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UNIVERSITY OF IDAHO DEPARTMENT OF ELECTRICAL AND COMPUTER ENGINEERING Interfacing an Avista SR-12 Hydrogen Fuel Cell to the Analog Model Power System (AMPS) May 13, 2005 Project by: Daniel Hubbard Sponsors/Advisors: Dr. Brian Johnson [email protected] ECE Department University of Idaho Adam Lint Dr. Herb Hess [email protected] ECE Department University of Idaho Chris Cockrell [email protected]

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Page 1: UNIVERSITY OF IDAHO DEPARTMENT OF … Report I/Final...Interfacing an Avista SR-12 Hydrogen Fuel Cell to ... along with simulation data for the entire ... The PSpice simulation of

UNIVERSITY OF IDAHO DEPARTMENT OF ELECTRICAL AND COMPUTER ENGINEERING

Interfacing an Avista SR-12 Hydrogen Fuel Cell to the Analog Model Power System (AMPS)

May 13, 2005

Project by: Daniel Hubbard Sponsors/Advisors: Dr. Brian Johnson [email protected] ECE Department University of Idaho Adam Lint Dr. Herb Hess [email protected] ECE Department University of Idaho Chris Cockrell [email protected]

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Abstract Alternative energy sources are of great focus in the energy industry as the world realizes that its dependency on fossil fuels must diminish because of pollution, oil prices, or other factors. For this reason it is important that students at the University of Idaho have exposure to some of the alternative energy sources available in the 21st century. This report outlines a plan for interfacing an Avista SR-12 hydrogen fuel cell to the UI analog model power system. Fuel cell characteristics and system specifications are discussed along with simulation data for the entire system. However, the primary focus of the simulation data discussion is on the zero detection circuitry used for synchronizing the AC signal from the DC/AC converter with the utility frequency. The results of this simulation provide a method for implementing the design in hardware and show that the system will need to be designed to transfer a maximum of 200W to the AMPS. Key Terms: Fuel Cell, Alternative Energy, Zero-Crossing Detection, Synchronization, Voltage Regulation, Voltage Conversion, Model Power System.

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TABLE OF CONTENTS:

1 PROJECT DESCRIPTION ................................................................................................... 1

1.1 OBJECTIVE AND SCOPE ........................................................................................................ 1 1.2 REQUIREMENTS .................................................................................................................... 1 1.3 SIGNIFICANCE OF THE PROJECT.......................................................................................... 2 1.4 BACKGROUND/HISTORY ...................................................................................................... 3 1.5 FUNCTIONAL SPECS.............................................................................................................. 3 1.6 CONTRAINTS ......................................................................................................................... 3 1.7 SOLUTION.............................................................................................................................. 4

2 STATUS ................................................................................................................................... 5

2.1 DESIGNED AND WORKING.................................................................................................... 5 2.2 DESIGNED AND NOT WORKING ........................................................................................... 5 2.3 DESIGNED AND NOT TESTED................................................................................................ 6 2.4 NOT DESIGNED...................................................................................................................... 6

3 METHOD OF SOLUTION.................................................................................................... 7

3.1 FUEL CELL ............................................................................................................................ 7 3.1.1 TYPES OF FUEL CELLS [3]................................................................................................. 7 3.1.2 OPERATION OF THE PEM FUEL CELL ............................................................................. 8 3.1.3 THE AVISTA SR-12 PEM FUEL CELL .............................................................................. 9 3.1.4 CHARACTERIZING THE SR-12 FUEL CELL ...................................................................... 9 3.1.5 ADDITIONAL CONSIDERATIONS ...................................................................................... 11 3.2 DC/DC CONVERTER........................................................................................................... 12 3.3 FLYBACK CONVERTER ....................................................................................................... 13 3.4 DC/AC CONVERTER........................................................................................................... 13 3.5 TRANSFORMER.................................................................................................................... 14 3.6 SYSTEM CONTROL.............................................................................................................. 15 3.6.1 DC TO AC CONVERTER .................................................................................................. 16 3.6.2 ZERO-CROSSING DETECTION ......................................................................................... 19 3.7 PROTECTION ....................................................................................................................... 24

4 VALIDATION....................................................................................................................... 25

4.1 FUEL CELL .......................................................................................................................... 25 4.2 DC/DC CONVERTER........................................................................................................... 26 4.3 DC/AC CONVERTER........................................................................................................... 26 4.4 ZERO-CROSSING DETECTION CIRCUITRY ........................................................................ 26

5 RESULTS .............................................................................................................................. 27

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5.1 FUEL CELL OPERATING PROCEDURE ............................................................................... 27 5.1.1 SAFETY AND CARE OF THE FUEL CELL.......................................................................... 27 5.1.2 STARTUP PROCEDURES ................................................................................................... 27 5.1.3 TROUBLESHOOTING ........................................................................................................ 28 5.2 VALIDATION RESULTS........................................................................................................ 29 5.2.1 DC/DC CONVERTER........................................................................................................ 29 5.2.2 DC/AC CONVERTER........................................................................................................ 30 5.2.3 ZERO DETECTION CIRCUITS........................................................................................... 32 5.3 COST ANALYSIS .................................................................................................................. 34

BIBLIOGRAPHY ....................................................................................................................... 35

