1 st Joint GOSUD/SAMOS Workshop The Florida State University 1 Sensitivity of Surface Turbulent Fluxes to Observational Errors  or.

Slides:



Advertisements
Similar presentations
Modeling of Data. Basic Bayes theorem Bayes theorem relates the conditional probabilities of two events A, and B: A might be a hypothesis and B might.
Advertisements

Running a model's adjoint to obtain derivatives, while more efficient and accurate than other methods, such as the finite difference method, is a computationally.
Mean, Proportion, CLT Bootstrap
A thermodynamic model for estimating sea and lake ice thickness with optical satellite data Student presentation for GGS656 Sanmei Li April 17, 2012.
PRESENTS: FORECASTING FOR OPERATIONS AND DESIGN February 16 th 2011 – Aberdeen.
Hurricanes and Atlantic Surface Flux Variability Mark A. Bourassa 1,2, Paul J. Hughes 1,2, Jeremy Rolph 1, and.
Global Warming and Climate Sensitivity Professor Dennis L. Hartmann Department of Atmospheric Sciences University of Washington Seattle, Washington.
EXPERIMENTAL ERRORS AND DATA ANALYSIS
Lecture 7 Water Vapor.
Chapter 9 Vertical Motion. (1) Divergence in two and three dimensions. The del “or gradient” operator is a mathematical operation performed on something.
Basic Measurement Concepts ISAT 253 Spring Dr. Ken Lewis Mod. 2 Measurement Concepts So far… In the Design of Experiments In the Design of Experiments.
Using Scatterometers and Radiometers to Estimate Ocean Wind Speeds and Latent Heat Flux Presented by: Brad Matichak April 30, 2008 Based on an article.
Using observations to reduce uncertainties in climate model predictions Maryland Climate Change Workshop Prof. Daniel Kirk-Davidoff.
MET 61 1 MET 61 Introduction to Meteorology MET 61 Introduction to Meteorology - Lecture 4 “Heat in the atmosphere” Dr. Eugene Cordero San Jose State University.
Experimental Evaluation
Statistical Treatment of Data Significant Figures : number of digits know with certainty + the first in doubt. Rounding off: use the same number of significant.
MET 61 1 MET 61 Introduction to Meteorology MET 61 Introduction to Meteorology - Lecture 3 Thermodynamics I Dr. Eugene Cordero San Jose State University.
Introduction to Numerical Weather Prediction and Ensemble Weather Forecasting Tom Hamill NOAA-CIRES Climate Diagnostics Center Boulder, Colorado USA.
1 Seventh Lecture Error Analysis Instrumentation and Product Testing.
Evaporative heat flux (Q e ) 51% of the heat input into the ocean is used for evaporation. Evaporation starts when the air over the ocean is unsaturated.
Wind Driven Circulation I: Planetary boundary Layer near the sea surface.
OCO Review 2006 Tropical Cyclone Activity  and  North Atlantic Decadal Variability of Ocean Surface Fluxes Mark.
Instrumentation and Measurements
V. Rouillard  Introduction to measurement and statistical analysis ASSESSING EXPERIMENTAL DATA : ERRORS Remember: no measurement is perfect – errors.
Psy B07 Chapter 1Slide 1 ANALYSIS OF VARIANCE. Psy B07 Chapter 1Slide 2 t-test refresher  In chapter 7 we talked about analyses that could be conducted.
AM Recitation 2/10/11.
Monin-Obukhoff Similarity Theory
Ch 8.1 Numerical Methods: The Euler or Tangent Line Method
Determining Sample Size
Calculating the amount of atmospheric carbon dioxide absorbed by the oceans Helen Kettle & Chris Merchant School of GeoSciences, University of Edinburgh,
Evaporative heat flux (Q e ) 51% of the heat input into the ocean is used for evaporation. Evaporation starts when the air over the ocean is unsaturated.
Metrology Adapted from Introduction to Metrology from the Madison Area Technical College, Biotechnology Project (Lisa Seidman)
Applications for Fine Resolution Marine Observations Mark A. Bourassa.
Atmospheric Moisture Vapor pressure (e, Pa) The partial pressure exerted by the molecules of vapor in the air. Saturation vapor pressure (e s, Pa ) The.
LECTURER PROF.Dr. DEMIR BAYKA AUTOMOTIVE ENGINEERING LABORATORY I.
Comparison of Surface Turbulent Flux Products Paul J. Hughes, Mark A. Bourassa, and Shawn R. Smith Center for Ocean-Atmospheric Prediction Studies & Department.
Chapter 13 Weather Forecasting and Analysis. Weather forecasting by the U.S. government began in the 1870s when Congress established a National Weather.
Dataset Development within the Surface Processes Group David I. Berry and Elizabeth C. Kent.
