Normalized 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)

Size: px
Start display at page:

Download "Normalized 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)"

Transcription

1 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: Type: Closed Box Shape: Prism, square --Box Parameters-- Vb =.5 cu.ft V(total) =. cu.ft Qtc =.735 QL = F3 = 19.9 Hz Fill = heavy Normalized Amplitude Response (-SPL/Hz) Driver Properties Name: BetaA Type: Standard one-way driver Company: Eminence Speaker LLC, USA --Configuration-- No. of Drivers = 1 --Mechanical Parameters-- Fs =. Hz Qms = 3. Vas = 3.51 liters Cms =.15 mm/n Mms = 1.93 g Rms =.3 kg/s Xmax =.5 mm Xmech = 5.7 mm P-Dia = 7. mm Sd = 9.9 sq.cm P-Vd =.57 liters --Electrical Parameters-- Qes =. Re = 5.1 ohms Le =.3 mh Z = ohms BL =.13 Tm Pe = 175 watts --Electromech. Parameters-- Qts =.5 no =.9 % 1-W SPL = V SPL = Custom Amplitude Response (-SPL/Hz at 1 m) with 1 watts Maximum Acoustic Power (-SPL/Hz at 1 m) File: BetaASmallSealedMidRange1Watts.bb

2 Page Two -- BetaASmallSealedMidRange1Watts.bb Maximum Electric Input Power (W/Hz) watts 1 1 Cone Displacement (mm/hz) with 1 watts mm System Impedance (ohms/hz) ohms

3 Page Three -- BetaASmallSealedMidRange1Watts.bb Phase Response (deg/hz) deg 9-9 ±1 9-9 ±1 msec Group Delay (msec/hz) 1 - -

4 BetaA Small Vented Mid/Bass Design By Jerry McNutt, Eminence Speaker LLC 175 Watts. F3 of 119 Hz. Best to use a steep High Pass above 11 Hz. PA or Autosound High Power Mid/Bass Ohms. Box Properties Name: Type: Vented Box Shape: Prism, square --Box Parameters-- Vb =.1 cu.ft V(total) =.15 cu.ft Fb = 5 Hz QL = 7 F3 = 117. Hz Fill = minimal --Vents-- No. of Vents = Vent shape = round Vent ends = one flush Dv = 1.59 in Lv =.5 in Normalized Amplitude Response (-SPL/Hz) Custom Amplitude Response (-SPL/Hz at 1 m) with 175 watts Driver Properties Name: BetaA Type: Standard one-way driver Company: Eminence Speaker LLC, USA --Configuration-- No. of Drivers = 1 --Mechanical Parameters-- Fs =. Hz Qms = 3. Vas = 3.51 liters Cms =.15 mm/n Mms = 1.93 g Rms =.3 kg/s Xmax =.5 mm Xmech = 5.7 mm P-Dia = 7. mm Sd = 9.9 sq.cm P-Vd =.57 liters --Electrical Parameters-- Qes =. Re = 5.1 ohms Le =.3 mh Z = ohms BL =.13 Tm Pe = 175 watts --Electromech. Parameters-- Qts =.5 no =.9 % 1-W SPL = V SPL = Maximum Acoustic Power (-SPL/Hz at 1 m) File: BetaASmallVentedMiass175Watts.bb

5 Page Two -- BetaASmallVentedMiass175Watts.bb Maximum Electric Input Power (W/Hz) watts 1 1 Cone Displacement (mm/hz) with 175 watts mm Vent Air Velocity (m/sec/hz) with 175 watts m/s 3 3 1

6 Page Three -- BetaASmallVentedMiass175Watts.bb System Impedance (ohms/hz) ohms Phase Response (deg/hz) deg 9-9 ±1 9-9 ±1 msec Group Delay (msec/hz) 1 - -

7 BetaA Medium Sized Vented Mid/Bass Design By Jerry McNutt, Eminence Speaker LLC 175 Watts. F3 of 97 Hz. Best to use a steep High Pass above 1 Hz. PA or Autosound High Power Mid/Bass Ohms. Box Properties Name: Type: Vented Box Shape: Prism, square --Box Parameters-- Vb =.3 cu.ft V(total) =.37 cu.ft Fb = 15 Hz QL = 7 F3 = 9.1 Hz Fill = minimal --Vents-- No. of Vents = Vent shape = round Vent ends = one flush Dv = 1.9 in Lv =.5 in Normalized Amplitude Response (-SPL/Hz) Custom Amplitude Response (-SPL/Hz at 1 m) with 175 watts Driver Properties Name: BetaA Type: Standard one-way driver Company: Eminence Speaker LLC, USA --Configuration-- No. of Drivers = 1 --Mechanical Parameters-- Fs =. Hz Qms = 3. Vas = 3.51 liters Cms =.15 mm/n Mms = 1.93 g Rms =.3 kg/s Xmax =.5 mm Xmech = 5.7 mm P-Dia = 7. mm Sd = 9.9 sq.cm P-Vd =.57 liters --Electrical Parameters-- Qes =. Re = 5.1 ohms Le =.3 mh Z = ohms BL =.13 Tm Pe = 175 watts --Electromech. Parameters-- Qts =.5 no =.9 % 1-W SPL = V SPL = Maximum Acoustic Power (-SPL/Hz at 1 m) File: BetaAMediumVentedMiass175Watts.bb

