E13e Switching Processes and Damped Oscillations

Similar documents
Coupled pendulums and degree of coupling

W 18e Heat Capacity Ratio γ

Inductance, RL and RLC Circuits

Inductance, Inductors, RL Circuits & RC Circuits, LC, and RLC Circuits

Electromagnetic Oscillations and Alternating Current. 1. Electromagnetic oscillations and LC circuit 2. Alternating Current 3.

Handout 10: Inductance. Self-Inductance and inductors

Old Dominion University Physics 112N/227N/232N Lab Manual, 13 th Edition

MASSACHUSETTS INSTITUTE OF TECHNOLOGY Department of Physics 8.02 Spring 2003 Experiment 17: RLC Circuit (modified 4/15/2003) OBJECTIVES

Basic RL and RC Circuits R-L TRANSIENTS: STORAGE CYCLE. Engineering Collage Electrical Engineering Dep. Dr. Ibrahim Aljubouri

MODULE I. Transient Response:

Coupled Electrical Oscillators Physics Advanced Physics Lab - Summer 2018 Don Heiman, Northeastern University, 5/24/2018

Lab 4 RC Circuits. Name. Partner s Name. I. Introduction/Theory

Lecture 39. PHYC 161 Fall 2016

Chapter 32. Inductance

Physics 4 Spring 1989 Lab 5 - AC Circuits

Self-inductance A time-varying current in a circuit produces an induced emf opposing the emf that initially set up the time-varying current.

Active Figure 32.3 (SLIDESHOW MODE ONLY)

Chapter 30. Inductance. PowerPoint Lectures for University Physics, 14th Edition Hugh D. Young and Roger A. Freedman Lectures by Jason Harlow

Physics Investigation 10 Teacher Manual

AC Circuits Homework Set

Chapter 4 Transients. Chapter 4 Transients

University of TN Chattanooga Physics 1040L 8/18/2012 PHYSICS 1040L LAB LAB 4: R.C. TIME CONSTANT LAB

Slide 1 / 26. Inductance by Bryan Pflueger

Capacitors. The charge Q on a capacitor s plate is proportional to the potential difference V across the Q = C V (1)

[1] (b) Fig. 1.1 shows a circuit consisting of a resistor and a capacitor of capacitance 4.5 μf. Fig. 1.1

Alternating Current Circuits. Home Work Solutions

Lab 08 Capacitors 2. Figure 2 Series RC circuit with SPDT switch to charge and discharge capacitor.

Inductance, RL Circuits, LC Circuits, RLC Circuits

Chapter 3: Capacitors, Inductors, and Complex Impedance

M15e Bending of beams

= (fundamental constants c 0, h, k ). (1) k

EE 242 EXPERIMENT 8: CHARACTERISTIC OF PARALLEL RLC CIRCUIT BY USING PULSE EXCITATION 1

Exercise 1: Capacitors

Experiment 8: Capacitance and the Oscilloscope

Switch. R 5 V Capacitor. ower upply. Voltmete. Goals. Introduction

Electrical Circuits Lab Series RC Circuit Phasor Diagram

Switch. R 5 V Capacitor. ower upply. Voltmete. Goals. Introduction

Michelson Interferometer

EXPERIMENT 5A RC Circuits

TAP 126-4: Charging capacitors

An Optimised High Current Impulse Source

Class #12: Experiment The Exponential Function in Circuits, Pt 1

Capacitor in the AC circuit with Cobra3

( ) ( ) = q o. T 12 = τ ln 2. RC Circuits. 1 e t τ. q t

Laboratory manual : RC circuit

RLC Circuits. 1 Introduction. 1.1 Undriven Systems. 1.2 Driven Systems

2005 AP PHYSICS C: ELECTRICITY AND MAGNETISM FREE-RESPONSE QUESTIONS

Switch. R 5 V Capacitor. ower upply. Voltmete. Goals. Introduction

ECE 241L Fundamentals of Electrical Engineering. Experiment 5 Transient Response

Exercise 4 Modeling transient currents and voltages

RLC Series Circuit. We can define effective resistances for capacitors and inductors: 1 = Capacitive reactance:

Name:... Section:... Physics 208 Quiz 8. April 11, 2008; due April 18, 2008

ELECTROMAGNETIC OSCILLATIONS AND ALTERNATING CURRENT

Prepare for this experiment!

RC Circuit (Power amplifier, Voltage Sensor)

Laboratory 7: Charging and Discharging a Capacitor Prelab

Lab #4 Capacitors and Inductors. Capacitor Transient and Steady State Response

Name: Lab Partner: Section:

On the axes of Fig. 4.1, carefully sketch a graph to show how the potential difference V across the capacitor varies with time t. Label this graph L.

