exp 1 - Experiment 1: RC Circuits Introduction In this...

Info iconThis preview shows pages 1–3. Sign up to view the full content.

View Full Document Right Arrow Icon
Experiment 1: RC Circuits 1 Experiment 1: RC Circuits Introduction In this laboratory you will examine a simple circuit consisting of only one capacitor and one resistor. By applying a constant 1 voltage (also called DC or direct current) to the circuit, you will determine the capacitor discharge decay time (defined later) and compare this value to that which is expected. Alternately, by applying alternating current (AC) and varying the frequency of the current you will be able to determine the decay time in another, independent way. You will determine these expected values using formulas derived from Ohm’s law, Kirchhoff’s Law and the concept of complex impedance. These concepts will be detailed further in the laboratory. In addition to these new ideas you will need to recall the concepts from last week’s lab. Specifically you will use the multimeter and oscilloscope during this lab. Recall that the oscilloscope must calibrated at the beginning of any experiment in which it is used. 1 Physics 1.1 Electrical Circuit Definitions Any section of a circuit that is at constant voltage is called a “node.” An example is a piece of wire joining two or more resistors. The sum of all the currents flowing into a node must be zero since charge can neither be created nor destroyed in a circuit. Circuit “elements” are resistors, capacitors, and inductors. One might consider wires connecting these elements to be a fourth circuit element but since idealized wires have no resistance, capacitance or inductance they are represented only by lines in a circuit diagram and do not appear in the equations relating current and voltage in circuits. Figure 1 Resistors in series Figure 2 Resistors R 4 and R 5 in parallel 1 Applying a square wave to the circuit is not exactly applying constant voltage. However, if the period of the square wave is long enough, you will not have to worry about what happens at the end when the voltage switches from one constant voltage to another.
Background image of page 1

Info iconThis preview has intentionally blurred sections. Sign up to view the full version.

View Full DocumentRight Arrow Icon
Experiment 1: RC Circuits 2 Two circuit elements are in series if all of the current flowing through one also flows through the other. In Figure 1, all of the current flowing from the battery must also flow through the resistors R 1 and R 2 . They are “in series.” In Figure 2, the current flowing through R 4 does not flow through R 5 (and vice versa) so that R 4 and R 5 are not in series. Two circuit elements are in parallel if they are connected to the same nodes. R 4 and R 5 in Figure 2 are both connected to nodes A and B. This then also requires that the potential difference (voltage drop) across all elements connected in parallel must be the same. In more complicated circuits you will need to generalize the notions of series and parallel. For example, in Figure 2, the equivalent resistance of R 4 and R 5 in parallel, 1 R 4 + 1 R 5 ( ) ! 1 = R 4 * R 5 R 4 + R 5 ( ) , is in series with R 3 .
Background image of page 2
Image of page 3
This is the end of the preview. Sign up to access the rest of the document.

This note was uploaded on 09/02/2009 for the course PHYS 2CL taught by Professor Bodde during the Spring '08 term at UCSD.

Page1 / 12

exp 1 - Experiment 1: RC Circuits Introduction In this...

This preview shows document pages 1 - 3. Sign up to view the full document.

View Full Document Right Arrow Icon
Ask a homework question - tutors are online