Copyright 2014 by Martin J. King. All Rights Reserved. Configuration : Extended Range Driver w/ Bass Driver Mounted on an Open Baffle
|
|
- Milton Carpenter
- 5 years ago
- Views:
Transcription
1 Open Baffle w/ 3 Drivers - Acoustic Response 12/3/1 Software : by Martin J. King MJKing57@aol.com Copyright 21 by Martin J. King. All Rights Reserved. Configuration : Extended Range Driver w/ Bass Driver Mounted on an Open Baffle Unit and Constant Definition cycle 2πrad Hz cyclesec 1 Air Density : ρ 1.25kgm 3 Speed of Sound : c 3msec 1 Part 1 : Thiele-Small Consistent Calculation Cable Series Resistance R add.ω Detailed User Input (Edit This Section and Input the Parameters for the System to be Analyzed) Power 1watt (Input Power) Applied Voltage Reference ---> R ref 8Ω Driver Thiele / Small Parameters : Lowther DX3 Average Driver Properties f d R e L vc Hz V ad liter V ad Ω R add Q ed R e R e R add. mh mh Q md Bl newton 1 1 Q td amp Q ed S 132.7cm 2 d 26cm 2 Q td.23 Q md 1 Bass Driver Thiele / Small Parameters : Eminence Alpha 15" High Efficiency f d R e L vc 1Hz V ad 26liter 5.88Ω Q ed mH Q md 7.23 Bl 7.7 newton 1 1 Q td amp Q ed S d 856.3cm 2 Q td Q md 1
2 Instructions : 1. A Zobel, Trap, and L-Pad are available for adjusting the Extended Range Driver's SPL output. 2. Select the crossover frequencies, orders, and types below. 3. Scroll down to the applicable crossover sections below and fill in the values of the circuit components. a. The theoretical values are shown to the right of each schematic. b, Theoretical values are calculated using only the driver's DC resistance, a textbook solution. c. Enter the actual component values, these should correspond to available components. d. Iterate the actual component values to optimize the crossover responses. e. You can mix the crossover orders and types by using only half of each pair of schematics.. Purchase the optimized actual component values and construct the crossover per the schematics. Crossover Definition For Even Order Crossovers : Type 1 = Linkwitz-Riley Type 2 = Bessel Type 3 = BEC Type = Butterworth Low Pass Filter High Pass Filter f LP 2Hz f HP 35Hz (Filter Frequency) LP order 2 HP order 2 (Filter Order :, 1, 2, 3, or ) LP type 1 HP type 3 (Filter Type : 1, 2, 3, or for even order only, for odd order this entry is ignored) Crossover Phase Connection and Extended Range Driver Attenuation LP phase 1 HP phase 1 (Phase : 1 = in phase, -1 = out of phase) L_Pad 3 db (L Pad Attemuation of Extended Range Driver)
3 Compensation Circuits (Default Actual Values Remove Circuits) Extended Range Driver Circuit Elements Zobel Components User Specified Compensation Circuit Values Suggested Values R zobel Ω Actual Values R zobel 1 1 Ω C zobel μf C zobel 1 1 μf Resonance Trap Components Suggested Values R trap Ω Actual Values R trap 1 1 Ω C trap μf C trap 1 1 μf L trap.856 mh L trap 1 1 mh L-Pad Components Suggested Values R parallel Ω Actual Values R parallel 1Ω R series Ω R series 2Ω
4 Woofer Circuit Elements Zobel Components User Specified Compensation Circuit Values Suggested Values R zobel Ω Actual Values R zobel 1 1 Ω C zobel μf C zobel 1 1 μf Resonance Trap Components Suggested Values R trap Ω Actual Values R trap 1 1 Ω C trap μf C trap 1 1 μf L trap mh L trap 1 1 mh L-Pad Components Suggested Values R parallel Ω Actual Values R parallel 1 1 Ω R series Ω R series Ω
5 Crossover Definition - 1 st Order High and Low Pass Crossover Definition - 2 nd Order High and Low Pass Schematic C1 + L1 - Tweeter Theoretical Values C 1 L μf mh + - L2 C2 Woofer L 2 C mh μf Enter Actual Component Values Below High Pass C 1 L 1 36μF R C1 Ω PE Part # mH R L1.7Ω PE Part # Low Pass L 2 C 2.7mH R L2.23Ω PE Part # μF R C2 Ω PE Part # Crossover Definition - 3 rd Order High and Low Pass Crossover Definition - th Order High and Low Pass
6 1 Electrical Crossover Curves Normalized Magnitude LP LP orderr HP HP orderr rdω Hz 1 Frequency (Hz) End of Detailed Input End of Part 1 Input
7 OB Driver Impedance 9 Phase (deg) argz r deg r Impedance (ohms) Z r r Frequency (Hz) Driver RMS Displacements (Red Curve - Woofers, Blue Curve - Extended Range Driver) 5 RMS Deflection (mm) x Lr mm x Hr mm rdω Hz 1 Frequency (Hz)
