Low Noise Amplifier Design

Slides:



Advertisements
Similar presentations
Noise Lecture 6.
Advertisements

Analytical figures of merit, noise, and S/N ratio Chemistry 243.
1.6 Op-Amp Basics High input impedance Low output impedance Made using difference amplifiers having 2 inputs and at least 1 output 1 Note: Terminals for.
Chapter 3. Noise Husheng Li The University of Tennessee.
ENTC 4350 HOMEWORK SET 3 Chapter 5.
Signal vs. Noise Every measurement is affected by processes not related to the measurement of interest. The magnitude of this noise, compared to the magnitude.
Storey: Electrical & Electronic Systems © Pearson Education Limited 2004 OHT 5.1 Signals and Data Transmission  Introduction  Analogue Signals  Digital.
Electrical Noise Wang C. Ng.
CERN Technical Training 2005
Equivalent Circuits - Resistors Resistor noise is dominated by thermal noise: Noiseless Resistor Noisy Resistor Noise Source.
Lecture 31 Electrical Instrumentation. Lecture 32 Electrical Instrumentation Electrical instrumentation is the process of acquiring data about one or.
Lecture161 Instrumentation Prof. Phillips March 14, 2003.
Fiber-Optic Communications
Prof. ParkELC 2221 Lecture 1: Introductory Topics Prof. Park ELC 222 Essex County College.
Chem. 133 – 2/17 Lecture. Announcements Lab Work –Electronics Lab Report due 2/19 –Let me know by today if you plan to do a lab practical instead –Half.
Z. Ghassemlooy 1 Noise in Communication Systems Professor Z Ghassemlooy Electronics and IT Division School of Engineering Sheffield Hallam University U.K.
Operation Amplifier. Golden Rules of OP Amp 1.i in =0, no current flow into op amp. 2.V + =V - Typically one end of op amp is connected to ground, therefore,
Chapter 5 Signals and Noise  Signal carries information about the analyte that is of interest to us.  Noise is made up of extraneous information that.
Chapter 5: Signals and Noise
CHAPTER Noise 5.2 Transmission Media & EM Propagations.
RFIC Design and Testing for Wireless Communications A PragaTI (TI India Technical University) Course July 18, 21, 22, 2008 Lecture 4: Testing for Noise.
Lecture 8: Oscillators Noise in electronic systems
Noise characteristics Reference: [4] The signal-to-noise ratio is the measure for the extent to which a signal can be distinguished from the background.
Current and Direct Current Circuits
COMMUNICATION SYSTEM EECB353 Chapter 4 NOISE ANALYSIS
5. SOURCES OF ERRORS Noise types
ECE 590 Microwave Transmission for Telecommunications Noise and Distortion in Microwave Systems March 18, 25, 2004.
EBB Chapter 2 SIGNALS AND SPECTRA Chapter Objectives: Basic signal properties (DC, RMS, dBm, and power); Fourier transform and spectra; Linear systems.
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.
1 In order to reduce errors, the measurement object and the measurement system should be matched not only in terms of output and input impedances, but.
Noise characteristics Reference: [4] The signal-to-noise ratio is the measure for the extent to which a signal can be distinguished from the background.
Biomedical Instrumentation Signals and Noise Chapter 5 in Introduction to Biomedical Equipment Technology By Joseph Carr and John Brown.
ECE 4710: Lecture #3 1 Signals & Noise  Received waveform contains the desired signal and the undesired noise  We will use deterministic waveforms (not.
1 In order to reduce errors, the measurement object and the measurement system should be matched not only in terms of output and input impedances, but.
Ya Bao, South Bank University 1 Noise Richard Read, The Essence of Communications Theory, Chapter 3.
CHAPTER Noise 5.2 Transmission Media & EM Propagations EKT 231 : COMMUNICATION SYSTEM CHAPTER 5 : NOISE IN COMMUNICATION SYSTEM.
Introduction to Analog And Digital Communications Second Edition Simon Haykin, Michael Moher.
Sources of noise in instrumental analysis
NOISE IN COMMUNICATION CHANNELS
1 LECTURE 7. Contents 5.Sources of errors 5.1.Impedance matching Non-energetic matching Energetic matching Non-reflective matching To.
Chapter 10: Noise In Microwave Circuits
TELECOMMUNICATIONS Dr. Hugh Blanton ENTC 4307/ENTC 5307.
EEM3A – Analogue Electronics Dr. T. Collins
Chapter 26 Lecture 22: Current: II
Electronic Noise Noise phenomena Device noise models
Chapter 1 : Part 3 Noise. Noise, interference and distortion  Noise  unwanted signals that coincide with the desired signals.  Two type of noise: internal.
ECE 4710: Lecture #37 1 Link Budget Analysis  BER baseband performance determined by signal to noise ratio ( S / N ) at input to detector (product, envelope,
Noise characteristics Reference: [4] The signal-to-noise ratio is the measure for the extent to which a signal can be distinguished from the background.
CHAPTER 1 Part 2.1  Noise.
Noise in communication system
NOISE in Audio Systems Today we have a VIP guest in our class. His name is:
Feedback.
OHM’S LAW AND ELECTRICAL POWER. OHM’S LAW “Provided the physical conditions, such as temperature, are kept constant, the resistance is constant over a.
CHAPTER 1 (cont…) Part 2.1  Noise. Objectives To differentiate the types of noise To calculate the thermal noise generated by a resistor To calculate.
Noise characteristics Reference: [4] The signal-to-noise ratio is the measure for the extent to which a signal can be distinguished from the background.
TE4201-Communication Electronics 1 2. Noise and Frequency Spectrum  AM communications system AM communications systemAM communications system  Noise.
1.1 What is Noise? any ‘unwanted” part of the analytical signal always some noise in a signal 1.2 Signal-to-noise ratio (S/N) for a set of data (replicate.
1 Noise Analysis Electrical Noise Electrical noise is defined as any undesirable electrical energy. Figure 57 shows the effect of noise on an electrical.
Noise in Communication Systems
What is thermal noise? Thermal noise in the resistance of the signal source is the fundamental limit on achievable signal sensitivity is unavoidable, and.
EE354 : Communications System I
Chem. 133 – 2/14 Lecture.
Analog Communication.
Random Signals and Noise
Chapter 5: Signals and Noise
Noise Figure Measurement using Natural Noise Sources
Differential Op - Amplifier TIM. 1 Introduction 2 Differential Amplifier: 2.1 Input Resistances: 2.2 Differential Gain: 2.3 Common Mode Input: 2.4 Common.
OP-AMPS: basics & Inverting-amplifier
Electronic Noise Noise phenomena Device noise models
Noise I Abigail Firme.
Presentation transcript:

Low Noise Amplifier Design Sources of Noise Low Noise Design

Sources of Noise Ambient Noise. Electrical Interference. Eg. Background noise in a recording Electrical Interference. Eg. Mains hum, mobile phones Amplifier Noise. Noise added by the amp

Sources of Amplifier Noise Thermal Noise Resistive components Shot Noise Semiconductor junctions Flicker Noise All components

Thermal Noise Random motion of electrons in a conductor (Brownian motion) causes thermal noise. It is a white Gaussian noise voltage of magnitude: k = Boltzmann’s constant T = Temperature [Kelvin] R = Resistance B = Bandwidth

White Noise |N(f)|2 frequency Flat spectrum extending to infinity implies a signal with infinite r.m.s. voltage – obviously impossible. In practice, interest is restricted to a finite band of frequencies.

Band-Limited White Noise |N(f)|2 frequency N(t) time

Band-Limited Thermal Noise The r.m.s. voltage level of a band-limited white noise signal is proportional to the square root of the bandwidth. For thermal noise: or,

Shot Noise - - - - - - - Current a number of carriers per second Dominates in semiconductor devices when carriers are diffusing. (In conductors, thermal noise is usually much bigger) - - - - - - - Current a number of carriers per second

Shot Noise Current The average number of carriers flowing past a point per second is proportional to the current. In any observation interval, the actual number of carriers will vary around this average – this variation is shot noise.

Flicker Noise Imperfections in the fabrication of a component cause flicker noise. Unlike thermal noise and shot noise, flicker noise is not white; it is pink. Also, it can be reduced depending on the quality of the component.

Flicker Noise Current f = frequency, K = component dependent constant. Note that the noise power is inversely proportional to frequency – i.e. pink noise.

Noise in Amplifiers A noisy amplifier Equivalent circuit

Noise Figure Noise from RS: Signal-to-noise ratio for vin: Equivalent circuit of a noisy amplifier with a noisy input.

Equivalent circuit of a noisy amplifier with a noisy input. Noise voltage level at the output will be the r.m.s. sum of the resistor noise and the amplifier noise. (Add power, not voltage) Output signal-to-noise ratio is, therefore: Equivalent circuit of a noisy amplifier with a noisy input.

The Noise Figure of the amplifier is the ratio between the output and input signal-to-noise ratios:

Noise Temperature RS vS RS Ideal amp RS is heated to Tn but amp is ideal vS Noisy amp If RS is cooled to zero:

The noise temperature of the amplifier is the value of Tn where: Noise temperature and noise figure are related since:

Introduction to Noise – Summary The main sources of amplifier noise are thermal noise, shot noise and flicker noise. Thermal noise and shot noise are both white and are irreducible. Flicker noise is pink and can be controlled. The noise performance of an amplifier can be quantified by either its Noise Figure or Noise Temperature.