APPENDIX .................................................................................................................................. 36

APPENDIX A – COMPAC DC/DC CONVERTER DATA SHEET................................................... 37 APPENDIX B – LF356 OP-AMP DATA SHEET............................................................................. 42 APPENDIX C – H11L1 OPTOISOLATOR DATA SHEET ............................................................... 52 APPENDIX D – ZERO DETECTION: CIRCUIT ANALYSIS ............................................................ 62 APPENDIX E – ZERO DETECTION: SIMULATION ....................................................................... 65 APPENDIX F – INDIVIDUAL PROJECT CONTRIBUTIONS ............................................................ 72

FIGURES AND TABLES:

TABLE 1 - PRELIMINARY FUEL CELL VOLTAGE LEVELS ............................................................................... 10 TABLE 2 - FUEL CELL LOADING CHARACTERISTICS ..................................................................................... 11 TABLE 3 - TROUBLESHOOTING THE FUEL CELL ............................................................................................ 28 TABLE 4 - BUDGET........................................................................................................................................ 34

FIGURE 1 - FUNCTIONAL BLOCK DIAGRAM .................................................................................................... 4 FIGURE 2 - PEM CHEMICAL REACTION .......................................................................................................... 8 FIGURE 3 - FUEL CELL LOADING CURVE ...................................................................................................... 11 FIGURE 4 - SCHEMATIC OF A FLYBACK CONVERTER..................................................................................... 13 FIGURE 5: TRIANGLE WAVE GENERATOR ..................................................................................................... 16 FIGURE 6: SINE WAVE GENERATOR.............................................................................................................. 17 FIGURE 7: DELTA ANGLE CONTROLLER........................................................................................................ 17 FIGURE 8: CONVERTER VOLTAGE CONTROLLER........................................................................................... 18 FIGURE 9: GATE SWITCHING CONTROL......................................................................................................... 18 FIGURE 10 - ZERO DETECTION CIRCUITS [4]................................................................................................. 20 FIGURE 11 - ZERO DETECTION CIRCUIT INPUT STATE [4] ............................................................................. 22 FIGURE 12 - ZERO DETECTION CIRCUIT MIDDLE STATE [4] ......................................................................... 23 FIGURE 13 - DC/DC CONVERTER ................................................................................................................. 29 FIGURE 14 - DC TO DC CONVERTER OUTPUT .............................................................................................. 30 FIGURE 15 - SYSTEM SIMULATION MODEL ................................................................................................... 31 FIGURE 16 - PWM INPUT: 1-PHASE .............................................................................................................. 31 FIGURE 17 - THREE PHASE AC OUTPUT ....................................................................................................... 31 FIGURE 18 - OP-AMP INPUT PIN SIMULATION............................................................................................... 33 FIGURE 19 - ZERO DETECTION CIRCUITS OUTPUT SWITCHING ..................................................................... 33

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1 Project Description

1.1 Objective and Scope The project objective is to interface an Avista SR-12 hydrogen fuel cell to the University

of Idaho Analog Model Power System (AMPS). This project will allow the fuel cell to

provide supplemental power to AMPS. Overall power quality and capacity is not

important in this project, as our main goal is to simply create the interface. Protection

circuitry is important to shield the fuel cell and the interface design from power surges or

faults on the AMPS.

1.2 Requirements

The requirements for this project are as follows:

1. Operation of the Fuel Cell must be better documented.

a. ECE students must be able to initialize and shut down the fuel cell in a

safe and timely manner.

b. ECE students must be able to identify and efficiently correct problems that

arise as a result of fuel cell operation.

2. The power converters must be simulated to show knowledge of their operation.

a. The DC to DC power converter for the fuel cell must accept 18-36V DC

and regulate it to 12V DC at the output. A tolerance of ±1V is acceptable.

b. The DC to AC power converter for the fuel cell must invert the regulated

DC voltage to a sinusoidal three-phase 208 V line-to-line AC voltage

±2%.

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c. All power converters, transformers, and other circuitry used in this design

must be capable of handling 200W peak power though, ideally, only

100W will ever pass through them.

3. The overall system simulation must provide power to the AMPS.

a. The fuel cell, when interfaced to the AMPS, must provide positive three

phase AC power flow into the model power system.

b. The interface design must include protective circuitry to ensure that surges

on the AMPS do not damage the fuel cell, either of the converters, the

transformer, or the zero detection circuitry.

4. The fuel cell system must be able to synchronize with the AMPS without drawing

excessive current.

a. “Excessive” will be classified as any current above the rated conditions for

the fuel cell: approximately 11A.

b. Maximum phase error will need to be determined by circuit analysis after

measuring the line impedance of both the fuel cell system and the AMPS.

1.3 Significance of the Project

The AMPS provides students with the opportunity to explore and understand a typical

power transmission system. The ECE department wishes to expand and improve this

system to include alternative energy sources. This project will further facilitate the

learning experience for students and enable them to experiment with new technologies in

the power industry. Ultimately, this project will benefit power companies and the people

of our nation as UI’s students can apply their knowledge in the workforce.