8 Part 2 : Detailed SPL Response Calculation Calculation Includes : Position of Drivers on the Baffle. Open Baffle Defraction for the Drivers. Floor Reflection for the Drivers. Geometry Coordinate System : Origin is the lower left corner of the front baffle y = horizontal direction z = vertical direction The variables num_r, n_low, and n_high control the number of simple sources used in the calculations. Increasing each will improve accuracy at the expense of longer calculation times. Increase each variable until final plotted SPL stops changing at which point the solution has converged. Enclosure Geometry Input X Y θ θ 1 Z 2ft 1.5ft 5deg deg 8ft stand m num_r 5 (Front Baffle Distance from Rear Wall > Depth of Enclosure) (Front Baffle Distance from Side Wall) (Rotation Towards Room Center) (Rotation Back of Baffle) (Floor to Ceiling Distance) (Height from Floor to Bottom Edge of Front Baffle) (Number of Points per Unit Length of Baffle Edge) Corner Coordinates Y coordinate y o y o1 y o2 y o3 2in Z coordinate 2in z o1 6in in z o2 6in in (Bottom Right Corner) (Top Right Corner) (Top Left Corner) (Bottom Left Corner) Extended Range Driver Geometry Input y dc z dc 12in in n_high 8 (Driver Center y Coordinate) (Driver Center z Coordinate) (Number of Points Across Diameter) Woofer Driver Geometry Input y w1 z w1 y w2 z w2 1in 9in 1in 26in n_low 15 (Lower Driver Center y Coordinate) (Lower Driver Center z Coordinate) (Upper Driver Center y Coordinate) (Upper Driver Center z Coordinate) (Number of Points Across Diameter)
9 Listening Position (Default Location is at 1 m Distance Along the Driver's Axis) n_listen = radius 3m θ z p deg 38in (Listening Position Relative to Speaker) (Calculation Radius, Effective Radius is Greater if y p is Changed from Default) ( deg is along the Driver's Axis, -8 deg < < 8 deg) (Default Height is Equal to Driver Height) n_listen = 1 X p Y p 1ft 7ft Z p z dc stand n_listen (Listening Position Relative to the Room Corner) (Default Height is Equal to Driver Height) (Method Selection) Floor Condition Reflect 1 ( = hardwood or concrete, 1 = carpeted) Refective Surface Selections (if 1 reflective surface is included, if reflective surface is removed) Inc_floor (Floor, Z = ) Inc_rear (Rear Wall, X = ) Inc_side (Left Side Wall, Y = ) Inc_ceiling (Ceiling)
10 Extended Range Driver and Two Woofer : Simple Source Pattern with Baffle Edge Outline 1.5 z d 1 z m z w z o y d y m y w y o
11 Three Dimensional View Axis Length (m) axis 2 <---- Change value of "axis" to rescale plots Room Corner is the Origin 2 Side view z driver 1.5 z outline z woofer 1 Side View - looking out from side wall z mic x driver x outline x woofer x mic 2 Front View z driver 1.5 z outline z woofer 1 Front View - looking towards rear wall z mic y driver y outline y woofer y mic 2 Top View y driver 1.5 y outline y woofer 1 Top View - looking down from ceiling y mic x driver x outline x woofer x mic
12 Plotted Response for the Extended Range Driver Dashed Red - Infinite Baffle Response Dashed Magenta - Baffle Response Dashed Brown - Crossover Response Solid Red - Combined Response SPL (db) 1 5 SPL IBr 5 X_over r 1 SPL 15 BFr 2 SPL nr rdω Hz 1 Phase (degrees) Phase r deg SPL (db) rdω Hz SPL Hr rdω Hz 1 Frequency (Hz)
13 Plotted Response for the Lower Woofer Driver Dashed Red - Infinite Baffle Response Dashed Magenta - Baffle Response Dashed Brown - Crossover Response Solid Red - Combined Response SPL (db) 1 5 SPL IBr 5 X_over r 1 SPL 15 BFr 2 SPL nr rdω Hz 1 Phase (degrees) Phase r deg rdω Hz 1 SPL (db) SPL Wr rdω Hz 1 Frequency (Hz)
14 Plotted Response for the Upper Woofer Driver Dashed Red - Infinite Baffle Response Dashed Magenta - Baffle Response Dashed Brown - Crossover Response Solid Red - Combined Response SPL (db) 1 5 SPL IBr 5 X_over r 1 SPL 15 BFr 2 SPL nr rdω Hz 1 Phase (degrees) Phase r deg rdω Hz 1 SPL (db) SPL Mr rdω Hz 1 Frequency (Hz)
15 Plotted Combined Response for the Woofer Drivers Phase (degrees) Phase r deg rdω Hz 1 SPL (db) SPL Lr rdω Hz 1 Frequency (Hz)
16 Plotted System Response for the Extended Range/Dual Woofer Open Baffle Design Phase (degrees) Phase r deg rdω Hz 1 SPL (db) SPL r 1 95 SPL 9 Lr 85 SPL Hr rdω Hz 1 Frequency (Hz)
17 System Time Response for an Impulse Input 3 Woofer Sound Pressure in Time Domain 2 p wooferr Pa rdt 1 System Sound Pressure in Time Domain 5 p summedr 1Pa rdt Time (sec)
18 Anechoic Horizontal Polar Response - Free Space Radius and Frequency Inputs radius ω 3m 37Hz (Calculation Radius Along the Driver's Axis) (Calculation Frequency : 1 Hz < < 1 Hz where must be an Integer Value) TOP VIEW B A C K SPL Hθ SPL Wθ SPL θ 18 5 F R O N T θdθ
19 Anechoic Vertical Polar Response - Free Space Radius and Frequency Inputs radius ω 3m 37Hz (Calculation Radius Along the Driver's Axis) (Calculation Frequency : 1 Hz < < 1 Hz where must be an Integer Value) SIDE VIEW B A C K SPL Hθ SPL Wθ SPL θ 18 5 F R O N T θdθ
20 System (no subscript) radius 3.m System Driver r Midrange Woofer r r r exp j rdω radius c System r SPL 2log r 21 5 Phase arg r System r Pa Phase (degrees) Phase r deg rdω Hz 1 SPL (db) SPL r rdω Hz 1 Frequency (Hz)
21
Open Baffle w/ 2 Drivers - Acoustic Response 12/30/14. Copyright 2014 by Martin J. King. All Rights Reserved.
