DOAS measurements of Atmospheric Species

Similar documents
Jasco V-670 absorption spectrometer

How to Make Photometric & Colorimetric Measurements of Light Sources using an Ocean Optics Spectrometer and SpectraSuite Software

Lab 5: Calculating an equilibrium constant

Measuring ph with Smart Cuvettes

Connect the Vernier spectrometer to your lap top computer and power the spectrometer if necessary. Start LoggerPro on your computer.

Operating the Celestron 14 Telescope

FIELD SPECTROMETER QUICK-START GUIDE FOR FIELD DATA COLLECTION (LAST UPDATED 23MAR2011)

Remember that C is a constant and ë and n are variables. This equation now fits the template of a straight line:

2. To measure the emission lines in the hydrogen, helium and possibly other elemental spectra, and compare these to know values.

CLEA/VIREO PHOTOMETRY OF THE PLEIADES

Astro 3 Lab Exercise

Instytut Fizyki Doświadczalnej Wydział Matematyki, Fizyki i Informatyki UNIWERSYTET GDAŃSKI

Ocean Optics Red Tide UV-VIS Spectrometer (Order Code: SPRT-UV-VIS)

Department of Physics and Astronomy University of Iowa 29:137 Astronomical Laboratory Fall 2011 Lab 4: Stellar Spectroscopy

Life Cycle of Stars. Photometry of star clusters with SalsaJ. Authors: Daniel Duggan & Sarah Roberts

You w i ll f ol l ow these st eps : Before opening files, the S c e n e panel is active.

Kinetics of Crystal Violet Bleaching

Diffuser plate spectral structures and their influence on GOME slant columns

Senior astrophysics Lab 2: Evolution of a 1 M star

Conservation of Mechanical Energy Activity Purpose

Background The power radiated by a black body of temperature T, is given by the Stefan-Boltzmann Law

Software BioScout-Calibrator June 2013

Variable Stars Advanced Lab

Menzel/Matarrese/Puca/Cimini/De Pasquale/Antonelli Lab 2 Ocean Properties inferred from MODIS data June 2006

C2A for Pulsar2 how to control your telescope from C2A

Conservation of Mechanical Energy Activity Purpose

MATLAB BASICS. Instructor: Prof. Shahrouk Ahmadi. TA: Kartik Bulusu

Newton's 2 nd Law. . Your end results should only be interms of m

Ocean Optics Educational Spectrometers. Getting Started Manual

Lab 1 Uniform Motion - Graphing and Analyzing Motion

Objectives: (a) To understand how to display a spectral image both as an image and graphically.

Electric Fields and Equipotentials

SkyGlobe Planetarium

RATE LAW DETERMINATION OF CRYSTAL VIOLET HYDROXYLATION

Assignment #0 Using Stellarium

EXPERIMENT 2 Reaction Time Objectives Theory

Lab 6: Spectroscopy Due Monday, April 10

You, too, can make useful and beautiful astronomical images at Mees: Lesson 3

AAG TPoint Mapper (Version 1.40)

Elastic and Inelastic Collisions

Experiment 1: The Same or Not The Same?

ARISTARCHOS TELESCOPE 2.3 m

Photoelectric Photometry of the Pleiades Student Manual

Experiment 14 It s Snow Big Deal

Ideal Gas Law and Absolute Zero

Linear Motion with Constant Acceleration

Determining the Concentration of a Solution: Beer s Law

Rate Law Determination of the Crystal Violet Reaction. Evaluation copy

Remote Sensing of Atmospheric Trace Gases Udo Frieß Institute of Environmental Physics University of Heidelberg, Germany

Okay now go back to your pyraf window

Students will explore Stellarium, an open-source planetarium and astronomical visualization software.

