LRC Phases

LRC Phases - PHY 132 LAB LRC circuit (phases) Introduction...

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

View Full Document Right Arrow Icon
PHY132 Labs ( © P. Bennett, JCHS) -1- 08/11/04 PHY 132 LAB LRC circuit (phases) Introduction "Phase" means the relative advance or retardation (expressed in radians) of one wave with respect to another. Two waves whose crests coincide are said to be "in phase" - if the crests of one lie over the valleys of the other, they are pi out of phase. It is only simple to define phase for waves of the same frequency. In this lab we will measure the phase difference between voltage and current for each component in a series LRC resonant circuit. The purpose of the lab is teach you about the concept of phase and reactance in AC electrical circuits. Resonant circuits are used in oscillators to generate radio waves, and are studied with this same circuit in the next lab. In this experiment we compare the phase of the voltage across "reactive" components (inductance, capacitance) with that of the current, which is the reference. (The phase of the current is equal to that of the voltage across any resistor , so we actually measure voltage instead. Voltage and current are "in step" across a resistor, but not across a capacitor or inductor). Capacitors and inductors have "Reactance", which is a kind of frequency- dependant resistance, and is used for inductors and capacitors because these circuit elements change the phase relationship between current and voltage through them, unlike a resistor. We will see that Ohm's still holds in frequency-dependant form for reactances. Theory R C V_in L Fig. 1 Generic series LRC circuit. Consider the steady-state (sinewave) behavior of a series LRC circuit as shown in Fig. 1. By definition, the same current flows through each component of a series circuit (it has the same value everywhere in the circuit at any particular time) and can be written as i(t) = I 0 sin( ω t) eq. 1
Background image of page 1

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

View Full DocumentRight Arrow Icon
PHY132 Labs ( © P. Bennett, JCHS) -2- 08/11/04 Here ω = 2 π f, where f is the frequency in cycles per second or Hz.
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 05/11/2008 for the course PHY 132 taught by Professor Tsen during the Fall '08 term at ASU.

Page1 / 6

LRC Phases - PHY 132 LAB LRC circuit (phases) Introduction...

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