Open Baffle w/ 2 Drivers - Acoustic Response 12/3/14 Software : by Martin J. King e-mail MJKing57@aol.com Copyright 214 by Martin J. King. All Rights Reserved. Configuration : Extended Range Driver w/
More informationOpen Baffle w/ 2 Drivers - Acoustic Response 12/27/12. Copyright 2012 by Martin J. King. All Rights Reserved.
Open Baffle w/ 2 Drivers - Acoustic Response 12/27/12 Software : by Martin J. King e-mail MJKing57@aol.com Copyright 212 by Martin J. King. All Rights Reserved. Configuration : Extended Range Driver w/
More informationDriver in a H Frame Transmission Line - Acoustic and Electrical Response 4/26/11. Copyright 2011 by Martin J. King. All Rights Reserved.
Driver in a H Frame Transmission Line - Acoustic and Electrical Response 4/26/ Software : by Martin J. King e-mail MJKing57@aol.com Copyright 2 by Martin J. King. All Rights Reserved. Line Configuration
More informationSection 7.0 : Design of a Back Loaded Exponential Horn By Martin J. King, 08/17/04 Copyright 2004 by Martin J. King. All Rights Reserved.
Section 7. : Design of a Back Loaded Exponential Horn By Martin J. King, 8/7/4 Copyright 4 by Martin J. King. All Rights Reserved. Section 7. : Design of a Back Loaded Exponential Horn For over a year,
More informationH C. Normalized Amplitude Response (db-spl/hz) Custom Amplitude Response (db-spl/hz at 1 m) with 450 watts Eminence Designer
KappaLite 31LF Small Vented Floor Wedge Or Sat By Jerry McNutt, Eminence Speaker LLC 45 Watts Power Handling, F3 of 72 Hz, High Pass Suggested at Hz. Box Properties --Description-- Name: Type: Vented Box
More informationPRO 5W-8. Professional series. SPL vs Freq. Specification. Materials of Construction
Professional series PRO 5W-8 Small in size, large in performance. Featuring an advanced X5 pulp cone, high temperature copper wire voice coil, and truncated cast frame chassis, the Pro 5W can handle your
More informationSection 6.0 : Advanced Transmission Line Modeling Techniques By Martin J King, 07/05/02 Copyright 2002 by Martin J. King. All Rights Reserved.
Section 6.0 : Advanced Transmission Line Modeling Techniques In Section 4.0, two simple models were derived for a closed end and an open end transmission line. In both of these models the driver is located
More informationNormalized Amplitude Response (db-spl/hz) Custom Amplitude Response (db-spl/hz at 1 m) with 850 watts Eminence Designer
Impero 1A Small Vented Design By Jerry McNutt, Eminence Speaker LLC 5 Watt Design; F3 at 9 Hz. Use a steep high pass filter at 35 Hz. Super Compact Subwoofer. Will not go very low, but gets very Loud!
More informationAlpha 3-8 Small Sealed Midrange Design By Jerry McNutt, Eminence Speaker LLC 30 Watts; F3 at 185 Hz. Best used above 250 Hz.
Alpha 3-8 Small Sealed Midrange Design By Jerry McNutt, Eminence Speaker LLC 30 Watts; F3 at 185 Hz. Best used above 250 Hz. Box Properties --Description-- Name: Type: Closed Box Shape: Prism, square --Box
More informationNormalized Amplitude Response (db-spl/hz) Custom Amplitude Response (db-spl/hz at 1 m) with 100 watts. Maximum Acoustic Power (db-spl/hz at 1 m)
Alpha 5-8 Small Sealed Design By Jerry McNutt, Eminence Speaker LLC Limit to 0 Watts; F3 of 132 Hz. Best used with a Highpass Filter at 153 Hz Small Sealed Midbass Box Properties --Description-- Name:
More informationNormalized Amplitude Response (db-spl/hz) Custom Amplitude Response (db-spl/hz at 1 m) with 160 watts. Maximum Acoustic Power (db-spl/hz at 1 m)
BetaA Micro Sealed Midrange Box By Jerry McNutt, Eminence Speaker LLC Limit to 1 Watts. F3 of 193 Hz. Best to use a steep High Pass above Hz. PA or Autosound High Power Midrange. Ohms. Box Properties Name:
More informationr p = r o r cos( φ ) cos( α )
Section 4. : Sound Radiation Pattern from the Mouth of a Horn In the previous section, the acoustic impedance at the mouth of a horn was calculated. Distributed simple sources were used to model the mouth
More informationComparison Between Theoretical Models and Experimental Measurements of Electrodinamic Loudspeaker Systems.