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1.4 Background/History In the mid-1990’s, the University of Idaho acquired the Analog Model Power System

(AMPS) from Idaho Power [1]. The AMPS is located in the basement of the Buchanan

Engineering Laboratory on UI’s main campus in Moscow, Idaho. The purpose of AMPS

is to provide insight into the workings of a power transmission and distribution system.

The main source of power is from the local utility company, Avista. Currently, a

generator is also interfaced with the AMPS to provide additional power to the system.

In addition to the generator, the UI has obtained an Avista SR-12 Hydrogen Fuel Cell

from Genesis Fueltech [2]. This fuel cell represents one of many alternative energy

sources available in the 21st

century.

1.5 Functional Specs The specifications for the interface are:

• 18-36V DC input from the Fuel Cell • Output 208V +/- 2 % (L-L 3-phase) • Output Voltage at 60Hz +/- 0.05Hz • Max power flow of 200W for the interface • Max phase difference when synchronizing; to be determined

1.6 Contraints The system must not draw power from the AMPS. It must be easy to operate and simple

to maintain. All safety precautions must be properly labeled to ensure the user’s safety.

Other constraints for the system include but are not limited to cost, reliability and

performance.

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1.7 Solution

In order to accomplish the project objective, a DC/DC was converter simulated to

regulate the DC output voltage of the fuel cell to a constant level (12V). After the

voltage has been regulated, it will be run through a custom-designed flyback converter to

step-up the voltage 120V DC. A custom-programmed DC/AC converter will then

convert the 120Vdc input to a three-phase AC signal at 60 hertz; the line to line output

voltage should be about 95 percent of the DC input due to switching losses in the

inverter. A parallel three-phase transformer will step up the voltage to 208V line to line

and connect to the AMPS to supply supplemental power. To correctly interface the

produced AC signal to the AMPS, the three phase signal must be synchronized with the

three phase signals already on AMPS. Zero detection circuitry connected to one of the

three phases on AMPS will provide the DC/AC converter with the required timings and

phase necessary for proper synchronization. A graphical representation of the design can

be seen below in a functional block diagram (Figure 1).

Figure 1 - Functional Block Diagram

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2 Status

2.1 Designed and Working In this project, the most important module is the Avista SR-12 PEM fuel cell. Its

characteristics define the specifications of all the other modules required to successfully

interface our system to the AMPS. A couple of modifications have been made to render

the fuel cell functionally operational and to increase performance specifications, such as

the external batteries and the bubble humidifier. Currently, the hydrogen fuel cell will

operate steadily at a maximum of 150W.

The design simulations are also operational. For the PSCAD simulation, the system

outputs a 208V line-to-line three phase signal—meeting the specifications for connecting

to the AMPS. The PSpice simulation of the zero crossing detection circuit is also fully

functional, capable of successfully detecting the desired crossing within 22 microseconds.

The results of these simulations are discussed in section 5.2 of this report.

2.2 Designed and Not Working While the simulated design is functional, difficulties with finding a low voltage DC/AC

inverter have arisen. The supplier for this device, Tier Electronics, will be unable to

provide a device for a price within the proposed budget. However, Tier Electronics can

supply a 120V inverter at a reasonable price; and, after some consideration, another

design alternative has been considered. This design alternative would require that the DC

voltage from the output of the fuel cell be regulated and increased to 120V, requiring the

use of a boost or flyback converter instead of a buck converter. Because low voltage,

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wide input boost converters would typically saturate before reaching the desired output, a

flyback converter is the most viable design option at this point. Further research will be

performed regarding the use of a flyback converter so that the overall design can be

adjusted to fit specifications and an appropriate power inverter can be purchased before

the start of the second phase of this project.

2.3 Designed and Not Tested The alternative design that incorporates the use of a flyback converter has not yet been

tested. Pending research and testing, proper functionality is expected and will allow us to

continue with the projected schedule. All other components, except for the fuel cell, have

not been physically tested since they are only available in simulation at this point.

2.4 Not Designed The control algorithm for the TI-2403 DSP has not yet been completely finalized. The

top down design has been started but does not define all of the present needs. Inquiries

and research into code algorithms and how the DSP will control the system components

have commenced but the algorithms are far from being designed. The greater portion of

next semester has been planned and set aside to meet these important criteria.

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3 Method of Solution

3.1 Fuel Cell 3.1.1 Types of Fuel Cells [3] There are five different types of fuel cells currently being operated and manufactured.

Each is named for the type of electrolyte used in the individual cells. Alkaline fuel cells

(AFCs) are the oldest design. AFCs have been used in the U.S. space program since the

1960’s but are not widely used within the earth’s atmosphere because of their

susceptibility to contamination due to impurities in the air. Because they require pure

hydrogen and oxygen to operate, they must be operated in special containment

environments, which make them expensive and impractical for terrestrial use.

Solid oxide fuel cells (SOFCs) are capable of supplying as much power as large utility

grade generators but operate at much higher temperatures than other types of fuel cells—

around 1000°C. SOFCs require more maintenance than other fuel cells because of their

high temperature, but they are potentially more efficient because the steam generated by

the high temperature operation can be used to power turbines and generate more

electricity. Molten carbonate fuel cells (MCFCs) run at lower temperatures than SOFCs

but still have the capability of generating steam. Their lower temperature (around 600°C)

makes them cheaper than SOFCs, but they still surpass other types of fuel cells with

respect to cost.