8 Page Two -- BetaAMediumVentedMiass175Watts.bb Maximum Electric Input Power (W/Hz) watts 1 1 Cone Displacement (mm/hz) with 175 watts mm Vent Air Velocity (m/sec/hz) with 175 watts m/s 3 3 1

9 Page Three -- BetaAMediumVentedMiass175Watts.bb System Impedance (ohms/hz) ohms Phase Response (deg/hz) deg 9-9 ±1 9-9 ±1 msec Group Delay (msec/hz) 1 - -

10 BetaA Large Vented Mid/Bass Design By Jerry McNutt, Eminence Speaker LLC 175 Watts. F3 of 95 Hz. Best to use a steep High Pass above 1 Hz. PA or Autosound High Power Mid/Bass Ohms. Box Properties Name: Type: Vented Box Shape: Prism, square --Box Parameters-- Vb =.3 cu.ft V(total) =.5 cu.ft Fb = 1 Hz QL = 7 F3 = 95. Hz Fill = minimal --Vents-- No. of Vents = Vent shape = round Vent ends = one flush Dv = 1.9 in Lv = 1.93 in Normalized Amplitude Response (-SPL/Hz) Custom Amplitude Response (-SPL/Hz at 1 m) with 175 watts Driver Properties Name: BetaA Type: Standard one-way driver Company: Eminence Speaker LLC, USA --Configuration-- No. of Drivers = 1 --Mechanical Parameters-- Fs =. Hz Qms = 3. Vas = 3.51 liters Cms =.15 mm/n Mms = 1.93 g Rms =.3 kg/s Xmax =.5 mm Xmech = 5.7 mm P-Dia = 7. mm Sd = 9.9 sq.cm P-Vd =.57 liters --Electrical Parameters-- Qes =. Re = 5.1 ohms Le =.3 mh Z = ohms BL =.13 Tm Pe = 175 watts --Electromech. Parameters-- Qts =.5 no =.9 % 1-W SPL = V SPL = Maximum Acoustic Power (-SPL/Hz at 1 m) File: BetaALargeVentedMiass175Watts.bb

11 Page Two -- BetaALargeVentedMiass175Watts.bb Maximum Electric Input Power (W/Hz) watts 1 1 Cone Displacement (mm/hz) with 175 watts mm Vent Air Velocity (m/sec/hz) with 175 watts m/s 3 3 1

12 Page Three -- BetaALargeVentedMiass175Watts.bb System Impedance (ohms/hz) ohms Phase Response (deg/hz) deg 9-9 ±1 9-9 ±1 msec Group Delay (msec/hz) 1 - -

13 BetaA Large Sealed Midrange Design By Jerry McNutt, Eminence Speaker LLC Limit to 1 Watts. F3 of 15 Hz. Best to use a steep High Pass above 15 Hz. PA or Autosound High Power Midrange. Ohms. Box Properties Name: Type: Closed Box Shape: Prism, square --Box Parameters-- Vb =.15 cu.ft V(total) =.17 cu.ft Qtc =.1 QL = F3 = 15. Hz Fill = heavy Normalized Amplitude Response (-SPL/Hz) Driver Properties Name: BetaA Type: Standard one-way driver Company: Eminence Speaker LLC, USA --Configuration-- No. of Drivers = 1 --Mechanical Parameters-- Fs =. Hz Qms = 3. Vas = 3.51 liters Cms =.15 mm/n Mms = 1.93 g Rms =.3 kg/s Xmax =.5 mm Xmech = 5.7 mm P-Dia = 7. mm Sd = 9.9 sq.cm P-Vd =.57 liters --Electrical Parameters-- Qes =. Re = 5.1 ohms Le =.3 mh Z = ohms BL =.13 Tm Pe = 175 watts --Electromech. Parameters-- Qts =.5 no =.9 % 1-W SPL = V SPL = Custom Amplitude Response (-SPL/Hz at 1 m) with 1 watts Maximum Acoustic Power (-SPL/Hz at 1 m) File: BetaALargeSealedMidRange1Watts.bb

14 Page Two -- BetaALargeSealedMidRange1Watts.bb Maximum Electric Input Power (W/Hz) watts 1 1 Cone Displacement (mm/hz) with 1 watts mm System Impedance (ohms/hz) ohms

15 Page Three -- BetaALargeSealedMidRange1Watts.bb Phase Response (deg/hz) deg 9-9 ±1 9-9 ±1 msec Group Delay (msec/hz) 1 - -

Alpha 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. 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 information

Normalized 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)

Normalized 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 information

Normalized Amplitude Response (db-spl/hz) Custom Amplitude Response (db-spl/hz at 1 m) with 850 watts Eminence Designer

Normalized 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 information

Normalized 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)

Normalized 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 information

H C. Normalized Amplitude Response (db-spl/hz) Custom Amplitude Response (db-spl/hz at 1 m) with 450 watts Eminence Designer

H 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 information

File: KappaPro15SmallVentedBox500Watts.bb6

File: 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 information

PRO 5W-8. Professional series. SPL vs Freq. Specification. Materials of Construction

PRO 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 information

Open 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. 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 information

Klippel Non-Linear Test Results. LSI (Large Signal Identification) Model #: PS Introduction. Large Signal Modeling. Nonlinear Characteristics

Klippel Non-Linear Test Results. LSI (Large Signal Identification) Model #: PS Introduction. Large Signal Modeling. Nonlinear Characteristics Klippel Non-Linear Test Results LSI (Large Signal Identification) Model #: PS180-8 Introduction Large Signal Modeling At higher amplitudes, loudspeakers produce substantial distortion in the output signal,

