Chapter 4 Modeling and Thevenin Equivalency 41 CHAPTER 4. MODELING AND THEVENIN EQUIVALENCY 4.1 Section Overview In this section a solar cell is examined. A solar cell is a non-ideal voltage and current source that can be modeled as a Thevenin equivalent circuit. Solar cells are an interesting class of energy sources because they do not produce energy in a linear fashion over all current and voltages. Instead every solar cell has a ‘sweet spot’ that gives the most power (remember power is voltage times current, P = V ∗ I) 4.2 Preparation In preparation for this lab, review the concept of the Thevenin equivalent model. 4.3 Procedure In this section, the following items will be covered. 1. Differential Measurements 2. Taking Measurements 3. Graphing Non-ideal Energy Sources 4.3.1 Differential Measurements To be able to plot power supplied by the solar cell, the current sourced by the cell must be determined. The DataLogger can only measure voltage, but current through an element is proportional to the voltage dropped across it. By using a fixed value resistor in the circuit and Ohm’s law, current can be found. To take measurements of the solar cell, begin by constructing the circuit in Figure 4.1. Do not connect the DataLogger to the circuit until it has been verified. The solar cell can supply enough energy to damage the DataLogger if it is not properly connected. Pay special attention to the orientation of power and ground pins! Figure 4.1: This circuit is used to characterize a solar cell Solar Cell Background The power generated by a solar cell is proportional the amount and type of light it is exposed to . In commercial solar cell production, a characterization process is conducted on every cell using a specific calibrated light source that 42 ENGR 201 Manual c �2010 Oregon State University 4.3. PROCEDURE closely matches the sun in spectrum and has a fixed intensity per unit area. These calibrated light sources can be very expensive but a basic understanding of the cells can be found using other light sources. For this experiment a traditional tungsten filament incandescent light bulb will be used. This light source is inexpensive and available but has more yellow and red in its spectrum compared to sun light. This change will result in a deviation from the specification of the solar cell from its manufacturer. The intensity of light striking a solar cell correlates to the voltage of the solar cell while unloaded. This means that a solar cell without much resistance attached to it will increase its output voltage when exposed to more light. Solar cells are designed with an upper voltage range and the voltage will not increase past this amount. This is important to note since the DataLoggers can only measure voltages of up to 3.3 volts approximately and could be damaged by too much voltage! Set the solar cell under the source so that the intensity of the light can be adjusted as in Figure 4.2. Figure 4.2: This setup is used to test the solar cell 1. With the DataLogger disconnected from the circuit and the potentiometer adjusted to 5K ohms, adjust the height of the light source so that there approximately 3.3V observed at the point ‘Input 1’ in Figure 4.1. 2. Once the solar cell is calibrated, vary the resistance of the potentiometer in the circuit to reduce its resistance. This reduction will cause more current to flow and the power supplied by the cell to change. Use caution, increasing the resistance at ‘Input 1’ could increase the supplied voltage and damage the DataLogger. Be sure to know which way to turn the potentiometer! 4.3.2 Taking Measurements 1. Configure the DataLogger to take 10 measurements per second (or more). Enable logging on both channels. 2. Connect the DataLogger to the circuit as shown in Figure 4.1. Switch the switch to run and begin sampling. 3. Reduce the resistance of the potentiometer slowly (taking approximately 10 seconds). The DataLogger will record these samples. Dump the data to a file and open it in Excel for inspection. 4.3.3 Graphing Non-ideal Energy Sources In order to analyze how the solar cell supplies energy, it is important to apply Ohm’s law and the equation for power before examining the results numerically and graphically. Include the following graphs for a thorough analysis: VIN P U T 1 , VIN P U T 2 vs. time ILOOP vs. RLOAD (RP OT + RF IXED ) c �2010 Oregon State University VIN P U T 1 vs. RLOAD (RP OT + RF IXED ) VIN P U T 1 vs. RLOAD (RP OT + RF IXED ) ENGR 201 Manual 43 CHAPTER 4. MODELING AND THEVENIN EQUIVALENCY The final outcome of this data manipulation should be the graph of load resistance on the x-axis, and power supplied on the y-axis. This includes using the compiled information to determine at what load resistance, optimal power is supplied. P = VSOLAR ∗ ILOOP (4.1) VP OT = VIN P U T 1 − VIN P U T 2 (4.2) ILOOP = VIN P U T 2 R2 (4.3) (4.4) VSOLAR = VIN P U T 1 Look at the scales of the graphs to ensure that the values are correct. The graphs should indicate that when power (P ) vs. either ILOOP or VSOLAR that there is a local maxima or minima that shows the sweet spot for using the solar cell. If this is not present, redo the experiment ensuring that the potentiometer is varied properly and that the same light is supplied to the solar cell during the entire test. 4.4 Lab Report Write a clear and concise report. Turn in the typed report following the second week of this lab. The report should include the following: 1. The type of data collected, where it was collected, and any conclusions that can be drawn from the data. 2. As mentioned previously include the following graphs: VIN P U T 1 , VIN P U T 2 vs. time ILOOP vs. RLOAD (RP OT + RF IXED ) VIN P U T 1 vs. RLOAD (RP OT + RF IXED ) VIN P U T 1 vs. RLOAD (RP OT + RF IXED ) 3. Any graphs that might help to display changes in measurements. 4. A schematic drawing of the sensor circuit used (using LTSpice or a similar program). 5. A simulation output showing the output voltage of Input1 , Input2 , and the power supplied by the source. Use the ‘Simulating a non-ideal voltage source’ tutorial found on the lab website as a reference. 6. A diiscussion of the differences between a linear and non-linear source. 7. Properly labeled graphs with titles, correct axes and correct scale. 8. A written explanation of the graphs and the data received (along with equations that were used to calculate final and intermediate values). Be aware that there is some error in the DataLogger measurements. Current guidelines and an example lab report are available on the lab website. 44 ENGR 201 Manual c �2010 Oregon State University