AOSC 634 Air Sampling and Analysis Lecture 1 Measurement Theory Performance Characteristics of instruments Nomenclature and static response Copyright Brock et al. 1984; Dickerson 2015 1 Static Response Output Sensor output in response to unchanging input. .. .. .. : } .. : :: . .. ..... : .. . .. . .. : .. .. : .. : . .. bias or zero offset Input 2 Static Response I = input, atmospheric, oceanic, or other environmental signal. O = Output, sensor response voltage, current, counts, etc. Nomenclature varies but concepts are fundamental. Sensitivity – slope of I/O diagram. Bias (zero offset) – Y intercept. Mass flow controllers are a good example. Range – max to min measureable. Span – max minus min. Linearity – how well the calibration curve fits a straight line. Resolution – the smallest change in the input that can produce a change in the output. 3 Primary vs. secondary variables Example - a pressure transducer sensitive to temperature . 4 UV absorption instruments • The [O3] indicated is actually a molecular number density. The mixing ratio (ppb) has to be corrected for air temperature and pressure. [O3 ]indicated æ 298 ö æ P(hPa) ö = [O3 ]real × ç ÷ ÷×ç è T(K) ø è 1013 ø • The ozone instrument has sensitivity to a secondary input – air density. 5 6 Indicated wind speed Example of threshold a cup anemometer with static friction. Input - Actual wind speed 7 Additional Nomenclature I don't like the traditional definitions of "precision" and "accuracy" given in Brock’s book, but they are in common use among meteorologists. Here are alternative definitions in common use by analytical chemists and meteorologists. Precision - The standard deviation of a series of measurements made under constant conditions. 8 Accuracy - This is a slippery concept that can only be determined if the "true" value of the variable of interest is known. For example, the "accuracy" of a thermometer can be determined at 0°C with an ice water bath. If we measure air temperature with the same thermometer we might be able to determine the "accuracy" of the measurement with a second, much better thermometer, but what about state-of-the-art instruments measuring unknown quantities? For the most interesting questions in atmospheric science, "accuracy" must be estimated. 9 Uncertainty - The combined effect of all the sources of noise or other error in a measurement. Usually expressed as some range of values at some confidence level; for example 25.03 ± 0.04°C. If the sources of error or uncertainty are "normal" or Gaussian, (and often they are not) these ranges might represent confidence of 68% (+/- σ), 95% (+/- 2 σ), or 99% (+/- 2.5 σ). y= 1 2ps e - [(x - x) / s ] / 2 2 10 Detection limit- Also called lowest detectable level, this is the concentration or amount below which an instrument cannot provide meaningful information. Because several definitions are common use, a good paper will define the detection limit used. Consider an atomic emission spectrometer that produces a net output of 2 V for an aqueous solution of 2.0 μM Na+, and a background signal with Gaussian noise with a standard deviation of 0.25 V when the signal integration time is 1 s. The signal-to-noise ratio is 2:1 for [Na+] of 2.0 μM for ±2σ. For a rainwater or aerosol sample then, the detection limit for sodium is 1.0 μM at a signal-to-noise ratio of 1:1 with a 95% confidence interval for a 1 s integration time. Again the detection limit might be better for longer sampling times, but the experimenter must prove this. 11 Summary • There are may “figures of merit” for an instrument or measurement. • The best ones depend on the application at hand. • For example do you want an instrument that is fast and sensitive for flux measurements of aircraft observations or one that is stable and insensitive to temperature and pressure for monitoring? 12