High-Resolution Climate Data from Research and Volunteer Observing Ships: A Strategic Intercalibration and Quality Assurance Program A Joint ETL/WHOI Initiative.
Automated Weather Observations from Ships and Buoys: A Future Resource for Climatologists Shawn R. Smith Center for Ocean-Atmospheric Prediction Studies.
MGS3100_04.ppt/Sep 29, 2015/Page 1 Georgia State University - Confidential MGS 3100 Business Analysis Regression Sep 29 and 30, 2015.
Instrumentation and Measurements Class 3 Instrument Performance Characteristics.
Fluxes With input from: USCLIVAR Working Group on High-Latitude Fluxes: Ed Andreas, Cecelia Bitz, Dave Carlson, Ivana Cerovecki, Meghan Cronin‏, Will Drennan,
Ping Zhu, AHC5 234, Office Hours: M/W/F 10AM - 12 PM, or by appointment M/W/F,
Modern Era Retrospective-analysis for Research and Applications: Introduction to NASA’s Modern Era Retrospective-analysis for Research and Applications:
Cooling and Enhanced Sea Ice Production in the Ross Sea Josefino C. Comiso, NASA/GSFC, Code The Antarctic sea cover has been increasing at 2.0% per.
Ice Cover in New York City Drinking Water Reservoirs: Modeling Simulations and Observations NIHAR R. SAMAL, Institute for Sustainable Cities, City University.
Graduate Course: Advanced Remote Sensing Data Analysis and Application A COMPARISON OF LATENT HEAT FLUXES OVER GLOBAL OCEANS FOR FOUR FLUX PRODUCTS Shu-Hsien.
Ocean Surface heat fluxes Lisan Yu and Robert Weller
Characterization of Errors in Turbulent Heat Fluxes Caused by Different Heat and Moisture Roughness Length Parameterizations 1. Background and Motivation.
Ocean Surface heat fluxes
An evaluation of a hybrid satellite and NWP- based turbulent fluxes with TAO buoys ChuanLi Jiang, Kathryn A. Kelly, and LuAnne Thompson University of Washington.
Evaluation of Satellite-Derived Air-Sea Flux Products Using Dropsonde Data Gary A. Wick 1 and Darren L. Jackson 2 1 NOAA ESRL, Physical Sciences Division.
Chapter 7: The Distribution of Sample Means
Moisture  There are several methods of expressing the moisture content (water in vapor form) of a volume of air.  Vapor Pressure: The partial pressure.
Meteorological Variables 1. Local right-hand Cartesian coordinate 2. Polar coordinate x y U V W O O East North Up Dynamic variable: Wind.
Wind Driven Circulation I: Ekman Layer. Scaling of the horizontal components  (accuracy, 1% ~ 1‰) Rossby Number Vertical Ekman Number R o and E v are.
SUR-2250 Error Theory.
A.Liudchik, V.Pakatashkin, S.Umreika, S.Barodka
Enhancement of Wind Stress and Hurricane Waves Simulation
A Fear-Inspiring Intercomparison of Monthly Averaged Surface Forcing
Lecture 8 Evapotranspiration (1)
A Simple, Fast Tropical Cyclone Intensity Algorithm for Risk Models
MET3220C & MET6480 Computational Statistics
Question 1 Given that the globe is warming, why does the DJF outlook favor below-average temperatures in the southeastern U. S.? Climate variability on.
High-Resolution Climate Data from Research and Volunteer Observing Ships: A Strategic Intercalibration and Quality Assurance Program A Joint ETL/WHOI Initiative.
Mark A. Bourassa and Qi Shi
Impacts of High Resolution SST Fields on Objective Analysis of Wind Fields Mark A. Bourassa Center for Ocean-Atmospheric Prediction Studies & Department.
Comparison of Aircraft Observations With Surface Observations from
MGS 3100 Business Analysis Regression Feb 18, 2016
Presentation transcript:

1 st Joint GOSUD/SAMOS Workshop The Florida State University 1 Sensitivity of Surface Turbulent Fluxes to Observational Errors  or  Where We Could Go Seriously Wrong Mark A. Bourassa and Paul J. Hughes Center for Ocean-Atmospheric Prediction Studies & Department of Meteorology, The Florida State University

1 st Joint GOSUD/SAMOS Workshop The Florida State University 2 The Relevant Types of Errors Depend on the Application  Estimating a climatological heat flux  Biases and sampling error (sampling vs. natural variability) are important  Satellite calibration  In many cases there are insufficient co-located observations to ignore random error.  Biases and random error are important  Input for numerical weather prediction (NWP)  Biases and random error are important  Approximately 95% of marine surface observations are rejected in NOAA’s data assimilation. NWP is not an ideal application.  Climate comparisons  If done correctly, dependent largely on errors in the mean (biases).  Random error is small if there are enough observations.