Assessment Schedule 2015 Physics: Demonstrate understanding of electrical systems (91526)

RC Circuit Lab - Discovery PSI Physics Capacitors and Resistors

Experiment Guide for RC Circuits

HOMEWORK 4: MATH 265: SOLUTIONS. y p = cos(ω 0t) 9 ω 2 0

Inductance. Slide 2 / 26. Slide 1 / 26. Slide 4 / 26. Slide 3 / 26. Slide 6 / 26. Slide 5 / 26. Mutual Inductance. Mutual Inductance.

RC, RL, and LCR Circuits

Core Technology Group Application Note 3 AN-3

Physics 4B Chapter 31: Electromagnetic Oscillations and Alternating Current

Capacitors. Example 1


PES 1120 Spring 2014, Spendier Lecture 35/Page 1

Electricity and Light Pre Lab Questions

Lab 5 AC Concepts and Measurements II: Capacitors and RC Time-Constant

Version 001 CIRCUITS holland (1290) 1

Physics 401 Classical Physics Laboratory. Experiment 5. Transients and Oscillations in RLC Circuits. I. Introduction II. Theory...

PHYSICS 171 UNIVERSITY PHYSICS LAB II. Experiment 6. Transient Response of An RC Circuit

Sinusoidal Response of RLC Circuits

RC Circuits. Equipment: Capstone with 850 interface, RLC circuit board, 2 voltage sensors (no alligator clips), 3 leads V C = 1

The RC Time Constant

ENERGY AND TIME CONSTANTS IN RC CIRCUITS By: Iwana Loveu Student No Lab Section: 0003 Date: February 8, 2004

Figure 1: Capacitor circuit

AC analysis. EE 201 AC analysis 1

PROBLEMS FOR EXPERIMENT ES: ESTIMATING A SECOND Solutions

(d) describe the action of a 555 monostable timer and then use the equation T = 1.1 RC, where T is the pulse duration

Lab 5 RC Circuits. What You Need To Know: Physics 212 Lab

As light level increases, resistance decreases. As temperature increases, resistance decreases. Voltage across capacitor increases with time LDR

first name (print) last name (print) brock id (ab17cd) (lab date)

P441 Analytical Mechanics - I. RLC Circuits. c Alex R. Dzierba. In this note we discuss electrical oscillating circuits: undamped, damped and driven.

EE292: Fundamentals of ECE

RC Studies Relaxation Oscillator

Practical 1 RC Circuits

Lecture 15. LC Circuit. LC Oscillation - Qualitative. LC Oscillator

Industrial Technology: Electronic Technology Crosswalk to AZ Math Standards

Laboratory 3 Measuring Capacitor Discharge with the MicroBLIP

Physics 212 Midterm 2 Form A

2.4 Models of Oscillation

Electric Circuits Fall 2015 Solution #5

Chapter 26 Direct-Current Circuits

RC & RL Transient Response

Capacitance Measurement

Lab 10: DC RC circuits

Transcription:

Fakultät für Physik und Geowissenschaften Physikalisches Grundpraktikum E13e Switching Processes and Damped Oscillations Tasks 1. To familiarize yourself with the computer-supported setup PA, measure various time dependent output voltages from a function generator. Determine the frequency and amplitude of the voltages using the cursor measurement-system.. Measure the time dependence of currents and voltages when switching on or off various R and RL series circuits. alculate the characteristic parameters of the circuit elements from the measured time constants. 3. Measure the free oscillations of a RL series circuit. Determine frequency f and damping of the oscillation. By using a variable ohmic resistor tune to the aperiodic limiting case. Literature Physics, P. A. Tipler, 3rd Edition, Vol., 3-, 6-8, 8-4 Physikalisches Praktikum, 14. Auflage, Hrsg. W. Schenk, F. remer, Elektrizitätslehre, 3.3, 4.1 (in German) Accessories Analog-to-digital converter PA with software, connection panel, function generator, laboratory power supply, resistors, capacitors, coils, digital multimeter ey Aspects for Preparation - Time dependence of the charging/discharging of a capacitor - Time dependence of the coil voltage during charging/discharging - Differential equation of the harmonic oscillator, eigenfrequency - Differential equation of the RL series circuit, eigenfrequency, quality factor, damping constant, logarithmic decrement, solutions for the oscillating case, aperiodic limiting case, creep case 1