Zetasizer Nano-ZS User Instructions

Albedo and Heat Absorption

CALCULATION OF UNDERSAMPLING CORRECTION SPECTRA FOR DOAS SPECTRAL FITTING

PHY221 Lab 2 - Experiencing Acceleration: Motion with constant acceleration; Logger Pro fits to displacement-time graphs

Designing a Quilt with GIMP 2011

Temperature measurement

PROJECT GLOBULAR CLUSTERS

ES205 Analysis and Design of Engineering Systems: Lab 1: An Introductory Tutorial: Getting Started with SIMULINK

Lab 1a Wind Tunnel Testing Principles & Drag Coefficients of Golf balls

The Geodatabase Working with Spatial Analyst. Calculating Elevation and Slope Values for Forested Roads, Streams, and Stands.

Relative Photometry with data from the Peter van de Kamp Observatory D. Cohen and E. Jensen (v.1.0 October 19, 2014)

Tutorial Three: Loops and Conditionals

WATER VAPOUR RETRIEVAL FROM GOME DATA INCLUDING CLOUDY SCENES

Simulating Future Climate Change Using A Global Climate Model

Experiment 2: The Beer-Lambert Law for Thiocyanatoiron (III)

HMS-5000 Manual. Product Name: HMS-5000 Hall Effect Measurement System with variable temperature from 80K to 350K. - Manual version: ver 5.

Measuring the Redshift of M104 The Sombrero Galaxy

Lab 1: Numerical Solution of Laplace s Equation

UNIVERSITY COLLEGE LONDON. Measuring a Stellar Spectrum

AstroBITS: Open Cluster Project

Lab Activity H4 It s Snow Big Deal

DAY LABORATORY EXERCISE: SPECTROSCOPY

Lab 4: Stellar Spectroscopy

Developing a Scientific Theory

ON SITE SYSTEMS Chemical Safety Assistant

MEASUREMENT: PART II

Astronomy 154 Lab 4: The Sun. NASA Image comparing the Earth with the Sun. Image from:

The Flow of Energy Out of the Sun

Technical Procedure for Glass Refractive Index Measurement System 3 (GRIM 3)

Elastic and Inelastic Collisions

Introduction. Concepts Kinetics Order of reaction Reaction rate Colorimetry. Background

CHARTING THE HEAVENS USING A VIRTUAL PLANETARIUM

Watershed Modeling Orange County Hydrology Using GIS Data

Open Cluster Research Project

Experiment 2: The Beer-Lambert Law for Thiocyanatoiron (III)

LAB: Photometry of the Pleiades Cluster

In Association With. Introduces. TPT Contractor

Structures in the Magnetosphere 2. Hover the curser over a point on the image. The coordinates and value at that point should appear.

Quantised Conductance

Tutorial 8 Raster Data Analysis

Astronomical spectroscopy with the USB 2000 spectrometer

Experiment: Oscillations of a Mass on a Spring

Detecting Galactic HI line using 4-m SRT

FOCUS 30/FOCUS 35 Field Calibration with Survey Pro Field Software

Project 3: Molecular Orbital Calculations of Diatomic Molecules. This project is worth 30 points and is due on Wednesday, May 2, 2018.

User Manual RGB Lasersysteme GmbH Qstick Spectrometer Version: Date: November 04, 2013

Empirical Gas Laws (Parts 1 and 2) Pressure-volume and pressure-temperature relationships in gases

17-Nov-2015 PHYS MAXWELL WHEEL. To test the conservation of energy in a system with gravitational, translational and rotational energies.

CHARTING THE HEAVENS USING A VIRTUAL PLANETARIUM

Transcription:

Practical Environmental Measurement Techniques: DOAS measurements of Atmospheric Species Last change of document: April 14, 2014 Supervisor: Dr. Andreas Richter, room U2090, tel 62103, and Dr. Folkard Wittrock, room U3140, tel. 62111 Lab: room U5090 Measurements All your measurements are performed using the software running on the computer attached to the instrument. The software is a WINDOWS program designed to set-up and control the experiment and facilitate automated long-term measurements. You will need only a small part of the available commands and should avoid changing any settings not explicitly mentioned here. The supervisor will help you with the operation of the instrument, but with this document you should know about the basic points: The DOAS instrument is operated from a computer in the lab room The measurement program is usually running when you start with your practical. (If not, you start it by double-clicking on the AMAX_OMA icon on the desktop.) Most commands can be interrupted by the <ESC> key or by clicking on the STOP button, but it may take some time until the previous command is finished Taking the measurements consists of several steps: o stopping a running measurement (if necessary) o changing the settings if necessary o selecting the operation mode (SINGLE in your case) o STARTing the measurement o saving the results to a folder on the desktop, using a unique name for each measurement (see below) For each measurement, you need a corresponding dark measurement taken with the same settings except that the telescope is closed by putting a box or a cloth over the telescope. You should measure the dark signal before and after you have finished your time series with the NO 2 cell. If you want to determine the best exposure time, just type <i> when in the main menu For all measurements, you will be prompted to give a file name. Save your files in a folder on the desktop. Later you can copy it on your USB stick. Select meaningful names for the files and use the ASCII format option. The extension has always to be DAT. After you are finished, please phone the tutor. He will reset the instrument back to automatic measurements. For the NO 2 cell measurements, the best exposure time might differ for the measurements with and without cell, and you will need different dark measurements for these data sets (see below). - 1 -

Example: taking one set of measurements: Step1: set MeasurementMode to <SINGLE> Step2: insert the NO 2 cell, measurement with cell Step3: click on <START> Step4: switch off the flag Automatic Exposuretime Based on your last measurements (or use of <i>), enter a good exposure time set Mirror Position to <90> (view to the zenith) set N average to <20> Step5: start measurement <Start Measurement> Step6: wait until measurement is finished Step7: set filename set <Use ASCII File Format> set <Save Binned> do NOT set <Save Image> save file <SAVE> Step8: take a note of which exposure time the program has selected for the measurement (e.g. 0.2s), this is important for the dark measurements Step9 : remove the NO 2 cell, for measurement without cell, and repeat steps 3 to 8 In order to get a meaningful time series of the NO 2 concentration in the cell you have to repeat measurements with and without cell for at least 120 minutes. This depends on weather conditions: for low sun or rainy weather more time is needed (up to 3 hours). The time within the measurements with and without cell should be less than one minute. The time between one pair of measurements with/without cell should be less than 5 minutes. After performing all the required measurements with and without cell you can perform the dark measurements necessary for the exposure times of your data set. Step10: dark measurements: Prevent light from entering the telescope by putting a box or a cloth over it repeat from step 3 to step 7 for every exposure time you have used for measurements with and without cell. In step 4 untag the flag Automatic Exposure time and select manually Off-axis measurements After having finished the measurements with the NO 2 cell, take some real atmospheric measurements without cell. For that, take a series of measurements, one in zenith direction (90 ) and one at each elevation between 1 and 15. You can set the elevation angle in the dialogue for the SINGLE measurements. Make sure that you use good exposure times and that you perform dark measurements for all of these exposure times as well. - 2 -

- 3 -

Data Analysis In the data analysis, you will use the spectra you have recorded to determine the NO 2 content in the cell and during the horizon measurements. Also, you will use simulated atmospheric spectra supplied to you to determine the atmospheric trace gas column (e.g. ozone or bromine monoxide or formaldehyde) for one sample day. NO 2 content in the cell In the lab, you should have taken the following spectra: several pairs of measurements with and without cell a series of measurements towards the horizon and to the zenith dark current measurements for all exposure times used for the cell measurements All the corresponding files are in ASCII format and can be read into MATLAB (or any other software you like) for further analysis. The data analysis consists of the following steps, which will be explained in more detail below. Here, we concentrate on the cell measurements first: 1. read all files into MATLAB, try to program a loop to analyse all measurements in one step a. measurements with cell b. dark measurement for exposure time with cell c. measurements without cell d. dark measurement for exposure time without cell e. differential cross-section for NO 2 NO2_DIFFXSECTION.DAT 2. subtract matching dark current from measured spectra 3. apply wavelength calibration to measured spectra using the simple polynomial formula provided 4. compute the optical density (OD) of measurement by taking ln (I0/I) 5. compute differential optical density by fitting a polynomial to the OD and then subtracting this fit from the OD 6. determine slant column by fitting the provided differential cross-section to the determined differential OD 7. convert to mixing ratio for NO 2 In practice, you will have to perform the following steps (if some command is not clear then use the MatLab help or write help command to get information about command.): 1. read data [pixel, var] = textread(filename,'%f%f','headerlines',16); where var is the variable you want to read from the file read raw spectra, I read data, I0 read dark current (dark) read differential cross sections (NO2 cross sections) 2. subtract dark current from I0 and I - 4 -

