NOISE in Audio Systems Today we have a VIP guest in our class. His name is:

Slides:



Advertisements
Similar presentations
Noise Lecture 6.
Advertisements

CHAPTER 3: SPECIAL PURPOSE OP-AMP CIRCUITS
LECTURE6 CT1303 LAN. DATA IMPAIRMENTS Thermal Noise شوشرة حرارية is the electronic noise generated by the thermal agitation of the charge carriers (usually.
Frequency modulation and circuits
Chapter 1 Problems ECET 214 Prof. Park NJIT.
ENTC 4350 HOMEWORK SET 3 Chapter 5.
Principles of Electronic Communication Systems Second Edition Louis Frenzel © 2002 The McGraw-Hill Companies.
Chem. 133 – 2/19 Lecture. Announcements Lab Work –Turn in Electronics Lab –Starting Set 2 HW1.2 Due Today Quiz 2 Today Today’s Lecture –Noise –Electrochemistry.
Chapter 7 Principles of Analog Synthesis and Voltage Control Contents Understanding Musical Sound Electronic Sound Generation Voltage Control Fundamentals.
Low Noise Amplifier Design
Department of Electronic Engineering City University of Hong Kong EE3900 Computer Networks Data Transmission Slide 1 Continuous & Discrete Signals.
Lecture161 Instrumentation Prof. Phillips March 14, 2003.
3.1 Chapter 3 Data and Signals Copyright © The McGraw-Hill Companies, Inc. Permission required for reproduction or display.
Electric Currents Physics Department, New York City College of Technology.
Prof. ParkELC 2221 Lecture 1: Introductory Topics Prof. Park ELC 222 Essex County College.
Copyright © 2009 Pearson Education, Inc. Lecture 10 – AC Circuits.
Lecture 101 Capacitors (5.1); Inductors (5.2); LC Combinations (5.3) Prof. Phillips March 7, 2003.
1 Announcements l Bring motors to lab this week. l Bring eight 1N4001 diodes to lab per team. Get them at the Scientific Supply Store (2 nd Floor Sciences.
Circuit Theory What you will use this for –Power management –Signals between subsystems –Possible analog data types How the knowledge will help you –Understanding.
Chapter 5: Signals and Noise
OSCILLATORS.
Engineering H192 - Computer Programming Gateway Engineering Education Coalition Lab 4P. 1Winter Quarter Analog Electronics Lab 4.
Electricity, Electronics And Ham Radio “Kopertroniks” By Nick Guydosh 4/12/07.
1 Complex Gain: Basic amplifier concepts Q: What is a Phasor? A Phasor is an ac voltage or current that maintains the same phase with respect to a standard.
General Licensing Class G7A – G7C Practical Circuits Your organization and dates here.
Chapter 22 Current Electricity.
Copyright © 2009 Pearson Education, Inc. Chapter 30 Inductance, Electromagnetic Oscillations, and AC Circuits.
Lecture 2 Most basic facts from Electricity needed for understanding telecommunications Local transmission lines in the telephone system Decibels Signals.
1 Chelmsford Amateur Radio Society Advanced Licence Course Carl Thomson G3PEM Slide Set 4: v1.2, 20-Aug-2006 (3) Technical Aspects - AC Circuits Chelmsford.
COMMUNICATION SYSTEM EECB353 Chapter 4 NOISE ANALYSIS
Chapter 29 Electromagnetic Induction and Faraday’s Law
09/16/2010© 2010 NTUST Today Course overview and information.
ECE 590 Microwave Transmission for Telecommunications Noise and Distortion in Microwave Systems March 18, 25, 2004.
Engineering H192 - Computer Programming The Ohio State University Gateway Engineering Education Coalition Lab 3P. 1Winter Quarter Analog Electronics Lab.
Noise and Interference Any signal or phenomena which degrades signal to noise ratio (S/N). External 1.Thermal noise (raw or amplified) 2.On-channel unwanted.