Remarks The aim of this experiment is the study of time-resolved switching on/off processes occurring in R and RL series circuits. Moreover, free oscillations of a RL series circuit should be investigated. The latter circuit is modelled by a linear homogeneous differential equation of. order that is known from the mechanics of the damped harmonic oscillator, but has also broad applications in optics, atomic and molecular physics. For preparation, use irchhoff s laws to set up the relevant differential equations describing the circuits and verify the following solutions for switching on/off processes as well as damped oscillations. Switching on/off of a R series circuit (see circuits below) Switch-on time-function (charging) [time constant τ R = R] U ( ) exp t I t = R R, t U ( t) = U 1 exp R Switch-off time-function (discharging) I (t) = U exp t R R, U ( t ) = U exp t R Switching on/off of a RL series circuit (see circuits below) Switch-on time-function [time constant τ RLE = L/(R+R Sp)] U + R RSp ISp( t) = 1 exp t, L R USp( t) = U 1 1 exp t R + R Sp L Switch-off time-function [time constant τ RLA = L / ( R+R Sp+R p )] U + + R RSp Rp ISp( t) = exp t, L R + Rp + Rp USp( t) = U exp t L

Free damped oscillations Oscillation [ ω o > δ, δ =R/L] - U ( ) = e t t U (cos t + sin t ) or ( ) o - t U sin ( ) t = U e t + with tan Aperiodic limiting case [ω o = δ ] - t U ( t ) = U e ( 1 + t ) reep [ω o < δ ] (U : terminal voltage, : damping constant) tanh - o t - t U ( t) = U e 1 - cosh - o t 1- o / Hints to the experiment All voltages must be limited to a maximum of U < 10 V. The following circuits must be set up in a voltageless state and have to be controlled by the supervisor before use. The time dependent electric voltages are digitized by the PA interface, an analog-to-digital converter (AD). Via an USB interface the data are transmitted to the P and are stored in the software PA. The sampling rate and other settings are adjusted via the software. The measurement conditions are different for the various tasks and various values of the circuit elements. Adjust the measurement parameter in such a way that the time curve can be evaluated with highest precision possible in this experiment. The optoelectronic relay of the PA interface is used to switch the circuits. To this end the numbering of the inputs has to be taken into account (see sketch to the right). In the initial state inputs 0 and 1 are connected, whereas after activation of the relay that occurs automatically in the course of the measurement process, a connection between 0 and is established. Inputs and relay circuit of the PA (schematic) 3

Get to know the setup onnect the output (OUTPUT 0-10 V pp, 50 ) of the function generator with the input (H 1) of the PA interface. Measure the time dependence of a sine and a triangular voltage. Determine the frequency (or period) and the amplitude using the cursor system of the PA software. R series circuit Discharging As capacitance an electrolytic capacitor is used; therefore, during setup of the circuit pay attention to the correct polarity. The capacitance X is unknown and should be determined. To this end choose ten values of the resistor decade between R = 0.9 k and R = 9 k, determine the time constants from the time dependent voltage U (t) and find X by linear regression of the time constants. harging In order to determine the unknown value of the resistance R X, use the capacitor from the previous task. Measure the switch-on time-curve I(t)=U R(t)/R. Export the data into Origin and determine the time constant R by linear regression of the linearized graph or by fitting an exponential function to the data. Use the value of the time constant to calculate R X. RL series circuit Switch-on process hoose values R = 100 or R = 00 at the decade resistor for the determination of the inductance (L 1, L or L 3) of one of the available coils. Measure the switch-on time-function of the current I(t)=U R(t)/R using the voltage U R(t). In order to determine RL,in, evaluate the measured curve either with the cursor system in PA or with an appropriate graphic analysis. 4

Switch-off process For the circuit to the right use resistances R P = 0 and R = 00 (decade resistor). Evaluate the time function U Sp(t) for the determination of the time constant RL,out graphically or by linear regression. RL series circuit For the measurement of the free oscillations of a RL circuit use two known, but different values of the capacitance (important: Osc). Determine the eigenfrequency and the damping constant with the cursor system of the PA software. From these values calculate the inductance used in the experiment and compare to the result of the previous tasks. Software PA The software PA allows for the adjustment of the measurement parameters of the PA interface, it facilitates the transmission of the recorded values to the P and serves for the analysis and storage of the data. Data are recorded on up to four selectable channels. The measured voltages of these channels are shown on a numerical display. For the measurement the sampling rate (number of measurements per second) and the number of measurement points must be adjusted. Take into account that the UI des Programms PA maximum sampling rate is given by 10 5 /number of channels. The voltage range is fixed to ±10 V. The digital resolution is 16 Bit. The switching of the optoelectronic relay integrated in the PA interface is controllable from the program. The recorded data are shown in a table and in a diagram. The export of the data for further analysis is possible in an ASII format. Within the diagram measurements can be directly made with a cursor system. 5