3. apply wavelength calibration using the formula 2 i 1 ( i) a j i = 1 N j0 N 1 j where is the wavelength N is the number of CCD pixels: for NO 2 : N = 1024 a0.. a2 are the calibration coefficients which have the values for NO 2 (ask the supervisor for current data): a0 = 429.494 a1 = 93.112 a2 = -6.050 4. choose the values of I and I0 in the fitting window: NO2: 432.5 465 nm 5. calculate ln(i0/i) (I and I0 have already to be dark current corrected!) use function log Note: make sure you get the sign of ln(i0 / I) right or else you might get 0 as fit result 6. fit a polynomial of order 3 to ln(i0/i) use function polyfit 7. subtract the fitted polynomial from ln(i0/i) to get the differential ln(i0/i) use function polyval 8. interpolate the differential cross section to the measurement wavelengths use function interp1 Remember that in this practical only a simplified analysis is done. After the interpolation all the necessary corrections according to the full DOAS method are ready and therefore the result of the next function will be THE coefficient that you are looking for. 9. DOAS fit, fit the differential cross-section to the differential ln(i0/i) use function lscov Note: use column vectors for the cross-sections and the differential OD. The function also returns the standard error of the fitted parameter. 10. Calculate the concentration of NO 2 in the cell 11. Plot your results, for example by figure plot(wl_fit, sc.*crs_dif, wl_fit, od_diff) xlabel('wavelength (nm)') ylabel('differential optical depth') legend('scaled NO2 reference', 'measurement') grid - 5 -

In your report, please include a plot of one (or all) measured differential optical depth(s) and the scaled differential NO 2 absorption cross-section, and determine the NO 2 concentration in the cell in molec/cm 3 depending on time. In order to check if atmospheric conditions were stable during your measurements, do the same analysis as for the cell using only the measurements without cell and the very first measurement as I0. How does the NO 2 in the atmosphere change during your measurements? How does this affect your estimate of the NO 2 amount in the cell? Add a brief error discussion for your results and give some interpretation on the NO 2 time series. Also don t forget to include a printout of the script you used for the data analysis! Off-axis measurements in Bremen In principle, this part is very similar to the determination of the NO 2 content in the cell. However, you now use the atmospheric measurements at 1..15 elevation as I, and the zenith-sky measurement as I0. Compute the NO 2 slant column from these observations and discuss the magnitude, its change with elevation angle and the quality of the agreement between measured differential optical depth and absorption cross-section. Simulated trace gas columns above Bremen This last part is again very similar to the determination of the NO 2 content in the cell. However, in this step, you will use two simulated atmospheric measurements taken at different solar zenith angles (TG_x_data_sza1.DAT and TG_x_data_sza2.dat) and 3 different cross-sections TGx_DIFFXSECTION.DAT, where TGx is O3 (ozone), BrO (bromine monoxide) and HCHO (formaldehyde). The data in these files is given in the units of cm 2 /molec. For the analysis, you should use the wavelength region 336 357 nm. In a first step, find out which of these three trace gases you can identify in the simulated atmospheric spectra. Only one is present! The result of this analysis is the difference of the trace gas slant column measured at two different solar zenith angles on that day. You can convert this to a vertical column by using the airmass factors provided in the files TGx_AMF.DAT. In your report, please include a plot of the simulated differential optical depth and the scaled differential trace gas absorption cross-section, and determine the trace gas slant column in molec/cm 2. Convert the slant column to the vertical column and compare it to "expected" values from the literature. Again, add a brief error discussion. - 6 -