More information

Copyright 2014 by Martin J. King. All Rights Reserved. Configuration : Extended Range Driver w/ Bass Driver Mounted on an Open Baffle

Copyright 2014 by Martin J. King. All Rights Reserved. Configuration : Extended Range Driver w/ Bass Driver Mounted on an Open Baffle Open Baffle w/ 3 Drivers - Acoustic Response 12/3/1 Software : by Martin J. King e-mail MJKing57@aol.com Copyright 21 by Martin J. King. All Rights Reserved. Configuration : Extended Range Driver w/ Bass

More information

Klippel Non-Linear Test Results LSI (Large Signal Identification) Driver Name: ND90-8. Introduction. Nonlinear Parameters. Large Signal Modeling

Klippel Non-Linear Test Results LSI (Large Signal Identification) Driver Name: ND90-8. Introduction. Nonlinear Parameters. Large Signal Modeling Klippel Non-Linear Test Results LSI (Large Signal Identification) Driver Name: ND90-8 Introduction Large Signal Modeling At higher amplitudes, loudspeakers produce substantial distortion in the output

More information

Nonlinear Losses in Electro-acoustical Transducers Wolfgang Klippel, Daniel Knobloch

Nonlinear 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 information

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 12/30/14. 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 information

Chapter 3. Background

Chapter 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 information

Driver 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 4/26/11. 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 information

Section 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 7.0 : 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 information

Nonlinear Modeling of the Heat Transfer in Loudspeakers

Nonlinear Modeling of the Heat Transfer in Loudspeakers Nonlinear Modeling of the Heat Transfer in Loudspeakers Wolfgang Klippel Klippel GmbH Dresden, 01277, Germany www.klippel.de ABSTRACT Traditional modeling describes the heat flow in loudspeakers by an

More information

Test 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 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 information

Contents. 0. Introduction Loudspeaker s Impedance Why is this useful? How good is it? Bibliography...

Contents. 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 information

Introduction to Audio and Music Engineering

Introduction 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 information

Section 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 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 information

P773 Acoustics June, 2008

P773 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 information

Acoustics Analysis of Speaker ANSYS, Inc. November 28, 2014

Acoustics Analysis of Speaker ANSYS, Inc. November 28, 2014 Acoustics Analysis of Speaker 1 Introduction ANSYS 14.0 offers many enhancements in the area of acoustics. In this presentation, an example speaker analysis will be shown to highlight some of the acoustics

More information

Phys102 Final-132 Zero Version Coordinator: A.A.Naqvi Wednesday, May 21, 2014 Page: 1

Phys102 Final-132 Zero Version Coordinator: A.A.Naqvi Wednesday, May 21, 2014 Page: 1 Coordinator: A.A.Naqvi Wednesday, May 1, 014 Page: 1 Q1. What is the potential difference V B -V A in the circuit shown in Figure 1 if R 1 =70.0 Ω, R =105 Ω, R 3 =140 Ω, ε 1 =.0 V and ε =7.0 V? A).3 V

More information

ENGR-4300 Spring 2009 Test 2. Name: SOLUTION. Section: 1(MR 8:00) 2(TF 2:00) 3(MR 6:00) (circle one) Question I (20 points): Question II (20 points):

ENGR-4300 Spring 2009 Test 2. Name: SOLUTION. Section: 1(MR 8:00) 2(TF 2:00) 3(MR 6:00) (circle one) Question I (20 points): Question II (20 points): ENGR43 Test 2 Spring 29 ENGR43 Spring 29 Test 2 Name: SOLUTION Section: 1(MR 8:) 2(TF 2:) 3(MR 6:) (circle one) Question I (2 points): Question II (2 points): Question III (17 points): Question IV (2 points):

More information

Note 11: Alternating Current (AC) Circuits

Note 11: Alternating Current (AC) Circuits Note 11: Alternating Current (AC) Circuits V R No phase difference between the voltage difference and the current and max For alternating voltage Vmax sin t, the resistor current is ir sin t. the instantaneous

More information

Nonlinear Force Factor Measurement of an Electrodynamic Loudspeaker

Nonlinear Force Factor Measurement of an Electrodynamic Loudspeaker Nonlinear Force Factor Measurement of an Electrodynamic Loudspeaker Antonin Novak Orkidia Audio, 64310 Ascain, France Pierrick Lotton Laurent Simon Summary An electrodynamic loudspeaker is usually characterized

More information

Extended Creep Modeling AN 49

Extended 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 information

REACTANCE. By: Enzo Paterno Date: 03/2013

REACTANCE. By: Enzo Paterno Date: 03/2013 REACTANCE REACTANCE By: Enzo Paterno Date: 03/2013 5/2007 Enzo Paterno 1 RESISTANCE - R i R (t R A resistor for all practical purposes is unaffected by the frequency of the applied sinusoidal voltage or

More information

Accurate Determination of Loudspeaker Parameters using Audio Analyzer Type 2012 and Laser Velocity Transducer Type 3544

Accurate 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 information

Basics 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. 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 information

Core Technology Group Application Note 3 AN-3

Core Technology Group Application Note 3 AN-3 Measuring Capacitor Impedance and ESR. John F. Iannuzzi Introduction In power system design, capacitors are used extensively for improving noise rejection, lowering power system impedance and power supply

More information

For More info visit

For More info visit In order to make the measurement of a physical quantity we have, first of all, to evolve a standard for that measurement so that different measurements of same physical quantity can be expressed relative