Comparison Between Theoretical Models and Experimental Measurements of Electrodinamic Loudspeaker Systems. Juan José Gómez Alfageme, Manuel Recuero López, José Luis Sánchez Bote Dpto. Ingeniería Audiovisual
More informationNormalized Amplitude Response (db-spl/hz) Custom Amplitude Response (db-spl/hz at 1 m) with 125 watts. Maximum Acoustic Power (db-spl/hz at 1 m)
Legend CA-1 "Classic" x Bass Guitar Cab By Jerry McNutt, Eminence Speaker LLC Limit to 15 Watts; F3 at 8 Hz. Two 1 ohm drivers in parallel for an 8 ohm load. Box Properties Name: Type: Vented Box Shape:
More informationImpedance and Loudspeaker Parameter Measurement
ECEN 2260 Circuits/Electronics 2 Spring 2007 2-26-07 P. Mathys Impedance and Loudspeaker Parameter Measurement 1 Impedance Measurement Many elements from which electrical circuits are built are two-terminal
More informationA R T A - A P P L I C A T I O N N O T E
Loudspeaker Free-Field Response This AP shows a simple method for the estimation of the loudspeaker free field response from a set of measurements made in normal reverberant rooms. Content 1. Near-Field,
More informationP773 Acoustics June, 2008
P773 Acoustics June, 2008 1 Physical principle 2 3 Denotes an Example 4 5 Measure pressure inside sealed box 6 Acoustic impulse response inside the box 7 8 Air spring only 9 10 For Plane Waves 11 More
More informationIntroduction to Acoustics Exercises
. 361-1-3291 Introduction to Acoustics Exercises 1 Fundamentals of acoustics 1. Show the effect of temperature on acoustic pressure. Hint: use the equation of state and the equation of state at equilibrium.
More informationEE-202 Exam III April 10, 2008
EE-202 Exam III April 10, 2008 Name: (Please print clearly) Student ID: CIRCLE YOUR DIVISION Morning 8:30 MWF Afternoon 12:30 MWF INSTRUCTIONS There are 13 multiple choice worth 5 points each and there
More information6.17 The Lossy Voice-Coil Inductance
6.7. THE LOSSY VOICE-COIL INDUCTANCE Solution. The impedance function is given by (/3.3) (s/38.2) Z VC (s) =7+0.008s +70 (s/38.2) 2 +(/3.3) (s/38.2) + Example 0 Solve for the element values in the equivalent
More informationFile: KappaPro15SmallVentedBox500Watts.bb6
KappaPro15A, Small Vented Box, For Mid/High use only. By McJerry, Eminence Speaker LLC Displacement limited to 3 watts if run down to 1 Hz. Displacement and thermally limited to 5 watts if run down to
More informationNonlinear Losses in Electro-acoustical Transducers Wolfgang Klippel, Daniel Knobloch
The Association of Loudspeaker Manufacturers & Acoustics International (ALMA) Nonlinear Losses in Electro-acoustical Transducers Wolfgang Klippel, Daniel Knobloch Institute of Acoustics and Speech Communication
More informationAccurate Determination of Loudspeaker Parameters using Audio Analyzer Type 2012 and Laser Velocity Transducer Type 3544
7/6-'89 Application Note Accurate Determination of Loudspeaker Parameters using Audio Analyzer Type 202 and Laser Velocity Transducer Type 3544 by Søren Jønsson, Brüel & Kjær, Denmark A method to determine
More informationChapter 31: RLC Circuits. PHY2049: Chapter 31 1
hapter 31: RL ircuits PHY049: hapter 31 1 L Oscillations onservation of energy Topics Damped oscillations in RL circuits Energy loss A current RMS quantities Forced oscillations Resistance, reactance,
More informationODEON APPLICATION NOTE Calibration of Impulse Response Measurements
ODEON APPLICATION NOTE Calibration of Impulse Response Measurements Part 2 Free Field Method GK, CLC - May 2015 Scope In this application note we explain how to use the Free-field calibration tool in ODEON
More informationEE221 Circuits II. Chapter 14 Frequency Response
EE22 Circuits II Chapter 4 Frequency Response Frequency Response Chapter 4 4. Introduction 4.2 Transfer Function 4.3 Bode Plots 4.4 Series Resonance 4.5 Parallel Resonance 4.6 Passive Filters 4.7 Active
More informationMechatronic design optimisation of subwoofer system. P6-project spring 2010 Group MCE6-621
Mechatronic design optimisation of subwoofer system P6-project spring 2010 Group MCE6-621 Title: Mechatronic design optimisation of subwoofer system Semester: 6th semester 2010 Semester theme: Mechatronic
More informationEE1.el3 (EEE1023): Electronics III. Acoustics lecture 18 Room acoustics. Dr Philip Jackson.
EE1.el3 EEE1023): Electronics III Acoustics lecture 18 Room acoustics Dr Philip Jackson www.ee.surrey.ac.uk/teaching/courses/ee1.el3 Room acoustics Objectives: relate sound energy density to rate of absorption
More informationAC Circuits Homework Set
Problem 1. In an oscillating LC circuit in which C=4.0 μf, the maximum potential difference across the capacitor during the oscillations is 1.50 V and the maximum current through the inductor is 50.0 ma.