Phosphoric acid fuel cells (PAFCs) have a much lower operating temperature than

SOFCs or MCFCs, but they have a longer warm-up time than proton exchange membrane

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fuel cells (PEMs). PEMs are relatively cheap to manufacture and maintain, and they

operate at temperatures around 80°C. They also have a fast startup time and are small

and portable compared to the other types of fuel cells. This makes them suitable for a

wide variety of applications. A PEM fuel cell has been donated to the University of

Idaho ECE department and will be used to complete this project.

3.1.2 Operation of the PEM Fuel Cell Proton exchange membrane fuel cells undergo a chemical reaction similar to that of a

battery. As shown in Figure 2, the hydrogen molecules are stripped of their electrons by

a thin membrane that has been specially treated to only conduct positively charged ions.

The electrons flow through a load and to the cathode where two oxygen atoms will

combine with the hydrogen ions to create water and heat.

Figure 2 - PEM Chemical Reaction

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3.1.3 The Avista SR-12 PEM Fuel Cell In 2003, the University of Idaho ECE department acquired a 500W Avista SR-12 PEM

fuel cell from Genesis Fueltech. This unit contains 12 fuel cell cartridges, and was once

capable of providing 500W peak power with a variable DC voltage range of 23V to 43V

[2]. Since its manufacture in 1999, its capabilities have degraded and its characteristics

have changed. For this reason, several load tests were performed on the fuel cell to re-

characterize it. These tests have been discussed in the remainder of this section.

3.1.4 Characterizing the SR-12 Fuel Cell The values shown in Table 1 and Table 2 reveal that the actual voltage range of the fuel

cell differs from that discussed in “Avista SR-12 PEM Hydrogen Fuel Cell” [2]. Fletcher

claims that the voltage range is 23–43V DC, but by performing three separate tests, it can

be shown that the actual voltage range varies between 18V DC and 36V DC if not

severely overloaded. This smaller voltage range greatly reduces the cost of a suitable DC

to DC converter. Table 1 shows the results of tests one and two. Note that for the nine

and ten minute marks for the loaded test, the values were not available because the fuel

cell failed because of weak batteries. This will be discussed in the “Troubleshooting”

section of this report.

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Table 1 - Preliminary Fuel Cell Voltage Levels

No Load >100 W Load time voltage time voltage

1 min. 29 1 min. 232 min. 31 2 min. 23.13 min. 30 3 min. 24.124 min. 28 4 min. 24.185 min. 29 5 min. 24.156 min. 30 6 min. 24.127 min. 31 7 min. 24.148 min. 29 8 min. 24.069 min. 29 9 min. N/A10 min. 31 10 min. N/A

The results of the third test, which include all ranges of the fuel cell voltage—including

overloaded conditions, are included shown in Table 2. This table shows load data

obtained by connecting a resistive load to the fuel cell while operating under nominal

conditions. Figure 3 shows a linear operation which is characteristic of most proton

exchange membrane fuel cells. This graph more concretely verifies the voltage range

presented in section 3.1.3, though an overload condition causes it to fall below the 18V

limit. When significant current is seen on the two 12V batteries used to power the

internal circuitry, the fuel cell should be considered overloaded. To reduce battery drain,

and to stay within specifications, the fuel cell should not be run in overloaded conditions.

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Table 2 - Fuel Cell Loading Characteristics

V[V] I (Load)[A] P (load) [W] I (Batteries) [A] R [Ω

35 0.3 10.5 0.0002 116.67 34.8 0.4 13.92 0.0004 87.00

35 0.4 14 0.0003 87.50 34.5 0.5 17.25 0.0003 69.00 33.6 0.8 26.88 0.0003 42.00 31.7 1.8 57.06 0.0003 17.61 29.2 2.5 73 0.0003 11.68 30.5 2.4 73.2 0.0004 12.71

30 2.6 78 0.0003 11.54 28.9 2.8 80.92 0.0003 10.32 28.3 3.2 90.56 0.0003 8.84 27.8 3.3 91.74 0.0004 8.42 26.8 4.1 109.88 0.0001 6.54 26.6 4.4 117.04 0.0001 6.05

25 5 125 ~0.0517 5.00 25.7 4.9 125.93 ~.0093 5.24 23.4 6.8 159.12 1.11 3.44

23 7.1 163.3 ~1.23 3.24

0

5

10

15

20

25

30

35

40

0 1 2 3 4 5 6 7 8 9 10 11 12

Current (Amps)

Volta

ge (V

olts

)

Figure 3 - Fuel Cell Loading Curve

3.1.5 Additional Considerations The load tests reveal that the fuel cell is capable of supplying just over 100W of power

before overload conditions occur. This loss efficiency can be attributed to the aging fuel

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cell cartridges. These cartridges depend on moisture content to operate well, and they

have lost some of their ability to self-humidify. To correct this, a bubble humidifier filled

with de-ionized water will be connected in line with the hydrogen to increase the

humidity in the system. Theoretically, this will noticeably increase the capabilities of the

fuel cell. This increase in power has been taken into account in the design of the

interface system. All components will be designed to withstand 200W peak power from

the fuel cell.

