Teaching Kids about Batteries and Photovoltaics George Hagerman © 1990 by George Hagerman Hiding in photo1 is the reflection of high-voltage transmission lines that carry nearly 1400 megawatts to heavily populated northern Virginia. This image captures the energy choices facing today's youngsters in an increasingly populous and resource-scarce world. Disposable or renewable fuels? Centralized or distributed generation? Next century's energy picture will be shaped by this decade's school children. Not all will be utility or government planners, but all will be energy consumers and voters. Will they have the knowledge to make wise choices, or even to ask the right questions? INSERT PHOTO 1 Photo 1. Student-built battery chargers reinforce the principles learned in this course. Photo by George Hagerman. Some are asking questions now! An unexpected result of my free, one-line listing in the Yellow Pages has been a small but steady stream of requests for help on school projects. Last year, after getting three calls in one week, I invited parents and their kids to my office to show them some solar basics and discuss their ideas. One young lady proposed to compare the cost of producing hydrogen from electrolysis of water by solar energy and by batteries. She borrowed a 2- watt panel and did a fine job on her project. A sixth-grader decided to build a miniature home power system - a small cardboard house, a penlight bulb, two rechargeable AA cells (in series), and two 6V/50mA mini-panels (in parallel) on the roof. Well all this inspired me greatly, and I began to realize that if we're going to stop the destruction of this planet, education is where it's at. Then I received a call from Lucy Negron-Evelyn. The El Ingeniero Program Lucy is Executive Director of Non-Profit Initiatives, Inc., in Silver Spring, Maryland. Each year she conducts a summer program called "El Ingeniero". This is a six-week course for gifted Hispanic-American junior high school students, funded by NASA as part of an effort that encourages minorities to pursue careers in engineering. The main focus of El Ingeniero '89 was hydraulics, but Lucy asked if I could spend a few days teaching the kids about solar energy. Jumping at the chance, it was soon apparent that I had much to learn. This article attempts to pass on some of the lessons. Overall Approach The course consists of two main activities. Through lectures and experiments, the students learn the relationship between solar cells, batteries, and electrical loads. They learn about the design process that determines the proper size, number, and arrangement of these components. This process is the same,whether you are powering a portable tape player, a remote weather station, an orbiting satellite, a house, a village medical clinic, or even a whole community of homes and businesses. As a second activity, each student designs and builds a battery charger for their favorite battery-powered gadget. This is something that they can use the rest of their lives, daily reinforcing the principles learned from lectures and experiments. It is also a solar energy application that will save most students the cost of 50-100 disposable batteries each year! Although the environmental advantages of this are significant and important, it really hits home when you can reach these kids in terms of their weekly allowance. This article focuses on the lectures and experiments. The design, construction and performance of the battery chargers built by El Ingeniero '89 will be detailed in the next issue of Home Power. Building the charger can be a course all by itself, as can the series of lectures and experiments. The course is more effective if both activities are combined, but lack of equipment or budget may make this impossible. The lectures and experiments are presented here in six sessions, but this may have to be modified to fit a particular teaching schedule (e.g. regular school session vs. summer workshop). This article describes the course not as I taught it, but as I would teach it again. It was my first teaching experience, and there are many things I'd do differently. Several new experiments have been added, and although not yet used in a classroom, all have been thoroughly tested to be sure they work. Session 1 - Lecture on Batteries and Loads The sun's rays are not always available when you need the power. A reading lamp connected directly to a PV panel is a useless item. The concept of battery storage is fundamental to the application of solar energy (or any other intermittent resource). Given the hydraulic focus of El Ingeniero '89, electrochemical storage cells were introduced to the class as little tanks of water. Voltage is analogous to the water's height (pressure), and capacity is analogous to the tank's volume. Electric current is analogous to the flow of water out of the tank, through a valve which represents the load. As the cell discharges, the tank drains, and the water