More informationSCHOOL OF COMPUTING, ENGINEERING AND MATHEMATICS SEMESTER 1 EXAMINATIONS 2012/2013 XE121. ENGINEERING CONCEPTS (Test)
s SCHOOL OF COMPUTING, ENGINEERING AND MATHEMATICS SEMESTER EXAMINATIONS 202/203 XE2 ENGINEERING CONCEPTS (Test) Time allowed: TWO hours Answer: Attempt FOUR questions only, a maximum of TWO questions
More informationElectrical Engineering Fundamentals for Non-Electrical Engineers
Electrical Engineering Fundamentals for Non-Electrical Engineers by Brad Meyer, PE Contents Introduction... 3 Definitions... 3 Power Sources... 4 Series vs. Parallel... 9 Current Behavior at a Node...
More informationBME/ISE 3511 Bioelectronics - Test Five Review Notes Fall 2015
BME/ISE 35 Bioelectronics - Test Five Review Notes Fall 205 Test Five Topics: RMS Resistive Power oss (I 2 R) A Reactance, Impedance, Power Factor R ircuit Analysis alculate Series R Impedance alculate
More informationNumerical Model of the Insertion Loss Promoted by the Enclosure of a Sound Source
Numerical Model of the Insertion Loss Promoted by the Enclosure of a Sound Source Gil F. Greco* 1, Bernardo H. Murta 1, Iam H. Souza 1, Tiago B. Romero 1, Paulo H. Mareze 1, Arcanjo Lenzi 2 and Júlio A.
More informationTest Report. Force applied by the Transducer of the Frequencer TM, model Written by: Bruno Tardif, P.Eng. Dymedso Inc.
Test Report Force applied by the Transducer of the Frequencer TM, model 1001 Written by: Bruno Tardif, P.Eng. Dymedso Inc. Date: November 11 th, 2006 Abstract This experiment examined the force applied
More informationSpeaker: Arthur Williams Chief Scientist Telebyte Inc. Thursday November 20 th 2008 INTRODUCTION TO ACTIVE AND PASSIVE ANALOG
INTRODUCTION TO ACTIVE AND PASSIVE ANALOG FILTER DESIGN INCLUDING SOME INTERESTING AND UNIQUE CONFIGURATIONS Speaker: Arthur Williams Chief Scientist Telebyte Inc. Thursday November 20 th 2008 TOPICS Introduction
More informationSteady State Frequency Response Using Bode Plots
School of Engineering Department of Electrical and Computer Engineering 332:224 Principles of Electrical Engineering II Laboratory Experiment 3 Steady State Frequency Response Using Bode Plots 1 Introduction
More informationProduct Data. Brüel & Kjær B. Sound Power Source Type Introduction
Product Data Sound Power Source Type 425 USES: Determination of sound power output of equipment by the Substitution Method Determination, by the Juxtaposition Method, of sound power output of equipment
More informationSimulation and measurement of loudspeaker nonlinearity with a broad-band noise excitation
Simulation and measurement of loudspeaker nonlinearity with a broad-band noise excitation Andrzej Dobrucki, Rafal Siczek To cite this version: Andrzej Dobrucki, Rafal Siczek. Simulation and measurement
More informationContents. 0. Introduction Loudspeaker s Impedance Why is this useful? How good is it? Bibliography...
Contents 0. Introduction... 2... 2 1. Loudspeaker s Impedance... 2 2. Why is this useful?... 10 3. How good is it?... 13 4. Bibliography... 14 0. Introduction In this article I present a way to model a
More informationLast time: small acoustics
Last time: small acoustics Voice, many instruments, modeled by tubes Traveling waves in both directions yield standing waves Standing waves correspond to resonances Variations from the idealization give
More informationEE-202 Exam III April 13, 2015
EE-202 Exam III April 3, 205 Name: (Please print clearly.) Student ID: CIRCLE YOUR DIVISION DeCarlo-7:30-8:30 Furgason 3:30-4:30 DeCarlo-:30-2:30 202 2022 2023 INSTRUCTIONS There are 2 multiple choice
More informationERRATA AND ADDITIONS FOR "ENGINEERING NOISE CONTROL" 4th Edn. First printing April 23, 2018
ERRATA AND ADDITIONS FOR "ENGINEERING NOISE CONTROL" 4th Edn. First printing April 3, 08 p4, Eq..3 should not have the ± symbol on the RHS p36, 3 lines from the bottom of the page, replace cos b with cos
More informationSymbolic SPICE TM Circuit Analyzer and Approximator
ymbolic PICE ymbolic PICE TM Circuit Analyzer and Approximator Application Note AN-001: eries Resonant Circuit by Gregory M. Wierzba Rev 07010 A) Introduction The schematic shown below in Fig. 1 is a series
More informationROOM ACOUSTICS THREE APPROACHES 1. GEOMETRIC RAY TRACING SOUND DISTRIBUTION
ROOM ACOUSTICS THREE APPROACHES 1. GEOMETRIC RAY TRACING. RESONANCE (STANDING WAVES) 3. GROWTH AND DECAY OF SOUND 1. GEOMETRIC RAY TRACING SIMPLE CONSTRUCTION OF SOUND RAYS WHICH OBEY THE LAWS OF REFLECTION
More informationDesign of Mufflers and Silencers. D. W. Herrin, Ph.D., P.E. University of Kentucky Department of Mechanical Engineering
D. W. Herrin, Ph.D., P.E. Department of Mechanical Engineering Types of Mufflers 1. Dissipative (absorptive) silencer: Duct or pipe Sound absorbing material (e.g., duct liner) Sound is attenuated due to
More informationINTRODUCTION. Description
INTRODUCTION "Acoustic metamaterial" is a label that encompasses for acoustic structures that exhibit acoustic properties not readily available in nature. These properties can be a negative mass density,
