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Analytical figures of merit, noise, and S/N ratio Chemistry 243
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Analytical figures of merit, noise, and S/N ratio Chemistry 243.

Mar 28, 2015

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Page 1: Analytical figures of merit, noise, and S/N ratio Chemistry 243.

Analytical figures of merit, noise, and S/N ratio

Chemistry 243

Page 2: Analytical figures of merit, noise, and S/N ratio Chemistry 243.

Noise A signal is only of analytical value if it can be

definitively attributed to the species/system of interest in the presence of noise.

0.5

1

1.5

2

2.5

0 20 40 60 80 100

data point

sig

nal

0.5

1

1.5

2

2.5

0 20 40 60 80 100

data point

sig

nal

Looks like a real signalProbably noise, or not very useful;

a hint of a signal

Page 3: Analytical figures of merit, noise, and S/N ratio Chemistry 243.

What is signal and noise?

Page 4: Analytical figures of merit, noise, and S/N ratio Chemistry 243.

Signal-to-Noise Ratio (S/N) Signal-to-noise ratio (S/N) is a measure of the

quality of an instrumental measurement Ratio of the mean of the analyte signal to the

standard deviation of the noise signal High value of S/N : easier to distinguish analyte

signal from the noise signal

1

xSN s

SN RSD

Rev. Sci. Inst., 1966, 37, 93-102.

MostlySignal

MostlyNoise

signal

Std. Dev.

Page 5: Analytical figures of merit, noise, and S/N ratio Chemistry 243.

Where does noise come from?

Chemical noise Temperature, pressure, humidity, fumes, etc.

Instrumental noise

Page 6: Analytical figures of merit, noise, and S/N ratio Chemistry 243.

Detector and post-detector noise

Thermal (Johnson) noise Shot noise Flicker (1/f) noise Environmental noise Popcorn (burst) noise Microphonic noise

Page 7: Analytical figures of merit, noise, and S/N ratio Chemistry 243.

Thermal (Johnson) noise

Random motions of charge carriers (electrons or holes) that accompany thermal motions of solid lattice of atoms.

Lead to thermal current fluctuations that create voltage fluctuations in the presence of a resistive element Resistor, capacitor, etc.

4rms kTR f

nrms = root-mean-square noise voltagek = Boltzman’s constantT = temperature

R = resistance of element (W)Df = bandwith (Hz) = 1/(3tr)tr = rise time

Page 8: Analytical figures of merit, noise, and S/N ratio Chemistry 243.

Thermal (Johnson) noise continued

Dependent upon bandwidth (Df) but not f itself white noise

Can be reduced by narrowing bandwidth Slows instrument response time More time required for measurement

Reduced by lowering T Common to cool detectors

298K77K lowers thermal noise by factor of ~2

4rms kTR f

nrms = root-mean-square noise voltagek = Boltzman’s constantT = temperature

R = resistance of element (W)Df = bandwith (Hz) = 1/(3tr)tr = rise time

N2(l): bp=77K

Page 9: Analytical figures of merit, noise, and S/N ratio Chemistry 243.

Shot noise

Arises from statistical fluctuations in quantized behaviors Electrons crossing junctions or surfaces

Independent of frequency Example: current

10.5 e-/s

10 e-/s

11 e-/s

2rmsi Ie f irms = root-mean-square noise currentI = average direct currente = electron chargeDf = bandwidth (Hz)

Page 10: Analytical figures of merit, noise, and S/N ratio Chemistry 243.

Flicker (1/f) noise

Magnitude is inversely proportional to the frequency of the signal

Significant at frequencies lower than 100 Hz Long-term drift

Origin is not well understood Dependent upon materials and device shape

Metallic resistors have 10-fold less flicker noise than carbon-based resistors.

Referred to as “pink” noise—more red (low frequency) components

Page 11: Analytical figures of merit, noise, and S/N ratio Chemistry 243.

