Noise Lecture 1. EEL6935 Chris Dougherty (TA)

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1 Noise Lecture 1 EEL6935 Chris Dougherty (TA)

2 An IEEE Definition of Noise The IEEE Standard Dictionary of Electrical and Electronics Terms defines noise (as a general term) as: unwanted disturbances superposed upon a useful signal that tend to obscure its information content. Applies both to intrinsic and extrinsic noise intrinsic noise is the noise generated inside components themselves extrinsic noise designates noise originating elsewhere

Extrinsic Noise (interference) Due to: Cross-talk between circuits E/M (Lightning) Grounding issues Unwanted coupling of AC power supply + harmonics Examples (symptoms of)

3 Extrinsic Noise (interference) Due to: Cross-talk between circuits E/M (Lightning) Grounding issues Unwanted coupling of AC power supply + harmonics Examples (symptoms of) AM/FM radio (especially AM!) during lightning storm Hum or buzz of electric guitar (from lights, etc) When using portable phone and hear unwanted third party conversation on the line

4 Intrinsic Noise Due to: Resistor thermal noise BJT/diode shot noise MOS thermal (broadband) and flicker (low-freq) noise Examples (or rather symptoms of) The shhhhh sound of analog TV when signal lost snow on the TV screen when signal lost Tape hiss heard in old recordings

5 To Reiterate: Two General Categories of Noise Extrinsic Interference, a better term Unwanted signals coupled from sources outside, not due to circuit elements themselves Solutions: Topology choice, grounding, shielding Intrinsic Fundamental noise Inherent to all active devices, resistors Statistical in nature Solution: Careful design to minimize effect

6 This lecture focuses on intrinsic sources of noise (but both have major impact in bio applications) From here on noise implies intrinsic noise, unless specified.

7 Noise Noise is random in amplitude and phase Possible to predict the randomness of noise Mean (often is zero) Standard deviation Equal to the RMS value of the noise V NOISE_RMS σ Noise waveform and Gaussian distribution of noise amplitudes

8 Gaussian Noise Distribution Probability Density (ρ) ρ e V V ( ) RMS V ππ RMS Instantaneous Noise Amplitude

9 Gaussian Noise Distribution ρ e V RMS V ( V ) RMS π V RMS T 1 T 0 v ( t ) dt Recall that V RMS is the same as the standard deviation, σ Thus, the instantaneous noise amplitude is within +/- 3σ (3 x V RMS ) ~99.7% of the time.

10 Noise Examples mentioned show that problems due to noise are apparent at the output Sources of noise unique to low-level circuitry, typically input stage A 1 A + V NOISE1 V NOISE R L V OUT - V OUT V A A NOISE1 1 Assuming A 1 is much greater than 1, VNOISE1 dominates and we can ignore the output noise contribution of V NOISE.

11 Thermal Noise (aka Johnson noise, Nyquist noise) Due to random motion of electrons in conductor when above absolute zero temperature Resistor Noise Model From Nyquist: R Available Noise Power P AVAIL k T f V NOISE Noiseless k1.38x10-3 J/K (Boltzmann s constant) T is temp in K f is the noise bandwidth 3dB bandwidth V NOISE?

12 Thermal Noise Find V NOISE from Available Noise Power Eqn 1. P AVAIL k T Resistor Noise Model R f V OUT Conjugate Match for max power transfer; P OUT under this condition is P AVAIL. Find expression for P AVAIL in terms of V NOISE RL VOUT VNOISE R + R I P OUT AVAIL V R NOISE L P + OUT R L V R V OUT NOISE I V OUT NOISE VNOISE 4 R V NOISE I OUT R L R Eqn. P AVAIL V NOISE 4 R

13 Thermal Noise Find V NOISE from Available Noise Power P AVAIL Eqn 1. k T f Eqn. P AVAIL VNOISE 4 R V NOISE? Let Eqn 1. Eqn. Find V NOISE Resistor Noise Model k T f VNOISE 4 R R V NOISE 4kTR f V NOISE Note: Thermal noise applies only to true physical resistances, anything that represents energy loss from a system has thermal noise. r π from BJT model does NOT contribute thermal noise.