3.2 DC/DC Converter To successfully regulate the output voltage from the fuel cell, the DC/DC converter is

required to meet the following specifications:

• Wide Input Voltage Range: 20-36V • Constant Output Voltage: 12V • Power Rating: 200W • Over voltage/Current Protection

For the initial interface design, the ComPAC DC/DC power supply from Vicor

Electronics was chosen. The ComPAC, custom-built by Vicor, completely satisfies the

above specifications. This DC/DC converter has a wide input range (18-36V DC),

constant output (12V), protection circuitry, and a power rating of 200W. The low cost of

the ComPAC converter and relatively quick delivery time (2-6 weeks) also make this

desirable. A data sheet for the ComPAC DC/DC power supply is included in Appendix

A.

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3.3 Flyback Converter As an alternative to a low voltage buck converter, a flyback converter could be used if the

120V input DC/AC converter is purchased. Since flyback converters use a transformer

with a parallel tertiary winding on the primary side to operate, they are capable of

outputting a much higher voltage range than any other type of step-up converter. Figure

4 shows the schematic diagram of a flyback converter. Since the flyback converter is a

relatively new design option, its operation and specifications have not yet been studied.

Research regarding the flyback converter will continue as phase two of this project

begins.

Figure 4 - Schematic of a Flyback Converter

3.4 DC/AC Converter The next stage of the interface design requires converting the regulated voltage from the

fuel cell into a 208V three phase AC signal at 60 hertz. A DC/AC converter inverts the

DC signal using a switching scheme controlled by a digital signal processor (DSP). For

this project, a DSP provides the calculation speeds necessary to allow for synchronization

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of the AC signals with AMPS. The DSP used by the DC/AC converter also needs to be

re-programmable to allow the converter controls to be adjusted in case of changes on the

system. As with the DC/DC converter, the DC/AC converter needs to have a power

rating of at least 200W.

The Tier Electronics Universal Power Converter (UPC) is a suitable DC/AC converter. It

will be custom-constructed for this project by Tier Electronics and is controlled by a

Texas Instrument 2403 DSP. Tier’s UPC meets the power requirements (1kW) and will

provide extra I/O pins on the DSP for zero detection signals.

3.5 Transformer Both single phase and three phase transformers were considered for this design. Single

phase transformers are normally used for large industrial applications due to the

economics associated with maintenance fees and replacement. However, this design

utilizes a three phase transformer because of its higher efficiency, smaller size, and lower

cost.

When considering three phase transformer options for this design, there were four

configuration choices: delta to delta, delta to wye, wye to delta, and wye to wye. The

simulated design incorporates a delta to wye configuration. There are two primary

reasons for this decision: a wye configuration on the high side allows the transformer to

be easily grounded. This adds a significant level of protection to the system. Because of

this grounding, a fault on any of the phases could be detected by breakers or relays in the

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ground line. Without a ground, such as with a delta configuration, the fault would go

undetected on the secondary side of the transformer and would continue to draw high

current across the transformer. This high current could damage the transformer before

being detected by other circuit protection. Secondly, a delta connection must be used on

the low voltage side in order to filter the sine-triangle pulse width modulation produced

by the switching devices used in the inverter. This filtering removes a third harmonic

that circulates in the delta and is dissipated in the transformer’s energy losses. The wye

to wye configuration would not output our desired signal because the currents could not

circulate through the transformer legs. The design specifications are only met with a delta

to wye configuration, thus the final choice for the transformer type.

The physical transformer will be designed based on the output of the power inverter.

This transformer will step up the voltage to 208V line-to-line and account for the fact that

an inverter actually outputs a peak line to line voltage of about 95 percent of the DC

voltage input.

3.6 System Control System control is important for stable operation of this interface design. The DC to AC

converter and the synchronization circuitry both play an important role in controlling the

system. The DC to AC converter will be controlled by the TI-2403 DSP. This processor

is built in to the power inverter and will be programmed based on inputs from the

synchronization circuitry to ensure stable system operation.

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3.6.1 DC to AC Converter Power inverters require a significant amount of control to operate safely and efficiently.

The simulation of the DC to AC converter contains five separate sub-systems to control

the inverter. These sub-systems, if present in hardware, will all be controlled by the TI-

2403 DSP.

Two of the systems control and regulate a synchronous sine-triangle pulse width

modulation scheme. Figure creates two separate triangle waves by tracking the power

frequency and outputting one triangle wave for turning on the switching devices and

another for turning them off. The frequency of these triangle waves is a product of a

user-defined integer and the power frequency. Figure creates two sinusoidal reference

signals that are later compared with the triangle signals.

Figure 5: Triangle Wave Generator

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Figure 6: Sine Wave Generator

The third sub-system, shown in Figure 7, is used to control power flow by varying the

angle between the converter voltage and the system voltage. The control of power flow

is represented by the following equation where Vconv is the

effective converter voltage, Vsys is the system voltage and X is the line reactance.

PV conv V sys⋅

Xsin δ( )⋅

Figure 7: Delta Angle Controller

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The forth sub-system, shown in figure 8, controls the converter Voltage, |Vconv| by

controlling the variable mi in the equation . This is an extra level of

control that can also be used to vary the power flow.