level (cell voltage) drops - slowly for a small load (nearly closed valve), quickly for a large load (nearly open valve). The size of a cell (AA, C, D, etc.) is related to its capacity, not its voltage. This fits the water tank analogy, since a AA cell and a C cell are about the same height, but the C cell is significantly fatter. Cell voltage is related to the nature of the electrochemical reaction - 1.5 volts for zinc-carbon, and 1.25 volts for nickel-cadmium. This is an opportunity to take some of the mystery out of what goes on inside a battery. Soak a piece of paper towel in lemon juice and sandwich it between a nickel and a piece of aluminum foil. This nickel-aluminum (Ni-Al) cell will develop an open-circuit potential of about half a volt. What's happening? When dissimilar metals are "bridged" by an acid or alkaline solution, chemical reactions cause one metal to develop a positive charge, the other a negative charge. The negative charge is a build-up of free electrons, and depends on the metals involved. For example, a nickel-iron (Ni-Fe) cell has twice the voltage of a Ni-Al cell, which can be shown by replacing the aluminum foil with a steel washer. The nickel-cadmium (Ni-Cad) reaction is reversible, and Ni-Cad cells are rechargeable. The discharge curves (voltage vs. capacity) for zinc-carbon, alkaline, and Ni-Cad cells are compared. Zinc-carbon and alkaline cells do behave like little cylindrical tanks of water - as the cell drains, voltage drops almost linearly. Ni-Cad cells behave more like hollow-stemmed wine glasses - very little change in voltage until the cell is almost empty, and then voltage plummets as the last bit of water drains from the glass stem. The electrical consequences are explained for something like a flashlight. Zinc-carbon or alkaline cells will give early warning of their demise as the light gets gradually dimmer. With Ni-Cads, you get a nice bright light throughout most of the cells' life, and then, poof ... sudden death. The mathematical relationship between battery capacity, current drain, and discharge time is explained, as is the meaning of a "C" or "C/5" rate. A chart is drawn on the board showing the capacity of different Ni-Cad cells. Simple questions are offered - "If two D cells are used in a flashlight that draws 800 mA, how long will they last?". Finally, the class is shown how individual cells can be connected in series (add voltages, same capacity) or parallel (same voltage, add capacities). It is explained how a certain threshold voltage is required to operate any given load. Returning to our simple Ni- Fe cell, switch off the classroom lights and show how four in series (Photo 2) have enough voltage to power a light-emitting diode (LED). The class should be able to guess how many Ni-Al cells are required to produce the same LED brightness. INSERT PHOTO 2 Photo 2. A four-cell Ni-Fe battery made from nickels, steel washers, and a weak acid electrolyte (vinegar also works). When the bent wire of the LED shown in the photo is touched to the face of the terminal nickel, it lights, and the voltage drops to about 1.8 volts. Stacked next to the Ni-Fe battery are eight Ni-Al cells in series, fashioned from nickels and cut square pieces of aluminum pie plate. Photo by George Hagerman. It should be emphasized that the ability to develop adequate voltage depends only on the number of cells in series, and not their size. For example, a tape recorder takes four fat C cells - will it run off four tiny AAA cells? The kids may be skeptical, so set it up in front of the class. Sure enough, tunes start to emanate from the machine. The digital multi-meter used earlier can now be used to show a current drain of about 140 mA. Judging from the chart on the board, how long are those AAA's going to last? Should the kids use a "C" or "C/5" rate to calculate the answer? If Session 1 is in the morning and Session 2 is in the afternoon, have the students listen to the tape recorder during lunch and see if it stops when they predicted it would. Session 2 - Experiments With Batteries and Loads Six experiments are set up at different locations in the room. The students should work in groups of two or three. This way they can help each other and talk about what they are doing. If the groups are too large, then the quickest kids will do all of the "hands-on" work, while those that are slower, or more shy, hold back. Another way to ensure active participation is to give each student a work sheet. This has specific questions for each experiment, which can be answered only if the student DOES something, like changing a wiring connection and reading a meter. With only six experiments and 25 kids working in pairs, they can't all be occupied at once. One solution is to divide the class in half, with one group working on experiments, and the other on building their battery chargers. Then half-way through the session, the two groups switch. The six experiments and the principles