More information

BME/ISE 3511 Bioelectronics - Test Five Review Notes Fall 2015

BME/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 information

200 SERIES CINEMA SCREENARRAY LOUDSPEAKER SYSTEM

200 SERIES CINEMA SCREENARRAY LOUDSPEAKER SYSTEM 200 SERIES CINEMA SCREENARRAY LOUDSPEAKER SYSTEM 200 SERIES FAMILY MAKE EVERY SEAT THE BEST SEAT IN THE HOUSE In designing the JBL 200 Series, our goal was to offer cinemas an affordable solution for creating

More information

Knud Thorborg Scan-Speak, Videbæk, Denmark,

Knud Thorborg Scan-Speak, Videbæk, Denmark, Knud Thorborg Scan-Speak, Videbæk, Denmark, kt@scan-speak.dk Traditional and Advanced Models for the Dynamic Loudspeaker The traditional equivalent circuit for a loudspeaker, based on the so-called Thiele-Small

More information

r p = r o r cos( φ ) cos( α )

r 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 information

University of Alberta ENGM 541: Modeling and Simulation of Engineering Systems Laboratory #7. M.G. Lipsett & M. Mashkournia 2011

University of Alberta ENGM 541: Modeling and Simulation of Engineering Systems Laboratory #7. M.G. Lipsett & M. Mashkournia 2011 ENG M 54 Laboratory #7 University of Alberta ENGM 54: Modeling and Simulation of Engineering Systems Laboratory #7 M.G. Lipsett & M. Mashkournia 2 Mixed Systems Modeling with MATLAB & SIMULINK Mixed systems

More information

Numerical investigation of a looped-tube traveling-wave thermoacoustic generator with a bypass pipe

Numerical investigation of a looped-tube traveling-wave thermoacoustic generator with a bypass pipe Available online at www.sciencedirect.com ScienceDirect Energy Procedia 142 (217) 1474 1481 www.elsevier.com/locate/procedia 9th International Conference on Applied Energy, ICAE217, 21-24 August 217, Cardiff,

More information

Introduction to Acoustics. Phil Joseph

Introduction to Acoustics. Phil Joseph Introduction to Acoustics Phil Joseph INTRODUCTION TO ACOUSTICS Sound and Noise Sound waves Frequency, wavelength and wavespeed Point sources Sound power and intensity Wave reflection Standing waves Measures

More information

LOUDSPEAKER ROCKING MODES MODELLING AND ROOT CAUSE ANALYSIS. William Cardenas and Wolfgang Klippel. Presented by Stefan Irrgang. KLIPPEL GmbH.

LOUDSPEAKER ROCKING MODES MODELLING AND ROOT CAUSE ANALYSIS. William Cardenas and Wolfgang Klippel. Presented by Stefan Irrgang. KLIPPEL GmbH. LOUDSPEAKER ROCKING MODES MODELLING AND ROOT CAUSE ANALYSIS William Cardenas and Wolfgang Klippel Presented by Stefan Irrgang KLIPPEL GmbH Loudspeaker Rocking Modes, Part 1 Modelling and root cause analysis,

More information

Sinusoidal Response of RLC Circuits

Sinusoidal Response of RLC Circuits Sinusoidal Response of RLC Circuits Series RL circuit Series RC circuit Series RLC circuit Parallel RL circuit Parallel RC circuit R-L Series Circuit R-L Series Circuit R-L Series Circuit Instantaneous

More information

A) 120 degrees B) 90 degrees C) 60 degrees D) 45 degrees E) 30 degrees

A) 120 degrees B) 90 degrees C) 60 degrees D) 45 degrees E) 30 degrees Phys10 - First Major 071 Zero Version Q1. Two identical sinusoidal traveling waves are sent along the same string in the same direction. What should be the phase difference between the two waves so that

More information

1. Dimensions of force constant are (MHT-CET-2003) (a) M 1 L 0 T 2 (b) M 1 L 0 T 2. (c) M 0 L 1 T 2 (d) MLT 2

1. Dimensions of force constant are (MHT-CET-2003) (a) M 1 L 0 T 2 (b) M 1 L 0 T 2. (c) M 0 L 1 T 2 (d) MLT 2 1. Dimensions of force constant are (MHT-CET-2003) M 1 L 0 T 2 M 1 L 0 T 2 M 0 L 1 T 2 MLT 2 2. A bar magnet is in oscillatory motion its frequency is n magnetic field induction is 0.4 10 5 T when the

More information

ST303C..L SERIES 515A. Features. Typical Applications. Major Ratings and Characteristics. Bulletin I25186 rev. A 05/94. case style TO-200AC (B-PUK)

ST303C..L SERIES 515A. Features. Typical Applications. Major Ratings and Characteristics. Bulletin I25186 rev. A 05/94. case style TO-200AC (B-PUK) ST303C..L SERIES INVERTER GRADE THYRISTORS Hockey Puk Version Features Metal case with ceramic insulator International standard case TO-AC (B-PUK) All diffused design Center amplifying gate Guaranteed

More information

Computational Acoustics by Means of Finite and Boundary Elements for Woofers, Tweeters, Horns and Small Transducers

Computational Acoustics by Means of Finite and Boundary Elements for Woofers, Tweeters, Horns and Small Transducers Computational Acoustics by Means of Finite and Boundary Elements for Woofers, Tweeters, Horns and Small Transducers Alfred J. Svobodnik NAD - Numerical Analysis and Design GmbH & Co KG as@nadwork.at http://www.nadwork.at

More information

Physics 1c practical, 2015 Homework 5 Solutions

Physics 1c practical, 2015 Homework 5 Solutions Physics c practical, 05 Homework 5 Solutions Serway 33.4 0.0 mh, = 0 7 F, = 0Ω, V max = 00V a The resonant frequency for a series L circuit is f = π L = 3.56 khz At resonance I max = V max = 5 A c Q =

More information

Gwinnett has an amazing story to share, spanning 200 years from 1818 until today.