More informationBasics of Sound and Noise. David Herrin, Ph.D., P.E. University of Kentucky Department of Mechanical Engineering
Basics of Sound and Noise David Herrin, Ph.D., P.E. Department of Mechanical Engineering Ø Public University Ø 16 Colleges Ø 93 Undergraduate Programs Ø 99 M.S. Programs Ø 66 Ph.D. Programs Ø 28,000 Students
More informationPhysics 2B Spring 2010: Final Version A 1 COMMENTS AND REMINDERS:
Physics 2B Spring 2010: Final Version A 1 COMMENTS AND REMINDERS: Closed book. No work needs to be shown for multiple-choice questions. 1. A charge of +4.0 C is placed at the origin. A charge of 3.0 C
More informationUNIVERSITY OF SASKATCHEWAN Department of Physics and Engineering Physics
UNIVERSITY OF SASKATCHEWAN Department of Physics and Engineering Physics Physics 111.6 MIDTERM TEST #3 January 24, 2008 Time: 90 minutes NAME: (Last) Please Print (Given) STUDENT NO.: LECTURE SECTION (please
More informationSophomore Physics Laboratory (PH005/105)
CALIFORNIA INSTITUTE OF TECHNOLOGY PHYSICS MATHEMATICS AND ASTRONOMY DIVISION Sophomore Physics Laboratory (PH5/15) Analog Electronics Active Filters Copyright c Virgínio de Oliveira Sannibale, 23 (Revision
More informationEE-202 Exam III April 6, 2017
EE-202 Exam III April 6, 207 Name: (Please print clearly.) Student ID: CIRCLE YOUR DIVISION DeCarlo--202 DeCarlo--2022 7:30 MWF :30 T-TH INSTRUCTIONS There are 3 multiple choice worth 5 points each and
More informationEE221 Circuits II. Chapter 14 Frequency Response
EE22 Circuits II Chapter 4 Frequency Response Frequency Response Chapter 4 4. Introduction 4.2 Transfer Function 4.3 Bode Plots 4.4 Series Resonance 4.5 Parallel Resonance 4.6 Passive Filters 4.7 Active
More informationHandout 11: AC circuit. AC generator
Handout : AC circuit AC generator Figure compares the voltage across the directcurrent (DC) generator and that across the alternatingcurrent (AC) generator For DC generator, the voltage is constant For
More informationMR Range. 0.82µF µ2F µ3F µ7F µF 85 50
MR Range. The MR range of capacitors is, we believe, the ultimate audio grade capacitor currently available on the market. It is the result of a two year research programme into the influence an audio
More informationNumerical modeling of the primary source in a hemi-anechoic room
Numerical modeling of the primary source in a hemi-anechoic room R. Arina 1, K. Völkel 2 1 Politecnico di Torino, Torino, Italy 2 Physikalisch Technische Bundesanstalt, Braunschweig, Germany ABSTRACT An
More informationISO 354 INTERNATIONAL STANDARD. Acoustics Measurement of sound absorption in a reverberation room
INTERNATIONAL STANDARD ISO 354 Second edition 2003-05-15 Acoustics Measurement of sound absorption in a reverberation room Acoustique Mesurage de l'absorption acoustique en salle réverbérante Reference
More informationLearnabout Electronics - AC Theory
Learnabout Electronics - AC Theory Facts & Formulae for AC Theory www.learnabout-electronics.org Contents AC Wave Values... 2 Capacitance... 2 Charge on a Capacitor... 2 Total Capacitance... 2 Inductance...
More informationSimulation of Horn Driver Response by Direct Combination of Compression Driver Frequency Response and Horn FEA
Simulation of Horn Driver Response by Direct Combination of Compression Driver Response and Horn FEA Dario Cinanni CIARE, Italy Corresponding author: CIARE S.r.l., strada Fontenuovo 306/a, 60019 Senigallia
More informationElectrodynamics Qualifier Examination
Electrodynamics Qualifier Examination January 10, 2007 1. This problem deals with magnetostatics, described by a time-independent magnetic field, produced by a current density which is divergenceless,
More informationUnit 2 Electrical Quantities and Ohm s Law
Electrical Quantities and Ohm s Law Objectives: Define a coulomb. Define an ampere. Define a volt. Define an ohm. Define a watt. Objectives: Compute electrical values using Ohm s law. Discuss basic types
More informationIntroduction to Audio and Music Engineering
Introduction to Audio and Music Engineering Lecture 7 Sound waves Sound localization Sound pressure level Range of human hearing Sound intensity and power 3 Waves in Space and Time Period: T Seconds Frequency:
More informationPHYS 241 EXAM #2 November 9, 2006
1. ( 5 points) A resistance R and a 3.9 H inductance are in series across a 60 Hz AC voltage. The voltage across the resistor is 23 V and the voltage across the inductor is 35 V. Assume that all voltages
More informationSound radiation and sound insulation
11.1 Sound radiation and sound insulation We actually do not need this chapter You have learned everything you need to know: When waves propagating from one medium to the next it is the change of impedance
More informationPhys102 Term: 103 First Major- July 16, 2011
Q1. A stretched string has a length of.00 m and a mass of 3.40 g. A transverse sinusoidal wave is travelling on this string, and is given by y (x, t) = 0.030 sin (0.75 x 16 t), where x and y are in meters,
More informationSample paper 1. Question 1. What is the dimensional formula of torque? A. MLT -2 B. MT -2 C. ML 2 T -2 D. MLT -1 E. ML 3 T -2.