they demonstrate are described below. Component wiring connections are illustrated in Figure 1. Parts access is given at the end of this article. Many of these components are reused in the photovoltaic experiments shown latter photos. INSERT FIGURE 1 Experiment BL1 demonstrates the different discharge characteristics of Ni-Cad and zinc-carbon batteries, and the difference between open-circuit and loaded voltage. It requires six AA Ni-Cads, two of which are fresh, two of which are half-discharged, and two that are dead. Six zinc-carbon cells, at comparable states of charge, are also required. Mark the cells with letters or numbers ahead of time, but don't tell the kids which marks go with which states of charge - they should determine that from voltage and/or load behavior. A low-drain load, like an AM radio, can be used for comparison with the high-drain lamp. Experiment BL2 demonstrates the importance of connecting loads in parallel rather than in series. The current drains of submerged and dry pumps should be measured when they are individually in circuit, then together in series, and finally together in parallel. When in series, the dry pump acts like a bottleneck, limiting the amount of current flowing through the circuit, thus reducing the output of the submerged pump. This also shows that a loaded motor draws more current than a free-spinning one. Experiment BL3 demonstrates the difference in current drain between a motor starting from rest and one already running. Starting current will always be more than running current, and depends on where the motor comes to rest (relative position of magnets, windings, and such). This is of considerable importance for motors that may be powered directly off photovoltaic panels, which are current limited. Examples include fans for venting cars or attics, and pumps for delivering water to irrigation systems. Experiment BL4 demonstrates the effect of voltage on motor speed. As a load, the motor may be considered a valve for electrons. When the voltage (or electron pressure) is increased, more electrons flow through the valve per unit time. As long as the mechanical load on the motor doesn't change, this greater flow of electrons results in more speed. Stall the motor, and the valve opens wide, draining the battery. Experiment BL5 demonstrates the effect of wire resistance on voltage drop. Again, the flow of electrons in a wire may be likened to that of water in a pipe. Electrons start their trip at a cell's negative terminal with a certain amount of potential energy (voltage), which is converted to other forms (heat, light, sound, shaft horsepower) as they travel through the circuit. This potential energy is completely lost by the time they reach the cell's positive terminal. Ideally, very little energy should be lost as they flow to and from the load. If the pipe (or wire) is too small, significant amounts will be lost to friction (heat), and not as much will be available to operate the load. When all four spools of wire are in circuit, two additional Ni-Cad cells are required to properly operate the load. Replace any one of these six good cells with a dead Ni-Cad. This shows how a "dead battery" may result from only one bad cell. Experiment BL6 demonstrates the effect of mechanical loading on the current drain of a motor. Most motors don't spin freely, but do work like lifting weights, pushing vehicles, and moving air or water. This experiment uses a commercially available motorized game that lifts little plastic dolphins to the top of a spiral track. They roll down to the bottom, where they are picked up by a slowly spinning wheel and carried to the top again. The wheel spins behind a cardboard sheet. Magnets on the wheel rim pick up the dolphins, which have small magnets on their sides. As the dolphins slide along the cardboard on their way to the top of the track, friction loads the motor, causing an 80 mA. jump per dolphin. These "leaping" dolphins are fun to watch and teach an important principle that applies to many practical situations: an electric winch lifting a heavier weight, a solar car driving up an increasingly steep hill, or a pump filling a higher reservoir. In all cases the current drain will increase. If the voltage source can't deliver any more current, then the rate of lifting will slow, the car's speed will drop, and a sea-level gusher will turn into a mountain-top trickle. Session 3 - Lecture on Photovoltaics Placing photovoltaics into context with other renewable energy technologies requires a brief overview of the four main methods for directly harnessing the sun's rays. These are passive solar heating (via solar building design), active solar heating (via special collectors for air or water), solar thermal electric (parabolic reflectors producing high- temperature steam running turbine/generators), and photovoltaics (direct conversion of photon energy into electron potential). Because wind is a result of unequal