1 st Joint GOSUD/SAMOS Workshop The Florida State University 3 Suggested Measurement Accuracy From the Handbook  I will assume that a 5Wm -2 is the limit for biases in radiative fluxes.  Then 5Wm -2 is the limit for biases in surface turbulent heat fluxes.

1 st Joint GOSUD/SAMOS Workshop The Florida State University 4 Historical and Modern Goals  During TOGA-COARE it was determined that a goal in surface turbulent flux observations was a bias of no more than 5Wm -2.  This same goal is currently being stated in comments on decadal satellite survey.  There have been several estimates on the observational accuracies required to achieve this goal.  HOWEVER these accuracies were determined for the environments being observed during TOGA-COARE (the tropical Pacific Ocean).  The conditions in the tropical Pacific Ocean are somewhat different from other parts of the globe.  How much do the necessary observational accuracies change for different environments?  Are they applicable to each application?  I will describe how to determine these requirements, and discuss how to trade off strengths and weaknesses to minimize errors in fluxes.  Good things to know when designing an observation system!

1 st Joint GOSUD/SAMOS Workshop The Florida State University 5 Observational Errors  We are primarily interested in how biases in observations of wind speed (w), sea surface temperature (SST), near surface air temperature (T air ), and near surface humidity (q air ) translate to biases in calculated fluxes.  Sensible heat (H), latent heat (E), and stress (  ).  In general, the bias in one of these observations can be related to the bias in a flux through a Sensitivity (S).  Errors can be described as composed of  A bias (this bias could be a function of environmental conditions),  And a random uncertainty.  The same tables can be used to determine the influence of the bias and the uncertainty.

1 st Joint GOSUD/SAMOS Workshop The Florida State University 6 Biases  To first order, the the biases can be calculated for each input variable, and then summed.  The maximum allowable bias in an observation (e.g., |  w|) can be estimated from the maximum specified error in the calculated variable (e.g., |  E| max ), and the sensitivity (e.g., S E,w )  |  w| max = |  E| max / |S E,w |  The bias in a calculated variable (a flux) is equal to the sum of ‘sensitivity (S) times the bias in a input observation).  Example: How much does a bias in speed (  w) contribute to a bias in the latent heat flux (  E)?   E = S E,w  w  If S E,w is very large, then even a small bias in w can result in a large bias in E.  If the sensitivity is very small, then the calculated variable is insensitive to errors in the observation.

1 st Joint GOSUD/SAMOS Workshop The Florida State University 7 How is the Sensitivity Determined?  The sensitivity is the partial derivative of the output quantity (e.g., the flux) with respect to the input observation (e.g., wind speed).  S E,w =  E/  w  The sensitivity can be determined by solving the bulk formula, and using finite differences to determine the partial derivative of the drag coefficients.

1 st Joint GOSUD/SAMOS Workshop The Florida State University 8 Example: Sensitivity of Sensible Heat Flux to Errors in Temperature (  H/  T)

1 st Joint GOSUD/SAMOS Workshop The Florida State University 9 Example: Sensitivity of Sensible Heat Flux to Errors in 10m Wind Speed (  H/  w)

1 st Joint GOSUD/SAMOS Workshop The Florida State University 10 Example: Sensitivity of Latent Heat Flux to Errors in Wind Speed:  (E/  q)/  w  Air/sea humidity differences are also important.  A third dimension is awkward to work with. Therefore Sensitivity, per kg/kg is given.  Humidity differences are typically on the order of 1g/kg.

1 st Joint GOSUD/SAMOS Workshop The Florida State University 11 Random Errors  If the random errors have a Gaussian distribution, which might be expected from the central limit theorem, then random errors are described by a standard deviation ( , which is used a measure of spread).  If the latent heat flux (E) is written as a function of the input variables:  E = f(x 1, x 2, x 3, x 4 ),  Then the uncertainty in E (   ) for a single observation can be written as  An uncertainty in the mean is equal to  E divided by the squareroot of the number of independent observations.