Sample paper 1 Question 1 What is the dimensional formula of torque? A. MLT -2 B. MT -2 C. ML 2 T -2 D. MLT -1 E. ML 3 T -2 Correct Answer: C Torque is the turning effect of force applied on a body. It
More informationEF 152 Final Exam - Fall, 2016 Page 1 Copy 169
EF 152 Final Exam - Fall, 2016 Page 1 Copy 169 The equation sheets may be removed when the test begins Instructions Do not open the exam until instructed to do so. Do not leave if there is less than 5
More informationEF 151 Final Exam, Fall, 2011 Page 1 of 11
EF 5 Final Exam, Fall, 0 Page of Instructions Do not open or turn over the exam until instructed to do so. Name, and section will be written on the st page of the exam after time starts. Do not leave your
More informationUniversity of Illinois at Chicago Spring ECE 412 Introduction to Filter Synthesis Homework #4 Solutions
Problem 1 A Butterworth lowpass filter is to be designed having the loss specifications given below. The limits of the the design specifications are shown in the brick-wall characteristic shown in Figure
More informationWAVE ACOUSTICS. F = k x (6.1) where k is the constant of proportionality or the spring constant.
WAVE ACOUSTICS Much of architectural acoustics can be addressed without consideration of the wave nature of sound. For example, environmental acoustics and the transmission of outdoor sound, for the most
More informationDriven RLC Circuits Challenge Problem Solutions
Driven LC Circuits Challenge Problem Solutions Problem : Using the same circuit as in problem 6, only this time leaving the function generator on and driving below resonance, which in the following pairs
More informationIII. The STM-8 Loop - Work in progress
III. The STM-8 Loop - Work in progress This contains the loop functions for a velocity input. The interaction between, forward gain, feedback function, loop gain and transfer function are well displayed.
More informationExpressions for f r (T ) and Q i (T ) from Mattis-Bardeen theory
8 Appendix A Expressions for f r (T ) and Q i (T ) from Mattis-Bardeen theory The Mattis-Bardeen theory of the anomalous skin effect in superconductors [0] may be used to derive the behavior of the resonance
More informationVehicle Dynamics CEE 320. Winter 2006 CEE 320 Steve Muench
Vehicle Dynamics Steve Muench Outline 1. Resistance a. Aerodynamic b. Rolling c. Grade. Tractive Effort 3. Acceleration 4. Braking Force 5. Stopping Sight Distance (SSD) Main Concepts Resistance Tractive
More informationEE-202 Exam III April 13, 2006
EE-202 Exam III April 13, 2006 Name: (Please print clearly) Student ID: CIRCLE YOUR DIVISION DeCarlo 2:30 MWF Furgason 3:30 MWF INSTRUCTIONS There are 10 multiple choice worth 5 points each and there is
More informationThermal Parameter Measurement AN 18
Thermal Parameter Measurement AN 18 Application Note to the R&D SYSTEM The lumped parameters of the thermal equivalent circuit are measured by using Power Test Module (PWT) The high-speed temperature monitoring
More informationNoise in enclosed spaces. Phil Joseph
Noise in enclosed spaces Phil Joseph MODES OF A CLOSED PIPE A 1 A x = 0 x = L Consider a pipe with a rigid termination at x = 0 and x = L. The particle velocity must be zero at both ends. Acoustic resonances
More informationD is the voltage difference = (V + - V - ).
1 Operational amplifier is one of the most common electronic building blocks used by engineers. It has two input terminals: V + and V -, and one output terminal Y. It provides a gain A, which is usually
More information100 Physics Facts. 1. The standard international unit (SI unit) for mass (m) is. kg (kilograms) s (seconds)
100 Physics Facts 1. The standard international unit (SI unit) for mass (m) is. kg (kilograms) 2. The standard international unit (SI unit) for time (t) is. s (seconds) 3. The standard international unit
More informationCambridge International Examinations Cambridge International Advanced Level
Cambridge International Examinations Cambridge International Advanced Level *1906711534* PHYSICS 9702/41 Paper 4 A2 Structured Questions May/June 2014 2 hours Candidates answer on the Question Paper. No
More informationNAME: PHYSICS 3 FALL 2009 FINAL EXAM (VERSION A ) A) Wood B) Glass C) Equal D) No reflection occurs from either material
NAME: PHYSICS 3 FALL 2009 FINAL EXAM (VERSION A ) 1. A sound wave in air ( v sound = 344 m/sec ) hits a wall made of wood ( v sound = 1000 m/sec ) which contains a window made of glass ( v sound = 700
More informationExtended Creep Modeling AN 49
Extended Creep Modeling AN 49 Application Note for the Klippel R&D SYSTEM This application note gives an outline how to deploy the CAL LPM Extended Creep Modeling Script to estimate linear transducer parameters
More informationDamage Inspection of Fiber Reinforced Polymer-Concrete Systems using a Distant Acoustic-Laser NDE Technique
SPIE Smart Structures/NDE March 11, 2010, San Diego, CA Session 10: Civil Infrastructure Health Monitoring I Damage Inspection of Fiber Reinforced Polymer-Concrete Systems using a Distant Acoustic-Laser