Environmental noise

Comes from the surroundings Biggest source is “antenna” effect of

instrument cabling

J. Chem. Educ., 1968, 45, A533-542.

Page 12: Analytical figures of merit, noise, and S/N ratio Chemistry 243.

Noise contributions in different frequency regimes

Frequency independent

Supposedly 1/f—mostly at low frequencies

Occurs at discrete frequencies

Page 13: Analytical figures of merit, noise, and S/N ratio Chemistry 243.

Enhancing signal-to-noise

Hardware methods Grounding and shielding Difference and Instrumentation Amplifiers Analog Filtering Lock-In Amplifiers

Modulation and Synchronous Demodulation

Software methods Ensemble averaging Boxcar averaging Digital filtering Correlation methods

Page 14: Analytical figures of merit, noise, and S/N ratio Chemistry 243.

Grounding and shielding

Surround circuits (most critical conductors) with conducting material that is connected to ground Noise will be picked up by shield and not by

circuit Faraday cage

http://www.autom8.com/images_product/table_farady_benchtop.jpghttp://farm2.static.flickr.com/1227/578199978_17e8133c7c_o.jpg

Page 15: Analytical figures of merit, noise, and S/N ratio Chemistry 243.

Analog filtering

Low pass filter removes high frequency noise Thermal and shot noise

High pass filter removes low frequency noise Drift and flicker noise

Narrow-band electronic filters

Example of low-pass filter

High freq removed.Low freq preserved

(passed).

Page 16: Analytical figures of merit, noise, and S/N ratio Chemistry 243.

Lock-in amplifiers

Modulation Translate low frequency signal

(prone to 1/f noise) to a high frequency signal which can amplified and then filtered to remove 1/f noise

Mechanical chopper

Page 17: Analytical figures of merit, noise, and S/N ratio Chemistry 243.

Lock-in amplifierscontinued

Synchronous demodulation Converts AC signal to DC signal synchronous with chopper

—follows reference Low-pass filtering

Back converts high frequency DC signal to return filtered, low frequency output.

Page 18: Analytical figures of merit, noise, and S/N ratio Chemistry 243.

Ensemble averaging to increase S/N

Averaging multiple data sets taken in succession Divide sum of data

sets by number of data sets

1

n

ii

x

S

Sn

J. Chem. Educ., 1979, 56, 148-153.

Page 19: Analytical figures of merit, noise, and S/N ratio Chemistry 243.

Ensemble averagingcontinued

Signal-to-noise improves with increasing number of data sets

n i

S SnN N

N = rms noise n = number of replicate scansi = number of replicate scans in other data set

# Scans, n Relative S/N

1 1 4 216 464 8

Page 20: Analytical figures of merit, noise, and S/N ratio Chemistry 243.

Boxcar averaging

Smoothing irregularities and increasing S/N Assumes signal varies slowly in time Multiple points are averaged to give a single

value Often performed in real time Detail is lost and utility limited for rapidly

changing samples Boxcar integrators commonly used in fast

(pico- to microsecond) measurements using pulsed lasers.

Page 21: Analytical figures of merit, noise, and S/N ratio Chemistry 243.

Moving average smooth

Similar to a boxcar average, but changes in time

0 200 400 600 800 1000

data point

sig

nal

(arb

un

its)

Average Standard Deviation

S/N Relative S/N

Original 100.2 6.0 16.6 1

4 point 100.2 3.0 33.4 2.0

16 point 100.2 1.5 67.1 4.0

100 point

100.2 0.6 160 9.7

Page 22: Analytical figures of merit, noise, and S/N ratio Chemistry 243.

Downside of moving average smoothing

50

60

70

80

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100

110

120

130

140

0 200 400 600 800 1000

sig

nal

(arb

un

its

)

data point

Page 23: Analytical figures of merit, noise, and S/N ratio Chemistry 243.

Digital filtering

Fourier transform Convert data from time- to frequency-domain,

manipulate to remove higher frequency noise components, regenerate time-domain signal

Polynomial data smoothing Moving average smooth Least-squares polynomial smoothing