14 Thermal Noise V NOISE 4kTR f I NOISE kt f 4 R Resistor Noise Models R V NOISE I NOISE R (From Norton s theorem)

15 Thermal Noise What about R in series? R 1 R 1 + R R 1NOISY R N1 V N V + V R NOISY V N1 4kT fr1 + 4kT fr R 1 + R V N ( R R ) 4kT f + 1

16 Thermal Noise What about R in parallel? R 1 I R R I 1 //R N1 N N1 I + I N I N1 + I N 4kT f R 1 + 4kT f R 4kT f R R R 1 + 4kT f R R R 1 1 I N1 + I N 4kT f ( R R R 1 + R 1 ) 4kT f R // 1 R

3dB Bandwidth Typically, the bandwidth of a filter is specified in terms of 3db (half-power) bandwidth For a given transfer function, bandwidth spans the frequency

17 3dB Bandwidth Typically, the bandwidth of a filter is specified in terms of 3db (half-power) bandwidth For a given transfer function, bandwidth spans the frequency range where the magnitude is greater than 3dB down from maximum gain. Can be easily measured by driving the circuit with a sinusoidal source and monitoring output level

18 Noise Bandwidth NOT same as 3dB (half-power) bandwidth Noise bandwidth defined in terms of the voltage-gain squared (power gain) Defined for a system with uniform gain throughout passband and zero gain outside Shaped like ideal brick-wall filter Since real systems exhibit practical roll-offs, we need to define bandwidth in a manner consistent with the noise equations

19 Uniform gain in baseband Noise Bandwidth f B A A( f ) df Actual Response and equivalent noise bandwidth (low-pass). Drawn in linear scale.

20 V IN f 0 R 1 π RC Noise Bandwidth Example C V OUT A( f ) 1 1 f f A f 0 f 0 A( f ) df f f 1+ df df f f + f f tanθ 0 Using trigonometric substitution: let so f f 0 π / 0 dθ f f π f 0 df f0 sec θ dθ Noise bandwidth is 1.57*BW 3dB for circuits with 1 st order roll-off

21 Relating Noise & 3dB Bandwidths Using circuit roll-off behavior (based on number of poles) can convert 3dB bandwidth to noise bandwidth Use conversion factor # of Poles f/bw 3db High Frequency rolloff (db/decade)

22 Thermal Noise vs. R and f Thermal Noise Voltage (µv) Resistance (kω)

23 Noise Spectral Density Noise Spectral Density is the mean-square value of the noise per unit bandwidth S S Can be defined in terms of V or I Noise spectral density of thermal noise is independent of frequency v i ( ( f f ) ) noise v f noise i f 4kTR Thermal noise is described as white noise because the energy is equal across all frequencies, an analogy to white light (equal light energy over all wavelengths). 4kT R

24 Spot noise Spot noise RMS value of the noise in a noise bandwidth of 1Hz. Units of Volts/sqrt(Hz) or Amps/sqrt(Hz) v noise f S v ( f ) 4kTR i noise f S i ( f ) 4kT R

25 Example: Thermal Noise What is spot noise of 1kΩ resistor at 300K? Use this to find V noise for 100kΩin 1MHz bandwidth 4kT is 1.6x10-0 at room temp (90K) v noise 0 4kT R f 4.07 nv/sqrt(hz)

26 Example: Thermal Noise Cont. What is spot noise of 1kΩ resistor at 300K? Use this to find V noise for 100kΩ in 1MHz bandwidth 4kT is 1.6x10-0 at room temp (90K) v noise For the 100kΩ resistor, V noise is: v noise f f R nv Hz 10 3 V noise 1.7 mv rms

27 Noise Floor Going back to Nyquist s expression for P AVAIL at room temperature (90K): P AVAIL k T f (Watts) Put in terms of dbm: log dBm Minimum noise level that is practically achievable in a system operating at room temperature. Thermal noise represents a minimum level of noise.

28 R OUT and Voltage Noise Ideal Amp with Gain A R out 0 R 1 A 4kTR 1 f R load 4kTR f load

29 R out : non-zero (otherwise ideal) R 1 R out V out 4kTR 1 f V in R IN A V in R load 4kTR f load (Semi) Ideal Amplifier

30 Shot Noise Present in diodes, transistors first observed in vacuum tubes Current flow across a potential barrier DC Current is actually the sum of many discrete events when a carrier crosses barrier I SHOT qi DC f RMS noise current, also white q is the electronic charge 1.6 x Coulombs I DC is bias current in Amps f is the noise bandwidth

31 Avalanche Noise Due to Zener or avalanche breakdown in a PN junction When breakdown occurs EHPs created Results in noise produced that is much greater than that of shot noise of same current Be cautious with zener based voltage references if noise is a concern

32 1/f Noise Low-frequency noise, NOT white AKA flicker noise Associated with contamination and crystal defects in all active devices Also present in carbon resistors (consider metal film instead)

33 1/f Noise (see Gray/Meyer) Note inverse dependence on frequency i d K I a D f f I D is the drain bias current (this is for long channel MOSFETs) K is a constant based on the device/technology a is a constant between 0.5 and

35 Example R 1 R 4 V out R s C R L C V s ~ R R 3 C

36 E.I.N. Model

37 E.I.N

38 E.I.N. Model

39 kt/c Noise

40 Resources EEE530 & EEE631 Notes (Dr. Fox) Low-Noise Electronic System Design by Motchenbacher and Connelly Electronic Noise and Interfering Signals by Vasilescu Noise Reduction Techniques in Electronic Systems by Ott

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