heating of the earth's surface by the sun, and waves are generated by wind blowing over water, these are also forms of solar energy. The photovoltaic (PV) effect is explained very simply: when light strikes a PV cell, it "kicks" electrons up to the surface layer from a deeper layer. Just as the voltage of an electrochemical cell depends on the two metals involved, the potential energy developed by a PV cell depends on the material composition of its upper and lower layers. The characteristic potential of silicon-based PV cells is about half a volt. At low levels of illumination (say on an overcast day), the voltage of a PV cell depends on the intensity of light striking its surface, but over most of its useful operating range, voltage varies only slightly with light intensity. On the other hand, the amount of current delivered by the cell depends strongly (and linearly) on light intensity. (the number of photons arriving per unit area per unit time). No matter how much potential energy it has, an electron cannot leave the cell's surface until a photon arrives to "kick" another one up from the lower layer to take its place. An electron also can't leave if it doesn't have anywhere to go, so in an open circuit, electrons "kicked" up by newly arriving photons fall back into the lower layer, until a circuit is completed. Open circuit PV cells behave much like electrochemical cells. Connected to a load their behavior is markedly different. For the power drains used here, a Ni-Cad cell's ability to deliver current is unlimited. A tiny AAA cell can deliver as much current as a big bad D cell; not for nearly as long, but it can still deliver. The current delivered by a PV cell is limited by the rate of photon arrival. Therefore, except when very lightly loaded (almost closed electron valve), the PV cell is a constant-current source. The current flowing through a medium load (half-open electron valve) is almost the same as that flowing through a short circuit (wide open electron valve). No matter how open the valve is, the rate of electron flow (current) is governed by the rate of photon arrival, which is the product of cell area and light intensity. Light intensity is affected by shading and angle of incidence. If photons are absorbed or reflected by the atmosphere, clouds, tree branches, or glass, then their rate of arrival at a PV cell is reduced. Even if there is nothing between the cell and its light source, the light intensity is affected by the angle at which light strikes the cell's surface. This can be illustrated on a chalkboard by drawing a beam of parallel rays striking a plane at various angles of incidence. Thus, less solar energy reaches the earth's surface during the winter; not only because the days are shorter, but also because the sun is at a lower angle in the sky. This reduces the angle of incidence and also means that the sun's rays have to pass through more of the atmosphere. Just as a battery is a series/parallel combination of electrochemical cells, a solar panel is a series/parallel combination of PV cells. Panel voltage, like battery voltage, can be increased by wiring cells in series. Wiring PV cells in parallel increases the amount of current that the panel can deliver under a given light intensity, having exactly the same effect as increasing the cell's area. At this point, break out a bunch of different PV cells and panels. The cells (protected in clear plastic boxes) can be handed around the class. Note the grid of fine wires on the cell's surface, which collects electrons "kicked" up by the light. This is the negative terminal. The metal surface on the back side of a cell is it's positive terminal. Briefly describe the different silicon cell types: single crystal, polycrystalline, and thin-film. Have the kids look at the panels. Can they distinguish series and parallel cell connections? If it happens to be sunny outside, show that panels of the same size may be high-voltage/low-current or low-voltage/high-current. What does this imply about series vs. parallel cell wiring? Also if you can get outside, demonstrate the constant-current feature of PV panels. Using the same tape recorder that drew about 140 mA from the Ni-Cad cells, connect a PV panel to its battery compartment terminals. Show the effect of tilt angle. Hold the panel at an angle just above the threshold at which the tape slows noticeably. Have one of the kids move the jumper cables from the tape recorder to a current meter, and note the short-circuit current. Can they guess beforehand what it will be? At lesser angles of incidence, the rate of photon arrival doesn't send enough electrons around the circuit to operate the load, eventhough its electron valve is open enough to accommodate them. Tape recorders are great for showing all sorts of things. More importantly, if you put on a tape with tunes that the kids know, you'll grab their attention immediately. There's nothing like a little "Straight