Electrical Principles 1 1 G5 - ELECTRICAL PRINCIPLES [3 exam questions - 3 groups] G5A - Reactance; inductance; capacitance; impedance; impedance matching.
TELECOM SPEED OF E.M.WAVES SPEED OF E.M.WAVES 3 x 10 8 m/s 3 x 10 8 m/s 3oo,ooo,ooo m/s.
ELECTRONIC COMMUNICATIONS A SYSTEMS APPROACH CHAPTER Copyright © 2014 by Pearson Education, Inc. All Rights Reserved Electronic Communications: A Systems.
Capacitive transducer. We know that : C=kЄ° (A/d) Where : K=dielectric constant Є° =8.854 *10^-12 D=distance between the plates A=the area over lapping.
Ya Bao, South Bank University 1 Noise Richard Read, The Essence of Communications Theory, Chapter 3.
Copyright © 2009 Pearson Education, Inc. Chapter 33 Inductance, Electromagnetic Oscillations, and AC Circuits Part II.
CHAPTER Noise 5.2 Transmission Media & EM Propagations EKT 231 : COMMUNICATION SYSTEM CHAPTER 5 : NOISE IN COMMUNICATION SYSTEM.
NOISE IN COMMUNICATION CHANNELS
Electrical Production of Sound 1Electric Circuits 2Electric Current 3Resistance 4Voltage 5Ohm’s Law 6Series and Parallel Circuits 7Electric Energy and.
Power Supplies, Batteries, Connectors and Test Equipment.
INTRODUCTION TO ELECTRICAL AND ELECTRONICS ENGINEERING Sakarya Üniversitesi Teknoloji Fakültesi Elektrik Elektronik Mühendisliği Bölümü T4 Blok Introducing.
Physics 213 General Physics Lecture 14. Test 1 1. Click in!!
CHAPTER 1 Part 2.1  Noise.
Electrical Principles 1 1 G5 - ELECTRICAL PRINCIPLES [3 exam questions - 3 groups] G5A - Reactance; inductance; capacitance; impedance; impedance matching.
Noise in communication system
Electromagnetism Lecture#12-13 Instructor: Engr. Muhammad Mateen Yaqoob.
Signal Analyzers. Introduction In the first 14 chapters we discussed measurement techniques in the time domain, that is, measurement of parameters that.
TE4201-Communication Electronics 1 2. Noise and Frequency Spectrum  AM communications system AM communications systemAM communications system  Noise.
EM OSCILLATION & AC. LC oscillation.
Physics 213 General Physics Lecture Last Meeting: Electric Generators, Alternating Current Today: Electromagnetic Waves, Maxwell’s Equations.
6. Unregulated Power Supply Design
1 Noise Analysis Electrical Noise Electrical noise is defined as any undesirable electrical energy. Figure 57 shows the effect of noise on an electrical.
Chapters 17 through 23 Midterm Review. Midterm Exam ~ 1 hr, in class 15 questions 6 calculation questions One from each chapter with Ch. 17 and 18 combine.
Chapter 3 – Diode Circuits – Part 3
Noise in Communication Systems
As Unit 1 - Electricity What you need to know..  Current is the rate of flow of charged particles.  In metals these are conduction electrons, most electrons.
What is thermal noise? Thermal noise in the resistance of the signal source is the fundamental limit on achievable signal sensitivity is unavoidable, and.
Balaji engineering college Special transformer
Inductance, Electromagnetic Oscillations, and AC Circuits
General Licensing Class
NET301 Lecture6 10/22/2015 Lect6 NET301.
OCR 21st Century Science Unit P5 a and b Revision
C H A P T E R 17 A.C. Filter Networks.
INFORMATION CAPACITY AND NOISE
Lecture 2 Electrical and Electronics Circuits. After you study, and apply ideas in this Lecture, you will: Understand differences among resistance, capacitance,
Presentation transcript:

NOISE in Audio Systems

Today we have a VIP guest in our class. His name is:

NOISE in Audio Systems Understanding the nature and the characteristics of noise is very important for the study of Electroacoustic systems.

NOISE in Audio Systems So... What is noise…

NOISE in Audio Systems So... What is noise… The definition of noise is similar to the definition of a weed…!!! What's a weed?...It's the flower you didn't plant and don't want to grow. What's noise?... It's the sound you didn't intentionally create, and don't want to hear.

NOISE in Audio Systems Types of Noise in Audio Systems: White noise……. Pink noise………. Hum……… Buzz…….. Static……. Blue, Brown, Violet, Gray

NOISE in Audio Systems Thermal/Random noise…. Is generated as a result of thermal agitation of the charge carriers which are typically electrons within an electrical conductor. This thermal noise actually occurs regardless of the applied voltage because the charge carriers vibrate as a result of the temperature. Thermal noise appears regardless of the quality of component used. The noise level is dependent only upon the temperature and the value of the resistance.

NOISE in Audio Systems So… What am I going to measure across this resistor with a voltmeter?

NOISE in Audio Systems So… What am I going to measure across this resistor with a voltmeter? A Noise voltage “Vn”

NOISE in Audio Systems So… What am I going to measure across this resistor with a voltmeter? A Noise voltage “Vn” With constant energy across all frequencies

NOISE in Audio Systems Assuming that the value of the resistance remain constant across all frequencies in a given bandwidth, the voltage of the thermal noise will be given by: Where: Vn = integrated RMS voltage between two frequencies. R = resistive component of the impedance (or resistance) Ω. T = temperature in degrees Kelvin. k = Boltzmann constant ( ^-23 J/K ⁰ )

NOISE in Audio Systems Assuming that the value of the resistance remain constant across all frequencies in a given bandwidth, the voltage of the thermal noise will be given by: Where: Vn = integrated RMS voltage between two frequencies. R = resistive component of the impedance (or resistance) Ω. T = temperature in degrees Kelvin. k = Boltzmann constant ( ^-23 J/K ⁰ ) Example: Calculate the thermal noise levels for room temperature, 20°C or 290°K, for a 1 Hz bandwidth, for an impedance of 50 Ω.

NOISE in Audio Systems White noise…. “White noise is unfiltered, unaltered thermal noise”. When the energy content of a white noise signal is averaged (integrated over time), it will be found to contain equal energy per Hz.

NOISE in Audio Systems White noise…. When the energy content of a white noise signal is averaged (integrated over time), it will be found to contain equal energy per Hz. “White noise is unfiltered, unaltered thermal noise”.

NOISE in Audio Systems White noise…. When the energy content of a white noise signal is averaged (integrated over time), it will be found to contain equal energy per Hz. “White noise is unfiltered, unaltered thermal noise”.

NOISE in Audio Systems A B “White noise is unfiltered, unaltered thermal noise”. White noise…. Energy (A) = Energy (B)

NOISE in Audio Systems Plotting the power of white noise, with respect to frequency in a logarithmic scale, will result in a 3 dB per octave buildup in level, as the frequency rises.

But…. What is OCTAVE …

Octave is a music/frequency interval defined by the ratio 2:1 regardless of the starting frequency. The frequency space from 100 Hz to 200 Hz is an octave, as is the interval from 2000 Hz to 4000 Hz.

NOISE in Audio Systems The 3dB-slope concept: For the octave 100->200 we have a frequency window of 100Hz For the octave 200->400 we have a frequency window of 200Hz If the power per Hz is “A” Watt, the total power for the octave 100->200 will be 100A Watt In a similar way the total power for the octave 200->400 will be 200A Watt The increase in dB will be then:

NOISE in Audio Systems Pink noise is white noise that has been modified with a filter that gives a 3 dB per octave roll- off. Pink noise: (Hz) dB

NOISE in Audio Systems Plotting the power of Pink noise, with respect to frequency in a logarithmic scale, will result in a straight line in level, as the frequency rises.

NOISE in Audio Systems As we can see now, pink noise has equal energy per octave, and therefore is more useful as a loudspeaker test and calibration signal.

NOISE in Audio Systems As we can see now, pink noise has equal energy per octave, and therefore is more useful as a loudspeaker test and calibration signal. Pink noise is balanced to more closely simulate the kind of signals the sound system will actually be required to reproduce.

NOISE in Audio Systems As we can see now, pink noise has equal energy per octave, and therefore is more useful as a loudspeaker test and calibration signal. Pink noise is balanced to more closely simulate the kind of signals the sound system will actually be required to reproduce. It is also closer to the way the human hearing performs.

NOISE in Audio Systems All other "coloured" types of noise are actually white noise with a different type of filtering….

NOISE in Audio Systems Noise caused by electric network.... Hum and Buzz……. Hum is generally the result of leakage of AC power line energy into the audio circuit. It can be caused by a poorly isolated power transformer, a power supply problem, ground loops or indirectly by electromagnetic coupling of AC magnetic fields into cables or other components. It is usually sine wave components at 120 Hz, 180 Hz, and other harmonics of 60 Hz. Buzz is similar to hum, but contains harmonically related noise energy across the audio spectrum, including high frequency energy. Static noise can be caused by distant lightning, by intermittent sparking of power lines, generators or electric motors, or by radio frequency energy that enters the sound equipment and is rectified.

NOISE in Audio Systems …Using noise as a test signal is one thing. Finding it at the output of a mixing console, a signal processor or a power amplifier that is supposed to be quiet is quite a problem…. …..So the next session will be, the measurement and the specification of noise in audio systems…