Instrumental Deviations from the Beer-Lambert Law

Σχετικά έγγραφα
Ε Κ Θ Ε Σ Η Δ Ο Κ Ι Μ Ω Ν


TUBO LED T8 LLUMOR PROLED ULTRA 25W 150CM

ΚΕΦ. 8 ΦΑΣΜΑΤΟΦΩΤΟΜΕΤΡΙΑ ΥΠΕΡΙΩΔΟΥΣ ΟΡΑΤΟΥ UV-Vis Μ. ΚΟΥΠΠΑΡΗΣ ΠΑΡΑΔΟΣΕΙΣ ΑΝΑΛΥΤΙΚΗΣ ΧΗΜΕΙΑΣ ΙΙ

TUBO LED T8 LLUMOR PROLED 25W 150CM

Impact of ozone cross-section choice on (WF)DOAS total ozone retrieval

TUBO LED T8 LLUMOR PROLED 18W 120CM

Electronic Supplementary Information

Optimizing Microwave-assisted Extraction Process for Paprika Red Pigments Using Response Surface Methodology

Current Status of PF SAXS beamlines. 07/23/2014 Nobutaka Shimizu

Electronic Supplementary Information (ESI)

Biostatistics for Health Sciences Review Sheet

TABLES AND FORMULAS FOR MOORE Basic Practice of Statistics

Monolithic Crystal Filters (M.C.F.)

HPLC. Spectrophotometric Measurement of Carbendazim Residue Levels in Cucumber and its Comparision with HPLC. Multivariate Curve

Πρόβλημα 1: Αναζήτηση Ελάχιστης/Μέγιστης Τιμής

Μενύχτα, Πιπερίγκου, Σαββάτης. ΒΙΟΣΤΑΤΙΣΤΙΚΗ Εργαστήριο 6 ο

ΟΙΚΟΝΟΜΕΤΡΙΑ. Βιολέττα Δάλλα. Εθνικό και Καποδιστριακό Πανεπιστήµιο Αθηνών

IV. ANHANG 179. Anhang 178

NPI Unshielded Power Inductors

Patrycja Miszczyk, Dorota Wieczorek, Joanna Gałęzowska, Błażej Dziuk, Joanna Wietrzyk and Ewa Chmielewska. 1. Spectroscopic Data.

Queensland University of Technology Transport Data Analysis and Modeling Methodologies

High Performance Voltage Controlled Amplifiers Typical and Guaranteed Specifications 50 Ω System


Artiste Picasso 9.1. Total Lumen Output: lm. Peak: cd 6862 K CRI: Lumen/Watt. Date: 4/27/2018

α + α+ α! (=+9 [1] ι «Analyze-Regression-Linear». «Dependent» ι η η η!ηη ι «Independent(s)» η!ηη. # ι ι ι!η " ι ιηη, ι!" ι ηιι. 1 SPSS ι η η ι ιηη ι η

Πανεπιστήμιο Κρήτης, Τμήμα Επιστήμης Υπολογιστών Άνοιξη HΥ463 - Συστήματα Ανάκτησης Πληροφοριών Information Retrieval (IR) Systems

Eight Examples of Linear and Nonlinear Least Squares

GAUGE BLOCKS. Grade 0 Tolerance for the variation in length. Limit deviation of length. ± 0.25μm. 0.14μm ±0.80μm. ± 1.90μm. ± 0.40μm. ± 1.

SUPPORTING INFORMATION. Diastereoselective synthesis of nitroso acetals from (S,E)- -aminated

Numerical Analysis FMN011

k A = [k, k]( )[a 1, a 2 ] = [ka 1,ka 2 ] 4For the division of two intervals of confidence in R +

Thin Film Chip Resistors

Probability and Random Processes (Part II)

difluoroboranyls derived from amides carrying donor group Supporting Information

Συνδυασμός Μαθηματικών με γραφικές παραστάσεις


ΑΝΑΛΥΣΗ Ε ΟΜΕΝΩΝ. 7. Παλινδρόµηση

Temperature: 25.5 CRH: 65% Spectrum Range: nm Scan Step: 5 nm. Spectral Distribution CIE1931 Chromaticity Diagram

SECTION II: PROBABILITY MODELS

Temperature: 25.5 CRH: 65% Spectrum Range: nm Scan Step: 5 nm. Spectral Distribution CIE1931 Chromaticity Diagram

Odometry Calibration by Least Square Estimation

Aquinas College. Edexcel Mathematical formulae and statistics tables DO NOT WRITE ON THIS BOOKLET

AI, A2, A3, A4, A5, A6, A7 AIAI, AIA2, AIA3, AIA4, AIA5, AIA6, AIA7 BI, B2, B3, B4, B5, B6, B7 BIBI, BIB2, BIB3, BIB4, BIB5, BIB6, BIB7

