Best estimation of a local mass to diameter function using imaging probe and hot-wire TWC measurement Case of the AIRBUS imager during the Cayenne flight.

Slides:



Advertisements
Similar presentations
“PAT” Applications for Biochemical Processes
Advertisements

POLARIMETRIC RADAR IMPROVEMENTS
A comparison between observed and simulated hydrometeor size distributions in MCS using the AMMA 2006 microphysical data set V. Giraud, C. Duroure and.
Non-life insurance mathematics
Hypothesis Testing Steps in Hypothesis Testing:
Wet Granulation Scale-up Experiments. Scale-up Approach with Dimensional Numbers 2 The effect of process parameter (i.e., impeller speed, liquid addition.
3.11 Adaptive Data Assimilation to Include Spatially Variable Observation Error Statistics Rod Frehlich University of Colorado, Boulder and RAL/NCAR Funded.
Formation et Analyse d’Images Session 8
Forschungszentrum Karlsruhe in der Helmholtz-Gemeinschaft NDACC H2O workshop, Bern, July 2006 Water vapour profiles by ground-based FTIR Spectroscopy:
Copyright © 2008 by the McGraw-Hill Companies, Inc. All rights reserved. McGraw-Hill/Irwin Managerial Economics, 9e Managerial Economics Thomas Maurice.
Robin Hogan Anthony Illingworth Marion Mittermaier Ice water content from radar reflectivity factor and temperature.
Logistic Regression Rong Jin. Logistic Regression Model  In Gaussian generative model:  Generalize the ratio to a linear model Parameters: w and c.
Original image: 512 pixels by 512 pixels. Probe is the size of 1 pixel. Picture is sampled at every pixel ( samples taken)
Computational grid size ~0.5 m Process ~5 mm REV Maco-Micro Modeling— Simple methods for incorporating small scale effects into large scale solidification.
Observational approaches to understanding cloud microphysics.
D. Waddicor, G. Vaughan, K. Bower, T. Choularton, H. Coe, M. Flynn, M. Gallagher, P. Williams Aerosol observations and growth rates in the TTL.
Quantitative Business Analysis for Decision Making Simple Linear Regression.
1 1 Slide Simple Linear Regression Chapter 14 BA 303 – Spring 2011.
STK 4540Lecture 6 Claim size. The ultimate goal for calculating the pure premium is pricing 2 Pure premium = Claim frequency x claim severity Parametric.
Aircraft spiral on July 20, 2011 at 14 UTC Validation of GOES-R ABI Surface PM2.5 Concentrations using AIRNOW and Aircraft Data Shobha Kondragunta (NOAA),
Measurements of microphysical properties of convective clouds in the tropics and the mid-latitudes.
Foliage and Branch Biomass Prediction an allometric approach.
The Importance of Atmospheric Variability for Data Requirements, Data Assimilation, Forecast Errors, OSSEs and Verification Rod Frehlich and Robert Sharman.
General Linear Model & Classical Inference London, SPM-M/EEG course May 2014 C. Phillips, Cyclotron Research Centre, ULg, Belgium
GADA - A Simple Method for Derivation of Dynamic Equation Chris J. Cieszewski and Ian Moss.
M. Alnafea1*, K. Wells1, N.M. Spyrou1 & M. Guy2
Regression. Population Covariance and Correlation.
A Simple Model of the Mm-wave Scattering Parameters of Randomly Oriented Aggregates of Finite Cylindrical Ice Hydrometeors : An End-Run Around the Snow.
Ice Crystals Clues from the clouds Rachel Schwartz April 17, 2009.
Size Distributions Many processes and properties depend on particle size –Fall velocity –Brownian diffusion rate –CCN activity –Light scattering and absorption.
Classical Inference on SPMs Justin Chumbley SPM Course Oct 23, 2008.
Spectral unmixing of vegetation, soil and dry carbon cover in arid regions: comparing multispectral and hyperspectral observations G.P.Asner and K.B.Heidebrecht.