Up" by Paula Abdul (from Forever Your Girl, copyright 1988 by Virgin Records America, Inc.) to get feet tapping. PVs should make you feel like dancin'! Session 4 - Experiments With Photovoltaics This is the one session that must be held outside on a bright day. What is bright"? If you can see sharp edged shadows on the ground for at least five out of every ten minutes, then all of the PV experiments will work. Experiment PV1 demonstrates that decreasing light intensity strongly affects current output, but it has little effect on voltage except at the lowest illumination levels. First, the panel is tilted at various angles, such that the students can collect enough data points to plot open-circuit voltage vs. short-circuit current. The panel is then returned to a position that is perpendicular to the sun's rays, and the effects of increasing cloud thickness are simulated by placing one, two, or three layers of translucent white foam over the panel. Are transmission efficiencies of multiple layers additive or multiplicative? Finally, a piece of opaque cardboard is used to completely shadow a portion of the panel. It has different effects, depending on whether it is oriented vertically or horizontally. Experiment PV2 demonstrates that if just one cell in a string of series cells is completely shadowed, then it develops a high resistance, causing a large voltage drop when the panel is under load. In this way, it has the same effect as a dead electrochemical cell in an otherwise good battery. The panel shown I used evidently has a few cells that are not of such high quality, since Paula still played up to tempo when one of these lesser-quality cells was shaded. Partially shading many cells in the panel has much less effect than completely shading just one good cell. Since even a single bare branch can cast a shadow large enough to cover an entire cell, the moral of the story is: avoid trees, and be particularly sure that they won't shade the panel in winter, when shadows are longest. Experiment PV3 simulates a solar powered irrigation system and the effect of starting vs. running current on system operation. Orient the panel so it is perpendicular to the sun's rays. Tilt the panel back until output from the pump stops just shy of the tip of the clear plastic tubing that comes with the pump. Note the angle, and tilt the panel back even farther, so that the sun "sets" completely, and the pump motor stops. Now slowly raise the panel to the angle noted earlier. Depending on what position the pump motor came to rest, it may be that there is not enough PV current to start the pump motor. The angle of incidence may have to be much higher, and it will be much closer to "solar noon" before the system starts to operate. If you want to keep the experimental set-up dry, it is better to use something deep like a cottage cheese container, rather than the shallow bowl shown in the photo. The clear plastic tubing should be duct-taped to the inside wall of the container, so that the pump is held level. Experiment PV4 demonstrates the effects of parallel and series connection of individual PV cells. First, short- circuit current and open-circuit voltage are measured. Then a submerged pump is connected, and it will be seen that wiring the PV cells in parallel has no effect on pump output, but wiring them in series does. This reinforces the principle already shown with batteries, that increasing voltage increases motor speed for a given mechanical load. Now connect a dry pump in parallel. Do the students recall why not in series? If the light intensity is high enough, it can be seen that the second pump will have no effect on the first one's performance as long as both are running smoothly. If the dry one is stalled by stopping its impeller with a toothpick, the output of the other pump drops dramatically. If current delivery is limited (as it is with PVs), and one valve opens wide (stalled motor), most of the electrons will take the path of least resistance, leaving the other load without adequate current. Experiment PV5 demonstrates that PVs can recharge Ni-Cads, and that current into the Ni-Cad equals current out (or very nearly so). The procedure is as follows. First, a dead Ni-Cad is connected to a motor, which has a 4.4-ohm resistor across its terminals so that it will only run for a few seconds on the "rebound" voltage of the dead Ni-Cad. The motor I used draws 10 to 15 mA at 1.2 volts without the shunt resistor, 100 mA with it. The Ni-Cad is then charged for two to four minutes, depending on sky conditions. The trick here is to continuously adjust the tilt of the panel, so that the charging current remains at exactly 50 or 100 mA. By casting a "weather eye" to the sky during this period, the student can anticipate upcoming tilt adjustments and will start to gain a feel for the effects of clouds and angle of incidence on PV output. The newly charged battery is then connected to the motor, again monitoring