Download The RC Circuit and Time Constant Lab Report and more Lab Reports Physics in PDF only on Docsity! The RC Circuit & Time Constant Lab Report 007 Professor Todd R. Gelbord Report Written By Galib F. Rahman PHYS 1442 Section D783 November 10, 2017 Table of Contents Objective 3 Theory 3 Charging a Capacitor 3 Discharging a Capacitor 4 Materials 4 Procedure 5 Data 7 DataStudio Graphs 7 Logarithmic Graphs 8 Table 10 Computations & Source of Error 11 Questions 11 Conclusion 11 Procedure First we constructed the circuit as shown below: We set the power supply voltage to 3.9 Volts and the resistance ,R, to 1000 Ω. The voltage sensors are connected to the PASCO CI-750 Science Workshop® 750 Interface, such that the voltage across the resistor is connected to the analog input Channel A and the voltage across the capacitor is connected to the analog input Channel B (as highlighted in the picture below). After the circuit we built, was approved, we proceeded to connect the sensors to DataStudio and initialized tables for both channels alongside their corresponding graphs. Next, we began the charging process of the capacitor, by moving the SPDT switch to position 1 (as shown in the schematic below), while simultaneously initiating the collection of data from the sensors in DataStudio. We terminated the data collection once the voltage of the capacitor reached the same magnitude of the output voltage, ε. Charging Phase To begin the discharging phase of the capacitor, we moved the switch to position 2(as shown in the schematic below), while simultaneously initiating the data collection from the sensors in DataStudio. Discharging Phase We terminated the data collection once the voltage of the capacitor decreased to zero. Data DataStudio Graphs Run 001: Charging phase of Capacitor Run 002: Discharging Phase of Capacitor Channel A: Resistor Channel B: Capacitor Table Input Voltage ε= 3.9 V Resistance R=1000 Ω Capacitance C= 3.82 mF Slope from the graph for the charging process Slope= -0.2233 s-1 Time constant for the charging process 𝛕= -1/Slope 4.48 s Slope from the graph for the discharging process Slope=-0.2233 s-1 Time constant for the discharging process 𝛕= -1/Slope4.48 s The average value for the time constant 𝛕=4.48 s % difference= 0% Time constant 𝛕=RC 𝛕=3.82 s % difference= 15.9 % Computations & Source of Error [All graphical computations were performed on Excel] Sample Percent Difference Computation One possible source of error, is the resistance of the wires utilized in the construction of this circuit. In our calculations of RC the only resistance accounted for was the resistance of the resistor box. Thus, additional, potential resistance may affect the accuracy of the data collected. Questions 1. Show that the product RC has a dimension of second when R is in Ohms and C is in Farads. 2. Figure 10.5 shows plots of VR(t) (dotted line & solid line) for two capacitors that separately discharge through the same resistor. Rank the plot according to the capacitance of the capacitors, with the greater one first. The greater the time constant is, in magnitude, the longer it takes for the capacitor to charge and discharge. Since the time constant, 𝛕, is equal to the product of the resistance, R , and capacitance, C , the “un-dotted” curve represents the discharging curve of the capacitor that has greater capacitance, in this case. On the other hand the dotted curve, which approaches zero at a faster rate, is representative of the discharging capacitor with the lesser capacitance. Conclusion In this experiment, we constructed a RC circuit and observed the charging and discharging phases of a capacitor. In addition, we deduced the time constant from the slope of natural log functions, for both the charging and discharging processes. After deducing the time constant from graphical analysis, we compared it to the product of the resistance of the resistor in the circuit and the capacitance of the capacitor, to verify the accuracy of the methods in deducing 𝛕.