Chapter 15 – CTRW Continuous Time Random Walks. Random Walks So far we have been looking at random walks with the following Langevin equation  is a.
A Comparative Analysis of Satellite-based Approaches for Aboveground Biomass Estimation in the Brazilian Amazon Dengsheng Lu: Indiana University.
IE 300, Fall 2012 Richard Sowers IESE. 8/30/2012 Goals: Rules of Probability Counting Equally likely Some examples.
Scatter Diagrams scatter plot scatter diagram A scatter plot is a graph that may be used to represent the relationship between two variables. Also referred.
A comparison of airborne in-situ cloud microphysical measurements with ground C and X band radar observations in African squall lines E. Drigeard 1, E.
OVERVIEW OF THE DATA OBTAINED DURING ASTAR 2007 (ARCTIC MIXED-PHASE CLOUDS) & CIRCLE-2 (MID-LATITUDE CIRRUS) Alfons Schwarzenboeck, Guillaume Mioche, Christophe.
Daniel Grosvenor, Thomas Choularton, Martin Gallagher (University of Manchester, UK); Thomas Lachlan Cope and John King (British Antarctic Survey). Daniel.
Linear Correlation (12.5) In the regression analysis that we have considered so far, we assume that x is a controlled independent variable and Y is an.
A comparison of cloud microphysics in deep tropical convection forming over the continent and over the ocean Emmanuel Fontaine 1, Elise Drigeard 1, Wolfram.
Lecture 17: Diffusion PHYS 430/603 material Laszlo Takacs UMBC Department of Physics.
An Optical Search for Small Comets R. L. Mutel & J.D. Fix University of Iowa An Optical Search for Small Comets R. L. Mutel & J.D. Fix University of Iowa.
EASA HighIWC EASA-HighIWC Final Meeting WP1/Task1.2: Analysis of the microphysical properties of the HighIWC regions using existing airborne in-situ observations.
- 1 - Satellite Remote Sensing of Small Ice Crystal Concentrations in Cirrus Clouds David L. Mitchell Desert Research Institute, Reno, Nevada Robert P.
Testbeam analysis Lesya Shchutska. 2 beam telescope ECAL trigger  Prototype: short bars (3×7.35×114 mm 3 ), W absorber, 21 layer, 18 X 0  Readout: Signal.
Geometrical description of the hydrometeor images sampled with the AIRBUS imager during the Cayenne flight 1423 Minimal model for the small ice particles.
Data Intercomparison – FAAM Flight Phil Rosenberg, Angela Dean.
Selecting Input Probability Distributions. 2 Introduction Part of modeling—what input probability distributions to use as input to simulation for: –Interarrival.
General Linear Model & Classical Inference London, SPM-M/EEG course May 2016 Sven Bestmann, Sobell Department, Institute of Neurology, UCL
Transportation Planning Asian Institute of Technology
23 Jan 2012 Background shape estimates using sidebands Paul Dauncey G. Davies, D. Futyan, J. Hays, M. Jarvis, M. Kenzie, C. Seez, J. Virdee, N. Wardle.
General Linear Model & Classical Inference Short course on SPM for MEG/EEG Wellcome Trust Centre for Neuroimaging University College London May 2010 C.
Date of download: 9/19/2016 Copyright © 2016 SPIE. All rights reserved. (a) Overview of a quantitative backscattered electron imaging (qBEI) image with.
B3. Microphysical Processes
Probing clouds: why its necessary to use multiple instruments.
MIT Microstructural Evolution in Materials 13: Precipitate Growth
Lunar observation data set preparation
A tale of many cities: universal patterns in human urban mobility
Microscope Measurement
Fundamentals of estimation and detection in signals and images
General Linear Model & Classical Inference
OBR: Cloud Physics Research
Optical flow , A tutorial of the paper:
Basic Estimation Techniques
Citation Data Comparison
Regression Assumptions
Dual-Aircraft Investigation of the Inner Core of Hurricane Nobert
Regression Assumptions
History of 50 years ozone soundings:
Presentation transcript:

Best estimation of a local mass to diameter function using imaging probe and hot-wire TWC measurement Case of the AIRBUS imager during the Cayenne flight 1423 C. Duroure, A. Delplanque (LaMP), M. Weber (AIRBUS) 1- We present a simple method to find the best mass to diameter function for a given sample set of hydrometeor images using as reference a alternate TWC measurement (in this case the hot wire Robust probe) 2- We compare the TWC estimation using this method with other methods (method using only the total count, methods using classical power law fit, method using estimation with more geometrical parameters (Lawson & Baker, JAMC,2006) 3- Examples of sampled images (capped columns) => simple geometrical model 4- Work in progress: Technical trouble: 1-Small particles PSD (D<100µm). Trouble in the ROI code ? 2-Sensibility of the results to the threshold rules (example of PSD with decreasing threshold) HAIC working document 18/11/2013 meeting

TWC hot wire (Robust) Best A.M estimate B Lawson & B. estimate Ctot estimate Three exemples of TWC estimations from imager using different rules, compared to hot wire probe

12 3 Scatter plot (TWC from imager, TWC from hot wire probe) 1- Best estimation using power law functions (see next slides) 2- Lawson and Baker geometrical estimation f(A,W,L,P) (non linearity, due to Lmax estimation ?) 3- Simplest estimation (using total count of hydrometeor images) Comparisons between imager and hot wire probe

Sigma using only total concentration Best estimation using PSD and M(D) power law Beta=1.93 B=1.93B=1.50B= Look for the best linear correlation of TWC from imager and hot wire (not sensible to theA prefactor, i.e. calibration factors, DOF,….) => Estimation of B Estimation of the mass(diameter) function mass=A*Diam^B

Step 2- Look for the best PDF correlation between the two probes  Empirical estimation of the prefactor M= 3.28e-5 Dsur Step 3- Verify the estimated mass to diameter law (Mass=A.D B) assuming: shape model and hydrometeor density - Imager … Hot wire 1.93

Capped columns Leg [12 h,12.7 h] Best estimate of B=1.93 Irregular+agregates Leg [12.7 h,12.8 h] Best estimate of B=1.98 (more dense objects ?)

Some examples of « well oriented » images of capped columns (more than 300 avaiable (D> 300µm) for the 10.6 Km leg [12h,12.7h ] Manual estimation of 4 geometrical variables: (Lc,Wc) columns part, (Lp,Wp) plates part 1 mm Lc Wc Lp Wp Assumed growth historie of these CP: 1- Start as column for higth sursatuation S 2- Transition to plate for low S Large variability observed for this transition => Dificult to define a « standard » shape

Some examples of « irregular» images (+aggregates+rosettes) for the 10.6 Km altitude sub-leg [12.7 h,12.8h ] (« old » region, low concentration) 1 mm Assumed growth historie of these cristal ? 1- Nucleation of supercooled droplet 2- Vapour diffusion process (low S ?) 2- Agregation On the site: CATROI_V1423all Catalogue of all ROI images of size larger than 300µm (for identification of regions)

Tresholding sensibility analysis Treshold definition: Amp=(max(image)-min(image))/2 Med= min(image)+Amp Tresh=med-S*Amp Binary image= image LE Tresh S=0 S=0.1 S=0.2 S=0.25 GEO ROI files on the site V1423_GEO_S000 S=0 V1423_GEO_S010 S= V1423_GEO_S030 S=0.3

S=0 S=0.1 S=0.2 S= pix S=0 S=0.1 S=0.2 S=0.25 Tresholding sensibility analysis Small diameter effect Large diameter effect Diameter measure shift (few pixel) Artefact for tail of large particles

Technical trouble: 1-Small particles PSD (D<100µm). Trouble in the ROI code ? 2-AIRBUS PSD jump ? Diameter (µm) AIRBUS PSD __ ROI PSD ?