1 st Joint GOSUD/SAMOS Workshop The Florida State University 12 Error Limits for Observation Errors  For this talk, we will ignore random errors, assuming that they will be small given enough samples.  This is a common assumption, but will not be true for all applications!  The maximum allowable bias in an observation (e.g., |  w|) can be estimated from the maximum specified error in the calculated variable (e.g., |  E|), and the sensitivity (e.g., S E,w )  |  w| max = |  E| max / |S E,w |

1 st Joint GOSUD/SAMOS Workshop The Florida State University 13 Example: How Much Bias in Wind Speed Can We Tolerate in Calculated SHF  We must be relatively accurate.  We can be relatively sloppy. Assume a bias in SHF of <1.25 Wm -2 is OK. Climate Accuracy 0.2 m/s

1 st Joint GOSUD/SAMOS Workshop The Florida State University 14 Example: How Much Bias in SST Can We Tolerate in Calculated SHF Assume a bias in SHF of <1.25 Wm -2 is OK.  We can be extremely sloppy. Can Gary Wick give us good satellite SST fields in a warm core seclusion? Climate accuracy 0.1  C

1 st Joint GOSUD/SAMOS Workshop The Florida State University 15 Example: How Much Bias in Wind Speed Can We Tolerate in Calculated LHF  Fortunately, high winds are usually associated with unstable stratification (SST –T air > 0).  In strong storms, we will not meet our accuracy requirement. 0.2 m/s (climate) 0.4 m/s (satellite)

1 st Joint GOSUD/SAMOS Workshop The Florida State University 16 How Much Bias in Air Temperature Can We Tolerate in Calculated LHF  Not a problem!

1 st Joint GOSUD/SAMOS Workshop The Florida State University 17 Saturation Vapor Pressure  ‘Surface’ humidity is considered to be 98% or 100% of the saturation value, which is a strong function of temperature.  The Clausius-Clapeyron equation describes how the saturation vapor pressure changes with temperature.  where e o = kPa, T o = 273K, and R v = 461 JK -1 kg -1 is the gas constant for water vapor.  L is either the latent heat of vaporization (L v = 2.5x10 6 Jkg -1 ), or the latent heat of deposition (L d = 2.83x10 6 Jkg -1 ), depending on whether or not we are describing equilibrium with a flat surface of water or ice. Figure from Meteorology by Danielson, Levin and Abrams

1 st Joint GOSUD/SAMOS Workshop The Florida State University 18 How Much Bias in SST Can We Tolerate in Calculated LHF?  For low temperature regions, we might what tighter accuracies than have been specified.  In areas with large  q, there could be issues for very high winds and unstable stratification.  Particularly so for point comparisons  Recall that these numbers should be divided by  q (in g/kg).

1 st Joint GOSUD/SAMOS Workshop The Florida State University 19 Maximize Benefits of Improvements in Observations  How do we decide which instruments to improve?  A ratio of sensitivities provides some indication of where improvements to accuracy will have the greatest influence. That is, which type of observation is the best to improve.  Technically this should be weighted by the cost and time involved in the improvement.  However, if you can estimate that it will take $x to make a certain amount of improvement, you can determine where the money is best spent.

1 st Joint GOSUD/SAMOS Workshop The Florida State University 20 When Will Improved Accuracy in Air Temperature and Speed Help The Most?  Examine the relative sensitivity of SHF to errors in T air and wind speed:  H/  w /  H  T air  A ratio of 1 indicates an improvement of x m/s will equal the improvement of x  C Improving T air has a greater impact Improving w has a greater impact

1 st Joint GOSUD/SAMOS Workshop The Florida State University 21 Take Home Messages  The type(s) of error (bias, random, sampling) that are relevant depend on the application.  Errors (or uncertainties) in observed variables can be used to determine the biases (and uncertainties) in calculated variables.  The same sensitivity tables can used to determine both random errors and biases.  The current suggestions for accuracies are for the most part good enough for many applications; however, there are conditions for which they are insufficient.  Ratios of these sensitivities provides some insight into which instruments to improve to improve fluxes.  Suggested changes to accuracies:  Tighter requirements for mean wind speed?  Tighter mean SST accuracy would be nice, but can we do it?  Tighter requirements preferred for satellite calibration.

1 st Joint GOSUD/SAMOS Workshop The Florida State University 22 Suggested Measurement Accuracy From the Handbook Wave data