Gwinnett has an amazing story to share, spanning 200 years from 1818 until today. I B, Lm, W - D I C Dm 15, 1818, W C, m D I. T m m m Ck Ck m Jk C. B m, 30, A 20. T mk, B, v v m C. m, m 1776, C C. O A 2, 1776, D I,. C v 437 q m xm 280,000. D 1980, C k, m v. A, 2010, j v 800,000 j m

More information

wave speed (metre/second, m/s) = frequency (hertz, Hz) x wavelength (metre, m)

wave speed (metre/second, m/s) = frequency (hertz, Hz) x wavelength (metre, m) Physics formulae: Unit P1 (GCSE Science ( Core Science )): The relationship between wave speed, frequency and wavelength: wave speed (metre/second, m/s) = frequency (hertz, Hz) x wavelength (metre, m)

More information

Chapter 17: Waves II. Sound waves are one example of Longitudinal Waves. Sound waves are pressure waves: Oscillations in air pressure and air density

Chapter 17: Waves II. Sound waves are one example of Longitudinal Waves. Sound waves are pressure waves: Oscillations in air pressure and air density Sound waves are one example of Longitudinal Waves Sound waves are pressure waves: Oscillations in air pressure and air density Before we can understand pressure waves in detail, we need to understand what

More information

Notes on Absorption and Impedance Measurements

Notes on Absorption and Impedance Measurements Notes on Absorption and Impedance Measurements Andrew F. Seybert University of Kentucky Lexington, KY 456-18 859-257-6336 x 8645 seybert@engr.uky.edu Applicable Standards. There are two standards 1,2 for

More information

N-Channel Enhancement-Mode Vertical DMOS FETs

N-Channel Enhancement-Mode Vertical DMOS FETs VN16 N-Channel Enhancement-Mode Vertical DMOS FETs Features Free from secondary breakdown Low power drive requirement Ease of paralleling Low C ISS and fast switching speeds High input impedance and high

More information

ST1230C..K SERIES 1745A. Features. Typical Applications. Major Ratings and Characteristics. Bulletin I25194 rev. B 01/00. case style A-24 (K-PUK)

ST1230C..K SERIES 1745A. Features. Typical Applications. Major Ratings and Characteristics. Bulletin I25194 rev. B 01/00. case style A-24 (K-PUK) ST1230C..K SERIES PHASE CONTROL THYRISTORS Hockey Puk Version Features Center amplifying gate Metal case with ceramic insulator International standard case A-24 (K-PUK) High profile hockey-puk 1745A Typical

More information

IES INDOOR REPORT PHOTOMETRIC FILENAME : RDISE24-LED48FRDMV35.IES. DESCRIPTION INFORMATION (From Photometric File)

IES INDOOR REPORT PHOTOMETRIC FILENAME : RDISE24-LED48FRDMV35.IES. DESCRIPTION INFORMATION (From Photometric File) DESCRIPTION INFORMATION (From Photometric File) IESNA:LM-63-2002 [TEST] LLIA000653-006 [TESTLAB] LightLab International Allentown, LLC [MANUFAC] Mobern Lighting Co., 8200 Stayton Drive, Jessup, MD 20794,

More information

Acoustic Quantities. LMS Test.Lab. Rev 12A

Acoustic Quantities. LMS Test.Lab. Rev 12A Acoustic Quantities LMS Test.Lab Rev 12A Copyright LMS International 2012 Table of Contents Chapter 1 Acoustic quantities... 5 Section 1.1 Sound power (P)... 5 Section 1.2 Sound pressure... 5 Section

More information

Nonlinear Modeling of a Guitar Loudspeaker Cabinet

Nonlinear Modeling of a Guitar Loudspeaker Cabinet 9//008 Nonlinear Modeling of a Guitar Loudspeaker Cabinet David Yeh, Balazs Bank, and Matti Karjalainen ) CCRMA / Stanford University ) University of Verona 3) Helsinki University of Technology Dept. of

More information

Q1. A) 53.3 cm/s B) 59.8 cm/s C) 77.5 cm/s D) 35.1 cm/s E) 44.7 cm/s. Ans: 1.6 Q2.

Q1. A) 53.3 cm/s B) 59.8 cm/s C) 77.5 cm/s D) 35.1 cm/s E) 44.7 cm/s. Ans: 1.6 Q2. Coordinator: Dr. W. Al-Basheer Wednesday, July 11, 2018 Page: 1 Q1. A string of 80.0 cm length is fixed at both ends. The string oscillates in the fundamental mode with a frequency of 60.0 Hz and a maximum

More information

Investigation of the Thermal Noise of MOS Transistors under Analog and RF Operating Conditions

Investigation of the Thermal Noise of MOS Transistors under Analog and RF Operating Conditions Investigation of the Thermal Noise of MOS Transistors under Analog and RF Operating Conditions Ralf Brederlow 1, Georg Wenig 2, and Roland Thewes 1 1 Infineon Technologies, Corporate Research, 2 Technical

More information

APPLICATION OF THE FINITE ELEMENT METHOD TO MODEL THE NONLINEAR VOICE COIL MOTION PRODUCED BY A LOUDSPEAKER MAGNET ASSEMBLY.