the current flow. A watch with a second hand (or digital second counter) is used to measure the time it takes the current to drop from 100 mA to 95 mA (it will plummet very quickly after that, and the motor will stop; the student should then switch the rotary dial on the current meter to "OFF" in order to avoid excessive discharge of the Ni-Cad). Experiment PV6 demonstrates the effect of PV voltage on how much charging current flows through a battery. It also demonstrates the need for (and the energy cost of) a blocking diode. First, the battery open-circuit voltage is measured, as well as the open-circuit voltage and short-circuit current of six, five, four, three, and two PV cells in series. This should be done with and without the diode. The diode can be taken out of circuit simply by clipping the jumper cable below, rather than above, the barrel of the diode, as shown in the photo. Then, battery charging current is measured for each of the different numbers of PV cells. This should be done without the diode first, so that the negative current flow (battery discharging into PV cells) can be seen for the two-cell configuration. Then the diode is placed in circuit, and it can be seen that this acts like a one-way valve to electron flow. As the student works back up to six PV cells, it will be seen that there is a price to be paid for this protection. Session 5 - Quiz & Session 6 - Wrap-Up Painful as it may seem, this is the best way for you to learn what you taught, rather than what you think you taught. Try to set up test problems that force the students to apply the principles that they have learned. You may even want to base these on some additional experiments. Should the students be told ahead of time, so they can study for it? Although surprise quizzes are not popular, they probably are a better measure of the actual working knowledge of a student. On the other hand, reviewing for a test is a valuable learning exercise in itself. What to do? Toss a coin. Return the quiz during session 6 and review any class-wide weak points. Open the floor for discussion. You may also want to hand out materials for further reading. These can include ideas for science fair projects. Access - Experimental Equipment The components needed to setup the experiments described in this article are specified in Table 1. It should be noted that some components (500mA. PV cells, 0-5 VDC meter, 0-1 Amp. meter, and motor with color wheel, all shown in the photos) came from a "Photovoltaic Demonstration Kit" made by Solarex Corporation (# ES 602073005), which is no longer available. Therefore, other sources have been located for these components. The 500 mA. solar cells are really too large, but I used them because they came with the Solarex kit. A better choice for experiment PV4 would be a 300 mA. cell. Bare cells require soldering, whereas the encased cells have wire lead already installed. The best choice for experiment PV6 are encased 100mA. cells. One advantage of these cells is that an inexpensive Radio Shack multimeter can be used in place of the high priced 0-1 Amp. meters. It is important to select a meter that has a large enough range to measure the maximum expected voltage or current, yet not so large that only tiny needle movements result from experimental manipulations. The 0-5 VDC meter is ideal for experiments BL1, BL5, PV4, and PV6, but is expensive. Not as good, but cheaper, is the Mitchell Instruments multimeter specified in Table 1. A 0-1 Amp. meter is specified for experiments BL1-2, BL6, and PV4, because this came with the Solarex kit. A 0-500 mA. range would be better. A possible source for inexpensive 0-5 VDC and 0-500 mA. panel meters Prime Instruments. At ten to fifteen dollars per meter, the price is right, but it was not possible to test them in time for this article. The 15mA. DC motor specified in Table 1 is a close duplicate of the Solarex kit motor, but it is not well matched to the 0-150 mA. meter. A better choice may be the 80 mA. motor, but this has not been tested. Regardless of motor, be sure to buy either color wheels or propellers, so students can plainly see changes in motor speed. For one dollar, Solar World sells a package of three color wheels with shaft adaptors or two friction-fit propellers. The Edmund DC pump at 2.5 Volts (experiment BL2) draws 120 mA. dry , 360 mA. submerged, and >800 mA. stalled. At 1.0 Volts (experiment PV4), it draws 90 mA. dry, 180 mA. submerged, and >300 mA. stalled. If you would like to design other experiments using different sizes of PV cells, try Solar World (10 to 650 mA. output) or Astropower (2.0 A. output). A good paperback text for high school or college students is The Solarex Guide to Solar Electricity. Although out-of-print, Solar George has a large stock of these for sale five dollars each (less in volume). Even more intriguing to the educator, Solar George has developed a 36-cell, 5-watt, "build-your- own" panel kit, which