More informationPhysics 405/505 Digital Electronics Techniques. University of Arizona Spring 2006 Prof. Erich W. Varnes
Physics 405/505 Digital Electronics Techniques University of Arizona Spring 2006 Prof. Erich W. Varnes Administrative Matters Contacting me I will hold office hours on Tuesday from 1-3 pm Room 420K in
More informationFinal Exam: 11 May 2001, Friday, 10 AM
Spring 2001 BE 3600 BioInstrumentation Final Exam: 11 May 2001, Friday, 10 AM ACTUALLY ADMINISTERED IN CLASS This exam: Consists of 12 questions, Score from this exam will determine 25-30 % of your grade,
More informationEE-202 Exam III April 15, 2010
EE-0 Exam III April 5, 00 Name: SOLUTION (No period) (Please print clearly) Student ID: CIRCLE YOUR DIVISION Morning 8:30 MWF Afternoon 3:30 MWF INSTRUCTIONS There are 9 multiple choice worth 5 points
More informationChapter 3. Background
Chapter 3. Background Parameters The following parameters and formulas are used within BoxCad program. General Parameters pi = 3.142 pi number ro = 1.18 density of air 1.18kg/m3 c = 344.8 speed of sound
More information3 Modeling and Simulation
ME 132, Spring 2005, UC Berkeley, A Packard 13 3 Modeling and Simulation 31 Systems of 1st order, coupled differential equations Consider an input/output system, with m inputs (denoted by d), q outputs
More informationChapter 10 Sound in Ducts
Chapter 10 Sound in Ducts Slides to accompany lectures in Vibro-Acoustic Design in Mechanical Systems 01 by D. W. Herrin Department of Mechanical Engineering Lexington, KY 40506-0503 Tel: 859-18-0609 dherrin@engr.uky.edu
More informationThe Approximating Impedance
Georgia Institute of Technology School of Electrical and Computer Engineering ECE 4435 Op Amp Design Laboratory Fall 005 DesignProject,Part A White Noise and Pink Noise Generator The following explains
More informationNAME: PHYSICS 6B SPRING 2011 FINAL EXAM ( VERSION A )
NAME: PHYSCS 6B SPRNG 2011 FNAL EXAM ( VERSON A ) Choose the best answer for each of the following multiple-choice questions. There is only one answer for each. Questions 1-2 are based on the following
More informationComparison between measurement and Boundary Element Modelization of subwoofers
Audio Engineering Society Convention Paper Presented at the 127th Convention 2009 October 9 12 New York NY, USA The papers at this Convention have been selected on the basis of a submitted abstract and
More informationSolved Problems. Electric Circuits & Components. 1-1 Write the KVL equation for the circuit shown.
Solved Problems Electric Circuits & Components 1-1 Write the KVL equation for the circuit shown. 1-2 Write the KCL equation for the principal node shown. 1-2A In the DC circuit given in Fig. 1, find (i)
More informationLaplace Transform Analysis of Signals and Systems
Laplace Transform Analysis of Signals and Systems Transfer Functions Transfer functions of CT systems can be found from analysis of Differential Equations Block Diagrams Circuit Diagrams 5/10/04 M. J.
More informationDELTA Test Report. DANAK TEST Reg. no Measurement of Sound Absorption Coefficient for Kvadrat Soft Cells Wall Panel Type Time
We help ideas meet the real world DELTA Test Report DANAK TEST Reg. no. 100 Measurement of Sound Absorption Coefficient for Kvadrat Soft Cells Wall Panel Type Time Client: Kvadrat Soft Cells A/S Page 1
More informationPhysics 6b Winter 2015 Final Campagnari Section Test Form D
Physics 6b Winter 2015 Final Campagnari Section Test Form D Fill out name and perm number on the scantron. Do not forget to bubble in the Test Form (A, B, C, or, D). At the end, only turn in the scantron.
More informationPhysics 6b Winter 2015 Final Campagnari Section Test Form A
Physics 6b Winter 2015 Final Campagnari Section Test Form A Fill out name and perm number on the scantron. Do not forget to bubble in the Test Form (A, B, C, or, D). At the end, only turn in the scantron.
More informationPhysics 1B Spring 2010: Final Version A 1 COMMENTS AND REMINDERS:
Physics 1B Spring 2010: Final Version A 1 COMMENTS AND REMINDERS: Closed book. No work needs to be shown for multiple-choice questions. 1. Four charges are at the corners of a square, with B and C on opposite
More informationPrediction of Sound Propagation From Power Transmission Plant
Prediction of Sound Propagation From Power Transmission Plant Jingchao Sun Stockholm, 2013 Thesis for the degree of Master of Science, 30 Hp Department of Sound and Vibration The Marcus Wallenberg Laboratory
More informationUNIVERSITY OF SASKATCHEWAN Department of Physics and Engineering Physics
UNIVERSITY OF SASKATCHEWAN Department of Physics and Engineering Physics Physics 117.3 MIDTERM TEST February 13, 2014 Time: 90 minutes NAME: (Last) Please Print (Given) STUDENT NO.: LECTURE SECTION (please
More informationOp-Amp Circuits: Part 3
Op-Amp Circuits: Part 3 M. B. Patil mbpatil@ee.iitb.ac.in www.ee.iitb.ac.in/~sequel Department of Electrical Engineering Indian Institute of Technology Bombay Introduction to filters Consider v(t) = v
More information