V conv mi k⋅ Vdc⋅

Figure 8: Converter Voltage Controller

Figure 9 controls the switching devices present in the DC to AC converter. It compares

the sine wave and the triangle wave and generates the PWM output necessary for turning

the switches on and off.

Figure 9: Gate Switching Control

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3.6.2 Zero-Crossing Detection For synchronization between the three phase signals produced by the DC/AC converter

and signals on the AMPS, accurate zero crossing detection is essential. If AC signals are

not synchronized when combined, current spikes and other undesirable transients will

appear on the system. In most common zero detection methods, a circuit is designed to

detect a zero crossing directly at its occurrence. This method is simple to implement but

is not relatively accurate when the precise location is necessary. The problem with single

output zero detection circuitry is that phase variations on the reference voltage will

translate into relatively inaccurate timings.

To maximize accuracy, this project utilizes a phase-locked loop algorithm that will create

two zero detection points, one right before the zero crossing and one directly after [4].

The DSP will count the time between the two signals, and then interpolate to find the

actual zero crossing. To interpolate the value, half of the count taken by the DSP will be

added to the pre-zero signal to estimate the actual zero crossing. Several readings will be

taken and then averaged to make the estimate more accurate. For this design, readings

will only be taken on the rising edge of the reference voltage.

The zero detection circuits designed for this project are shown in Figure 10. The top

circuit will give the pre-zero signal and the bottom the post-zero signal. The only

difference between the two circuits is the orientation of the biasing diodes on the input

stage.

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Figure 10 - Zero Detection Circuits [4]

3.6.2.1 Design Constraints There are several constraints that control how a zero detection circuit must be designed

for an application. The most important constraint is the speed of the circuit, or how

much time it takes for a signal to be outputted, given a zero crossing. If the circuit is too

slow, timing specifications may be violated or the DSP used to control the DC/AC

converter will not have enough time to properly control the switches for synchronization.

Another factor is that the input of the circuit needs to function under large variations of

magnitude. In this project, the input needs to handle a 120VAC signal coming from the

AMPS. The final factor is that the circuit needs to be consistent and accurate. Therefore,

noise immunity needs to be incorporated into the design of the circuit. These constraints

will be discussed in the following sections.

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3.6.2.2 Response Time To meet the timing requirements for this design, fast switching/responding devices were

chosen when creating the zero-crossing detection circuitry. The 1N914 diodes used in

this design have a max switching speed of 4ns. The 2N3904 switching transistor has rise

and fall times of 35ns and 50ns. The devices adding the most propagation delay to this

circuit are the LF356 op-amp and the H11L1 optoisolator. The LF356 op-amp has a

response time 12 V/µs (Appendix B). To reduce the response of the LF356 op-amp, the

output is clamped by a zener diode. The H11L1 has switching speed near 4µs (Appendix

C). The H11L1 optoisolator performs two functions: first, it provides isolation between

the zero detection circuit and the AMPS in case there is a surge or fault on the line; and,

second, it converts the output signal to logic levels that can be interpreted by the DSP.

3.6.2.3 Input Stage Both of the zero detection circuits utilize a resistance in series with diodes to

condition the input voltage to levels that can be used by the LF356 op-amp. The input

stage for the zero detection circuits can be seen in Figure 11. The only difference

between the input stages of the two zero detection circuits is the orientation of the biasing

diodes.

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Figure 11 - Zero Detection Circuit Input State [4]

SPICE simulations show that the input range created from the conditioning for the pre-

zero circuit is about -2 to 1V and -1 to 2V for the post-zero circuit. If the resistance is

chosen properly, the voltage input to the op-amp will not change greatly despite relatively

large variations in current.

3.6.2.4 Active Feedback/Middle Stage To provide noise immunity to the zero detection circuit, dynamic positive feedback is

employed with the op-amp output and the reference voltage. By providing noise

immunity, the op-amp won’t output multiple transitions if the input voltage rises too

slowly or if there is significant noise present. If multiple transitions were to occur

because of noise, severe degradation would been seen with respect to the accuracy of the

circuit. The middle stage of our zero detection circuit can be seen in Figure 12.

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Figure 12 - Zero Detection Circuit Middle State [4]

From an analysis of this stage, Vth, or the voltage on the positive terminal of the

op-amp has a relationship when there is a transition of:

Vth(t) = Vx + ∆Vz · e-t/RC (1)

A derivation of this equation can be seen in Appendix D.

This equation shows that immediately after a transition, the Vth jumps to (Vx+ ∆Vz), and

then decays back to Vx. When a transition occurs, Vth jumps out of the way to prevent

multiple transitions if there is noise on the signal or signal changes too slowly. After Vx

jumps by ∆Vz, it decays back to its original value without causing an extra, unwanted

transition. Equation (1) holds true for both circuits.

According to Equation (1), the time delay of the exponential decay depends on the

capacitor and resistor connected to the positive terminal of the op-amp. R and C must be

chosen to allow for the highest system frequency. If R is too small, the bias voltage, Vx,

will not hold true because of the large variation in current.

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3.6.2.5 Optoisolator/Output State To allow the zero detection circuits to interface with DSP I/O pins, the output signal will

be sent through a switching transistor and a Schmitt-triggered optoisolator. The

optoisolator conditions the voltage to hi/low voltage levels that can be used by the DSP

I/O pins. A big advantage of using the optoisolator to condition the voltage is that it will

also provide optical isolation for our zero-detection circuit from the DSP.

