The earth shall not be considered as an effective ground-fault current path.”

Let’s say we have a system with the building transformer and panel to ground impedance of 1000 ohms (we built this place on solid rock). Okay, we have a poor 277V reference and we will have flickering lights (that 277 voltage will bounce all over the place). But now, in our system above, if we take a phase wire and connect it to a motor shell, which is also connected to our grounding wire, will the upstream breaker trip? The answer is yes. If our phase-to-ground fault impedance is low we will trip the upstream feeder breaker no matter what the main panel ground rod impedance is. My point here is that is does not matter what our transformer grounding is or what our panel grounding is (ground rod is not important in this case). The breaker must trip because our circuit is complete between the phase conductor and the transformer wye leg.

As long as we have a utility main transformer to panel neutral conductor of proper size to handle our fault current and we size our grounding conductors properly and they are properly connected at each subpanel and each motor in our case, we will apply nearly full phase to ground voltage because our real ground fault path is from that motor, through the grounding conductor, through our sub panels, to our main panel, than back to the transformer. That ground current must flow through our building grounding conductor to the main panel and back to the transformer through that utility neutral wire which is connected to the wye leg of the transformer. And it does not matter what the transformer to ground rod connection is. We could take that out the transformer to ground rod connection and the main panel to ground rod connection completely and we are still connecting that phase wire, through the motor metal to the grounding conductor back to the wye leg of that utility transformer, which will complete our electrical circuit. Current will flow and the breaker will trip.