retails for about $35.00. Access - Other Ideas for Energy Education Here is a short, but by no means exhaustive, selection of materials that I've come across. They each have a different focus, as described below. Solar Energy Experiments for High School and College Students, by Thomas W. Norton, copyright 1977, Rodale Press, Emmaus, PA. Most of the experiments are concerned with solar heating, although some interesting exercises in solar astronomy and measurements are also included. Energy Education Guidebook, prepared by Design Alternatives, Inc. of Washington, DC, under contract to the Community Services Administration. It is available from the National Appropriate Technology Assistance Service (NATAS), P.O. Box 2525, Butte, MT 59702, tel. (800) 428-2525 (in Montana, dial 800-428-1718). This book describes a variety of projects, including some other renewable technologies, like a small wind generator and a simple bio-gas digester. NATAS can also provide an extensive bibliography of other energy education materials and resources. The Florida Solar Energy Center, in cooperation with the Governor's Energy Office, has prepared the Florida Middle School Education Project, which describes a variety of classroom, homework, and experimental activities dealing with energy production, consumption, and conservation. It is available from the Public Information Office, Florida Solar Energy Center, 300 State Road 401, Cape Canaveral, FL 32920, tel. (407) 783-0300. Finally, Jim Masker, who teaches at a private school in California, has developed his own short course in photovoltaics, including among other things, a solar-powered boat race across a swimming pool, and the design of a "home power" system for a dormitory room. He has also put together a self-contained kit (including an intense light source) for PV experiments. Descriptions of both are available from Jim Masker, Cate School, P.O. Box 5005, Carpinteria, CA 93013, tel. (805) 684-4127. Jim and I have been discussing the possibility of convening a short workshop at the Willits Energy Fair, where energy educators could get together, share ideas from their "bag of tricks", and brainstorm some new ones. If you've had experience teaching kids (or adults) about energy, and would be interested in attending such a workshop, then please contact either one of us. George Hagerman, SEASUN Power Systems, 124 East Rosemont Ave., Alexandria, VA 22301,telephone 703-549-8067. Acknowledgements First, I'd like to thank Richard and Karen Perez for their encouragement, patience, creative layout, and meticulous editing. Their input was invaluable. Many thanks also to Michael Meredith, a neighbor here in northern Virginia (see his Micro Ad), who definitely has the talent to put together a short course in solar thermal electricity. He loaned me a 12-inch multi-faceted parabolic mirror that fascinated the kids. A coil of copper tubing is located at the mirror's focus, such that when water is slowly fed through the coil, a puff of steam comes out the other side. Truly ingenious! I'd also like to thank Dr. John Wohlgemuth, who arranged a special tour of the Solarex Technical Center in Frederick, Maryland, where students could see how silicon is turned into solar cells and panels. The tour was well-organized and quite impressive. Last, but certainly not least, I'd like to thank Lucy Negron-Evelyn for giving me the opportunity to teach the students of El Ingeniero '89. These kids were wonderful, and their attentiveness and eagerness to learn convinced me that batteries and photovoltaics were not "too technical" to teach at the junior high school level. Their positive response and hard work inspired me to really polish the course, as it is presented here. I'm only sorry that I can't teach them again. Assistant Instructor, Edgar Hurtado, helped in a variety of ways, as did Lucy's teaching assistants: Alan, Rosa, and Janet. Thanks guys!! Supplier Access AEE Alternative Energy Engineering POB 339 Redway, CA 95560 707-923-2277 ¥ 800-777-6609 All Electronics Corp. POB 567 Van Nuys, CA 91408 818-904-0524 ¥ 800-826-5432 Astro Power 30 Lovett Avenue Newark, DE 19711 302-366-0400 Chronar POB 177 Princeton, NJ 08542 609-799-8800 Edmund Scientific 101 E. Glouchester Pike Barrington, NJ 08007 609-573-6250 Mitchell Instrument Co. 1570 Cherokee St. San Marcos, CA 92069 619-744-2690 Prime Instruments, Inc. 9805 Walford Avenue Cleveland, OH 44102 216-651-0400 Radio Shack 500 One Tandy Center Fort Worth, TX 76102 817-390-3011 Randix Industries Ltd. Granite Park, Fortune Blvd. Milford, MA 01257 508-478-8989 Solar George George Newberry POB 417 Big Pine Key, FL 33043 305-872-3976 Solar World 2807 North Prospect Colorado Springs, CO 80907 719-635-5125 Solarex Corporation 1335 Piccard Drive Rockville, MD 20850 301-948-0202 Spencer Gifts 1050 Black Horse Pike Pleasantville, NJ 08232 609-645-3300 Yokagawa Corp. of America 2 Dart Road, Shenandoah Industrial Park Newnan, GA 30265 404-253-7000