APPLICATION OF THE FINITE ELEMENT METHOD TO MODEL THE NONLINEAR VOICE COIL MOTION PRODUCED BY A LOUDSPEAKER MAGNET ASSEMBLY. APPLICATION OF THE FINITE ELEMENT METHOD TO MODEL THE NONLINEAR VOICE COIL MOTION PRODUCED BY A LOUDSPEAKER MAGNET ASSEMBLY. Mark Dodd Celestion International & KEF Audio (UK) Ltd. 1. INTRODUCTION Moving

More information

Simple harmonic motion the motion of springs is a very important topic in physics.

Simple harmonic motion the motion of springs is a very important topic in physics. Chapter 11 Potential and Kinetic Energy Together: Simple Harmonic Motion In This Chapter Using Hooke s law Working with simple harmonic motion Calculating simple harmonic motion velcoity Finding simple

More information

Impedance and Loudspeaker Parameter Measurement

Impedance 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 information

ELECTRONICS E # 1 FUNDAMENTALS 2/2/2011

ELECTRONICS E # 1 FUNDAMENTALS 2/2/2011 FE Review 1 ELECTRONICS E # 1 FUNDAMENTALS Electric Charge 2 In an electric circuit it there is a conservation of charge. The net electric charge is constant. There are positive and negative charges. Like

More information

Chapter 6 Work, Energy, and Power. Copyright 2010 Pearson Education, Inc.

Chapter 6 Work, Energy, and Power. Copyright 2010 Pearson Education, Inc. Chapter 6 Work, Energy, and Power What Is Physics All About? Matter Energy Force Work Done by a Constant Force The definition of work, when the force is parallel to the displacement: W = Fs SI unit: newton-meter

More information

Exam 2 Solutions. Note that there are several variations of some problems, indicated by choices in parentheses.

Exam 2 Solutions. Note that there are several variations of some problems, indicated by choices in parentheses. Exam 2 Solutions Note that there are several variations of some problems, indicated by choices in parentheses. Problem 1 Part of a long, straight insulated wire carrying current i is bent into a circular

More information

Single Phase Parallel AC Circuits

Single Phase Parallel AC Circuits Single Phase Parallel AC Circuits 1 Single Phase Parallel A.C. Circuits (Much of this material has come from Electrical & Electronic Principles & Technology by John Bird) n parallel a.c. circuits similar

More information

Alternate Midterm Examination Physics 100 Feb. 20, 2014

Alternate Midterm Examination Physics 100 Feb. 20, 2014 Alternate Midterm Examination Physics 100 Feb. 20, 2014 Name/Student #: Instructions: Formulas at the back (you can rip that sheet o ). Questions are on both sides. Calculator permitted. Put your name

More information

Simulation and measurement of loudspeaker nonlinearity with a broad-band noise excitation

Simulation 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 information

Introduction to Acoustics Exercises

Introduction 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 information

Mathewlal T 1, GauravSingh 2, Chetan Devadiga 3, Nehal Mendhe 3, 1 Mechanical Engineering Department, Fr CRIT, Vashi, Mumbai.

Mathewlal T 1, GauravSingh 2, Chetan Devadiga 3, Nehal Mendhe 3, 1 Mechanical Engineering Department, Fr CRIT, Vashi, Mumbai. Demonstration of Thermo Acoustic Refrigeration by Setting up an Experimental Model Mathewlal T 1, GauravSingh 2, Chetan Devadiga 3, Nehal Mendhe 3, 1 Mechanical Engineering Department, Fr CRIT, Vashi,

More information

ST223C..C SERIES 390A. Features. Typical Applications. Major Ratings and Characteristics. Bulletin I25174 rev. B 04/00. case style TO-200AB (A-PUK)

ST223C..C SERIES 390A. Features. Typical Applications. Major Ratings and Characteristics. Bulletin I25174 rev. B 04/00. case style TO-200AB (A-PUK) ST223C..C SERIES INVERTER GRADE THYRISTORS Hockey Puk Version Features Metal case with ceramic insulator International standard case TO-0AB (A-PUK) All diffused design Center amplifying gate Guaranteed

More information

MOLEX TAIWAN LTD ( GC ) TITLE : SINGLE PORT UP-RIGHT TYPE USB CONNECTOR

MOLEX TAIWAN LTD ( GC ) TITLE : SINGLE PORT UP-RIGHT TYPE USB CONNECTOR SINGLE PORT UP-RIGHT TYPE USB CONNECTOR 971205 1 of 8 1.0 SCOPE This specification covers the USB series product. 2.0 APPLICABLE DOCUMENTS The following documents form a part of this specification to the

More information

Lithium Sulfur Dioxide (LiSO 2 )

Lithium Sulfur Dioxide (LiSO 2 ) EaglePicher Technologies, LLC Commercial Power P.O. Box 47 Joplin, MO 64802 (417) 623-8000 inquiry.keeper@eaglepicher.com Lithium Sulfur Dioxide (LiSO 2 ) EaglePicher has design and manufacturing capabilities