3.7 Protection

Protection is vital in a system such as this. When converting and controlling high power

signals with low power devices, like in this project, there needs to be protection to

prevent any part of the system from becoming damaged in the case of a fault or other

undesirable situation such as a voltage or current surge. For this design, protection will

be present in each stage, ensuring that each subsystem is adequately protected.

The Avista SR-12 fuel cell already contains internal protection circuitry. If there is

improper hydrogen flow into the fuel cell, it will automatically shut off. Internal circuitry

also monitors the load on fuel cell. If too much power is being produced by the fuel cell,

it will automatically disconnect the load from the system.

The DC/DC converter selected for this project also has its own internal protection

circuitry. There is internal monitoring that will detect overvoltage situations and

shutdown the converter. The DC/DC converter also has reverse polarity protection,

which will prevent a surge from coming from the AMPS and passing through the

interface design to the fuel cell.

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The DC/AC converter protection will be controlled by our DSP. The DSP will take

continuous voltage measurements from the AMPS; and, if there is a sudden change in

voltage, indicating a fault on the line, it will open all the switches on the DC/AC

converter—disconnecting it from the system. The DSP will also be taking zero-crossing

measurements continuously from signals outputted from the zero detection circuitry. If

there is a sudden change in phase, the DSP will also disconnect the DC/AC converter

from the system. Besides controlling the switches on the DC/AC converter, the DSP will

also control switches between the DC/DC converter and DC/AC converter, isolating the

two components.

The zero detection circuit is designed to withstand wide variations of voltage and current

on its input. The optoisolator, used to generate the signals from the zero detection

circuits for the DSP, isolates the two subsystems from each other, protecting the DSP in

case of an accidental surge through the zero detection circuits.

4 Validation

4.1 Fuel Cell To validate the functionality and capabilities of the fuel cell, a thorough set of load tests

were performed. The load tests ranged from open circuit to a maximum of just over

150W. These load tests showed the output voltage range to be approximately 18-36V

DC and the max output power to be just over 150W. When a bubble humidifier is

installed during the next phase of the project, these tests will be performed again and any

design changes will be made accordingly.

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4.2 DC/DC Converter A simulation of the DC/DC converter using PSCAD validated its theoretical operation.

The simulation data shows that by varying the duty cycle, the desired output of 12V can

be obtained regardless of the input from the fuel cell. This variation of duty cycle will be

automatically controlled using the proposed DC/DC converter discussed in this report.

4.3 DC/AC Converter The DC/AC converter was simulated using PSCAD and the PWM and three phase

outputs are shown in section 5.2.2 of this report. A second simulation, which includes

the DC/DC converter and a delta to wye transformer, was also performed to ensure

functionality of the system as a whole. The transformer successfully steps up the voltage

to 208V RMS and filters the PWM waveform from the inverter.

4.4 Zero-crossing Detection Circuitry Using a schematic provided by Dan Gordon, Ken Hollinger and Jon Leman [4], a zero-

crossing detection circuit was simulated using PSpice. This simulation utilizes pre-zero

and post-zero detection circuitry to successfully detect when zero crossings occur in the

voltage waveform. This circuit simulation will function properly if given a pure

sinusoidal input as well as a sinusoidal input with a high frequency ripple.

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5 Results

5.1 Fuel Cell Operating Procedure 5.1.1 Safety and Care of the Fuel Cell As with all combustible gases, care should be exercised when working with hydrogen.

Only operate the fuel cell with the doors open, and never leave the fuel cell unattended

for long amounts of time. The fuel cell contains delicate circuitry and sensitive

components that could be damaged if operated improperly. To avoid damage to these

internal components, always follow the operating instructions, and never allow current to

flow into the fuel cell from an outside source.

5.1.2 Startup Procedures The startup procedures for the fuel cell outlined in “Avista SR-12 PEM Hydrogen Fuel

Cell” [2] have been summarized here to provide a more thorough understanding of the

operation of the fuel cell. In order to start the fuel cell in a safe and timely manner,

perform the following steps:

1. Turn the main flow regulator on the hydrogen tank to a minimum. This

requires counter-clockwise rotation of the black knob.

2. Turn on the main valve on the hydrogen tank and adjust the regulator to 6 or 7

psi. A flow rate in excess of 7 psi will cause the fuel cell to abort the

initialization process.

3. Hold down the “POWER” button on the fuel cell until all lights turn green.

Release the button to start the initialization.

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4. Wait for the fuel cell to initialize and warm up. Once flow has started, this

should take less than ten minutes. When the status indicator reads “OFF-

LINE” the startup procedure has completed.

5. To switch in a load, press and briefly hold the “LOAD” button. Power will be

sent to the load, and the display will read “ON-LINE.”

5.1.3 Troubleshooting This section includes the troubleshooting procedure from “Avista SR-12 PEM Hydrogen

Fuel Cell” [2] as well as additional troubleshooting procedures that have been

encountered since the start of this current project.