More information

The Effects of Noise and Time Delay on RWM Feedback System Performance

The Effects of Noise and Time Delay on RWM Feedback System Performance The Effects of Noise and Time Delay on RWM Feedback System Performance O. Katsuro-Hopkins, J. Bialek, G. Navratil (Department of Applied Physics and Applied Mathematics, Columbia University, New York,

More information

N5 H AH Physical Quantity Symbol Unit Unit Abbrev. 5 absorbed dose D gray Gy

N5 H AH Physical Quantity Symbol Unit Unit Abbrev. 5 absorbed dose D gray Gy 5 absorbed dose D gray Gy 5 absorbed dose rate D gray per second gray per hour gray per year Gys -1 Gyh -1 Gyy -1 5 6 7 acceleration a metre per second per second m s -2 5 6 7 acceleration due to gravity

More information

Series CCT-58S Multi-Throw DC 18 GHz, SP7T & SP8T Normally Open Coaxial Switch

Series CCT-58S Multi-Throw DC 18 GHz, SP7T & SP8T Normally Open Coaxial Switch PART NUMBER CCT-58S DESCRIPTION Commercial Normally Open Multi-throw, DC-18 GHz The CCT-58S/CT-58S is an internally terminated, broadband, multi-throw, electromechanical coaxial switch designed to switch

More information

Prof. Shayla Sawyer CP08 solution

Prof. Shayla Sawyer CP08 solution What does the time constant represent in an exponential function? How do you define a sinusoid? What is impedance? How is a capacitor affected by an input signal that changes over time? How is an inductor

More information

ST333C..L SERIES 620A. Features. Typical Applications. Major Ratings and Characteristics. Bulletin I25187 rev. B 04/00. case style TO-200AC (B-PUK)

ST333C..L SERIES 620A. Features. Typical Applications. Major Ratings and Characteristics. Bulletin I25187 rev. B 04/00. case style TO-200AC (B-PUK) ST333C..L SERIES INVERTER GRADE THYRISTORS Hockey Puk Version Features Metal case with ceramic insulator International standard case TO-AC (B-PUK) All diffused design Center amplifying gate Guaranteed

More information

University of Kentucky

University of Kentucky Introduction David Herrin Wave Animation http://www.acs.psu.edu/drussell/demos/waves-intro/waves-intro.html 2 Wave Motion Some Basics Sound waves are pressure disturbances in fluids, such as air or hydraulic

More information

EF 152 Final Exam - Fall, 2016 Page 1 Copy 169

EF 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 information

inter.noise 2000 The 29th International Congress and Exhibition on Noise Control Engineering August 2000, Nice, FRANCE

inter.noise 2000 The 29th International Congress and Exhibition on Noise Control Engineering August 2000, Nice, FRANCE Copyright SFA - InterNoise 2000 1 inter.noise 2000 The 29th International Congress and Exhibition on Noise Control Engineering 27-30 August 2000, Nice, FRANCE I-INCE Classification: 1.4 ON TWIN-SCREW COMPRESSOR

More information

Chapter 4. Energy. Work Power Kinetic Energy Potential Energy Conservation of Energy. W = Fs Work = (force)(distance)

Chapter 4. Energy. Work Power Kinetic Energy Potential Energy Conservation of Energy. W = Fs Work = (force)(distance) Chapter 4 Energy In This Chapter: Work Kinetic Energy Potential Energy Conservation of Energy Work Work is a measure of the amount of change (in a general sense) that a force produces when it acts on a

More information

Chapter 31 Electromagnetic Oscillations and Alternating Current LC Oscillations, Qualitatively

Chapter 31 Electromagnetic Oscillations and Alternating Current LC Oscillations, Qualitatively Chapter 3 Electromagnetic Oscillations and Alternating Current LC Oscillations, Qualitatively In the LC circuit the charge, current, and potential difference vary sinusoidally (with period T and angular

More information

Operating limits and tolerances of platinum resistance thermometers per EN 60751: 2008

Operating limits and tolerances of platinum resistance thermometers per EN 60751: 2008 Technical information Operating limits and tolerances of platinum resistance thermometers per EN 60751: 2008 WIKA data sheet IN 00.17 General information Temperature is a measurement for the thermal state

More information

IES INDOOR REPORT PHOTOMETRIC FILENAME : PFXC-CW-0-277E5-35WH-1.IES. DESCRIPTION INFORMATION (From Photometric File)

IES INDOOR REPORT PHOTOMETRIC FILENAME : PFXC-CW-0-277E5-35WH-1.IES. DESCRIPTION INFORMATION (From Photometric File) DESCRIPTION INFORMATION (From Photometric File) IESNA:LM-63-2002 [TEST] 3610-2.0 [ECN] 3658 [TESTLAB] Tempo LLC [ISSUEDATE] 10/29/2018 9:53:53 AM [MANUFAC] Tempo LLC [LUMCAT] pfxc-cw-0-277e5-35wh-1 [LUMINAIRE]

More information

Ljud i byggnad och samhälle (VTAF01) Sound propagation outdoors MATHIAS BARBAGALLO DIVISION OF ENGINEERING ACOUSTICS, LUND UNIVERSITY

Ljud i byggnad och samhälle (VTAF01) Sound propagation outdoors MATHIAS BARBAGALLO DIVISION OF ENGINEERING ACOUSTICS, LUND UNIVERSITY Ljud i byggnad och samhälle (VTAF01) Sound propagation outdoors MATHIAS BARBAGALLO DIVISION OF ENGINEERING ACOUSTICS, LUND UNIVERSITY recap from last lectures Pressure waves For a sound to be perceived

More information

3 Modeling and Simulation

3 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 information

Consider a simple RC circuit. We might like to know how much power is being supplied by the source. We probably need to find the current.