Table 3 - Troubleshooting the Fuel Cell

Problem Solution

Unable to initialize fuel cell Low battery power: replace or charge the batteries

Unable to power a load for longer than approximately 3 minutes: Fuel cell shuts off and

no message is displayed.

Batteries are not supplying enough current to handle loading due to internal circuitry:

Charge the batteries.

Message “Low Voltage” is displayed.

The fuel cell has been overloaded. Reduce the load to less than 100 Watts and press

“LOAD” to reinitialize.

Message “Shutdown=7a” is displayed.

This message indicated that the fuel cell is going to shutdown. This message will occur if “POWER” is pressed or if hydrogen flow is

lost. If hydrogen flow is lost, readjust the regulator to 6 or 7 psi.

Some of the cell status lights are red.

This most likely indicates an overload condition. Reduce the load and press

“Cartridge Reset” to restore the offline cells. If this step is not performed, the fuel cell will

automatically shut down.

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5.2 Validation Results 5.2.1 DC/DC Converter As seen in previous sections of this report, the output voltage of the fuel cell varies from

18 to 36 volts. This requires a wide range voltage converter to regulate it to 12 volts. A

simulation of the DC/DC converter shows its general operation. Its duty cycle will be

automatically adjusted to obtain the required output voltage. This simulation data was

used to understand the operation of the DC/DC converter, so that the most efficient and

cost effective converter can be purchased during the next phase of this project. Figures

13 and 14 show the simulation results, along with the components necessary to construct

the buck converter.

Figure 13 - DC/DC Converter

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Figure 14 - DC to DC Converter Output

5.2.2 DC/AC Converter The DC/AC converter is required for this project because the fuel cell can only provide

DC current. The AMPS operates on three phase AC current. The DC/AC converter, as

shown in Figure 15, will invert the DC voltage by using an appropriate pulse width

modulation switching scheme to control a series of power MOSFETs. The use of power

MOSFETs ensures that the 200W specification will be met since these devices are

capable of several hundred Amps. The DC/AC converter was simulated using PSCAD

and the PWM and three phase outputs are shown in Figures 16 and 17. The results and

components modeled in the simulation will be used to determine the parameters for the

purchase of a DC/AC converter in phase two of this project. Note that the DC/DC

converter has also been connected to the inverter and a delta to wye transformer is

modeled on the output to step up the voltage to 208V RMS and filter the PWM waveform

from the inverter.

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Buck Converter DC to AC inverter

Transformer

Figure 15 - System Simulation Model

Figure 16 - PWM input: 1-Phase

Figure 17 - Three Phase AC Output

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5.2.3 Zero Detection Circuits In order to complete the interface process, the waveforms from the fuel cell must be

synchronized with the waveforms on the AMPS. This is a crucial part of the interface

design because, without synchronization, massive current spikes will be seen on the

system. In addition, the system will take a long time to stabilize if not properly

synchronized. Current spikes and instability would push the converters beyond their

limits, and would overload the fuel cell. This would result in system shutdown or, worse,

system damage. By utilizing the high-speed digital signal processor on the DC/AC

converter, current and voltage levels can be sampled frequently, and zero-crossing

detection circuitry can locate the synchronization points to provide near-exact matching

of the two system signals. This will ensure a smooth transition when switching the fuel

cell system onto the model power grid. The zero-crossing detection circuitry was

simulated using PSpice, and the results seen in Figures 18 and 19 will be used to

determine component values required to build and optimize the hardware during phase

two of this project. Figure 18 shows the voltage level trends on the input pins of the op-

amp for each of the two zero detection circuits. Figure 19 shows the output of the zero

detection circuit with a rising clock edge. A complete set of simulation results is outlined

in Appendix E.

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Figure 18 - Op-Amp Input Pin Simulation

Figure 19 - Zero Detection Circuits Output Switching

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5.3 Cost Analysis Table 4 shows the updated budget for our project. No parts have been purchased yet but

there have been some updates in prices for the parts. The cost of the DC/DC converter

has dropped significantly through research of a new supplier.

Table 4 - Budget

Item Price DC/DC Converter (if needed) $216 DC/3-Phase AC Converter $1,800 Transformer $125 Flyback Converter (if needed) $500 Hydrogen $45 Design Poster/Report Binding $15 Project Display Costs $35 Protection Circuitry $100 Filtering $50 Software Licenses $250 Miscellaneous $300

Total $3,436

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Bibliography [1] AMPS User Guide. University of Idaho. Moscow, ID. [2] Fletcher, Nathan. (2002, Mar). Avista SR-12 PEM Hydrogen Fuel Cell. University of

Idaho. Moscow, ID. [3] Nice, Karim. “How Fuel Cells Work.” How Stuff Works. 2000. Accessed: 6 April,

2005 <http://science.howstuffworks.com/fuel-cell.htm>. [4] Gordon, Dan., Hollinger, Ken., and Leman, Jon. “TNA Fault Controller.” Senior

Design Report, University of Idaho, 2001.

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APPENDIX

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Appendix A – ComPAC DC/DC Converter Data Sheet

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Appendix B – LF356 Op-Amp Data Sheet

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Appendix C – H11L1 Optoisolator Data Sheet

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Appendix D – Zero Detection: Circuit Analysis

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Appendix E – Zero Detection: Simulation

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Appendix F – Individual Project Contributions

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