Consider a simple RC circuit. We might like to know how much power is being supplied by the source. We probably need to find the current. AC power Consider a simple RC circuit We might like to know how much power is being supplied by the source We probably need to find the current R 10! R 10! is VS Vmcosωt Vm 10 V f 60 Hz V m 10 V C 150

More information

ST700C..L SERIES 910A. Features. Typical Applications. Major Ratings and Characteristics. Bulletin I25190 rev. D 04/00. case style TO-200AC (B-PUK)

ST700C..L SERIES 910A. Features. Typical Applications. Major Ratings and Characteristics. Bulletin I25190 rev. D 04/00. case style TO-200AC (B-PUK) ST0C..L SERIES PHASE CONTROL THYRISTORS Hockey Puk Version Features Center amplifying gate Metal case with ceramic insulator International standard case TO-0AC (B-PUK) 910A Typical Applications DC motor

More information

RADIO AMATEUR EXAM GENERAL CLASS

RADIO AMATEUR EXAM GENERAL CLASS RAE-Lessons by 4S7VJ 1 CHAPTER- 2 RADIO AMATEUR EXAM GENERAL CLASS By 4S7VJ 2.1 Sine-wave If a magnet rotates near a coil, an alternating e.m.f. (a.c.) generates in the coil. This e.m.f. gradually increase

More information

04-Electric Power. ECEGR 452 Renewable Energy Systems

04-Electric Power. ECEGR 452 Renewable Energy Systems 04-Electric Power ECEGR 452 Renewable Energy Systems Overview Review of Electric Circuits Phasor Representation Electrical Power Power Factor Dr. Louie 2 Introduction Majority of the electrical energy

More information

Q1. For a given medium, the wavelength of a wave is:

Q1. For a given medium, the wavelength of a wave is: Phys10 First Major-091 Zero Version Coordinator: M Sunday, Noveber 15, 009 Page: 1 Q1. For a given ediu, the wavelength of a wave is: A) inversely proportional to the frequency B) independent of the frequency

More information

Mechatronic 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 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 information

Gen. Phys. II Exam 1 - Chs. 18,19,20 - Electric Fields, Potential, Current Feb. 12, 2018

Gen. Phys. II Exam 1 - Chs. 18,19,20 - Electric Fields, Potential, Current Feb. 12, 2018 Gen. Phys. II Exam 1 - Chs. 18,19,20 - Electric Fields, Potential, Current Feb. 12, 2018 Rec. Time Name For full credit, make your work clear. Show formulas used, essential steps, and results with correct

More information

Q1. In a stretched string the frequency of the wave DOES NOT depends on:

Q1. In a stretched string the frequency of the wave DOES NOT depends on: Coordinator: Al-Shukri Wednesday, June 08, 011 Page: 1 Q1. In a stretched string the frequency of the wave DOES NOT depends on: A) Amplitude of the wave B) Wavelength of the wave C) Velocity of the wave

More information

Lecture # 3: Wind Tunnels and Water Tunnels

Lecture # 3: Wind Tunnels and Water Tunnels ere 344 - Lecture Notes Lecture # 3: Wind Tunnels and Water Tunnels Dr. Hui Hu Dr. Rye Waldman Department of erospace Engineering Iowa State University mes, Iowa 50011, U.S. Sources/ Further reading: Barlow,

More information

H -Control of Acoustic Noise in a Duct with a Feedforward Configuration

H -Control of Acoustic Noise in a Duct with a Feedforward Configuration H -Control of Acoustic Noise in a Duct with a Feedforward Configuration K.A. Morris Department of Applied Mathematics University of Waterloo Waterloo, Ontario N2L 3G1 CANADA Abstract A mathematical model

More information

The Use of Multiphysics Models in the Design and Simulation of Magnetostrictive Transducers. Dr. Julie Slaughter ETREMA Products, Inc Ames, IA

The Use of Multiphysics Models in the Design and Simulation of Magnetostrictive Transducers. Dr. Julie Slaughter ETREMA Products, Inc Ames, IA The Use of Multiphysics Models in the Design and Simulation of Magnetostrictive Transducers Dr. Julie Slaughter ETREMA Products, Inc Ames, IA 1 ETREMA Products, Inc. Designer and manufacturer of technology

More information

Double Thyristor Module For Phase Control MT A2

Double Thyristor Module For Phase Control MT A2 Electrically isolated base plate Industrial standard package Simplified mechanical design, rapid assembly Pressure contact PROTON-ELECTROTEX RUSSIA Double Thyristor Module For Phase Control MT3-595-18-A2

More information

EXP. NO. 3 Power on (resistive inductive & capacitive) load Series connection

EXP. NO. 3 Power on (resistive inductive & capacitive) load Series connection OBJECT: To examine the power distribution on (R, L, C) series circuit. APPARATUS 1-signal function generator 2- Oscilloscope, A.V.O meter 3- Resisters & inductor &capacitor THEORY the following form for

More information

Ch. 23 Electromagnetic Induction, AC Circuits, And Electrical Technologies

Ch. 23 Electromagnetic Induction, AC Circuits, And Electrical Technologies Ch. 23 Electromagnetic Induction, AC Circuits, And Electrical Technologies Induced emf - Faraday s Experiment When a magnet moves toward a loop of wire, the ammeter shows the presence of a current When

More information