Μουσική Πληροφορική. Αλέξανδρος Ελευθεριάδης Αναπ. Καθηγητής Τµήµα Πληροφορικής και Τηλεπικοινωνιών Εθνικό και Καποδιστριακό Πανεπιστήµιο Αθηνών

Bulletin 1489 UL489 Circuit Breakers

Szabolcs Sofalvi, M.S., D-ABFT-FT Cleveland, Ohio

Outline Analog Communications. Lecture 05 Angle Modulation. Instantaneous Frequency and Frequency Deviation. Angle Modulation. Pierluigi SALVO ROSSI

Διερεύνηση ακουστικών ιδιοτήτων Νεκρομαντείου Αχέροντα

vibrational Supplementary density of the Beyer-

ΕΙΣΑΓΩΓΗ ΣΤΗ ΣΤΑΤΙΣΤΙΚΗ ΑΝΑΛΥΣΗ

(1) Describe the process by which mercury atoms become excited in a fluorescent tube (3)

20/01/ of 8 TOW SSD v3. C 2.78AC Σ Cumul. A*C. Tc 1 =A14+1 =B14+1 =C14+1 =D14+1 =E14+1 =F14+1 =G14+1 =H14+1 =I14+1 =J14+1 =K14+1

chlorostibine Iou-Sheng Ke and François P. Gabbai Department of Chemistry, Texas A&M University, College Station, TX

1. Ηλεκτρικό μαύρο κουτί: Αισθητήρας μετατόπισης με βάση τη χωρητικότητα

of the methanol-dimethylamine complex

Statistics 104: Quantitative Methods for Economics Formula and Theorem Review

Th, Ra, Rn, Po, Pb, Bi, & Tl K x-rays. Rn Kα1. Rn Kα2. 93( 227 Th)/Rn Kβ3. Ra Kα2. Po Kα2 /Bi K α1 79( 227 Th)/Po Kα1. Ra Kα1 /Bi K β1.

SUPPLEMENTAL INFORMATION. Fully Automated Total Metals and Chromium Speciation Single Platform Introduction System for ICP-MS

NKT NTC Thermistor. Negative Temperature Coefficient Thermistor FEATURES

Second Order RLC Filters

XKT. Metal Oxide Varistor FEATURES

Photometric Data of Lamp

First Sensor Quad APD Data Sheet Part Description QA TO Order #

Mock Exam 7. 1 Hong Kong Educational Publishing Company. Section A 1. Reference: HKDSE Math M Q2 (a) (1 + kx) n 1M + 1A = (1) =

Areas and Lengths in Polar Coordinates

Geographic Barriers to Commodity Price Integration: Evidence from US Cities and Swedish Towns,

ΚΥΠΡΙΑΚΗ ΕΤΑΙΡΕΙΑ ΠΛΗΡΟΦΟΡΙΚΗΣ CYPRUS COMPUTER SOCIETY ΠΑΓΚΥΠΡΙΟΣ ΜΑΘΗΤΙΚΟΣ ΔΙΑΓΩΝΙΣΜΟΣ ΠΛΗΡΟΦΟΡΙΚΗΣ 11/3/2006

SMD Transient Voltage Suppressors

χ 2 test ανεξαρτησίας

Electronic Supplementary Information (ESI)

Άσκηση 10, σελ Για τη μεταβλητή x (άτυπος όγκος) έχουμε: x censored_x 1 F 3 F 3 F 4 F 10 F 13 F 13 F 16 F 16 F 24 F 26 F 27 F 28 F

SUPPLEMENTARY MATERIAL. A Facile and Convenient Approach for the Synthesis of Novel Sesamol-Oxazine and Quinoline- Oxazine Hybrids

Ειζαγωγή ζηο MATLAB (MATLAB Fundamentals)

Supplementary Information 1.

Δείγμα (μεγάλο) από οποιαδήποτε κατανομή

ΕΚΘΕΣΗ ΦΩΤΟΜΕΤΡΗΣΕΩΝ PHOTOMETRIC TEST REPORT. Αντικείμενο μετρήσεων: Λαμπτήρας Ε40 με LEDs / Item tested: E40 lamp with LEDs

Enantioselective Synthesis of the Anti-inflammatory Agent ( )-Acanthoic Acid

UDZ Swirl diffuser. Product facts. Quick-selection. Swirl diffuser UDZ. Product code example:

Light Source Test Report

Thin Film Chip Resistors

Lampiran 1 Output SPSS MODEL I

Εργαστήριο Ανάπτυξης Εφαρμογών Βάσεων Δεδομένων. Εξάμηνο 7 ο

Areas and Lengths in Polar Coordinates

ΕΚΘΕΣΗ ΦΩΤΟΜΕΤΡΗΣΕΩΝ PHOTOMETRIC TEST REPORT

Quantitative chemical analyses of rocks with X-ray fluorescence analyzer: major and trace elements in ultrabasic rocks

The Echellograms and Response Functions from zj to M bands Calculated by Echelle Simulator V0.9 for IRCS

Φροντιστήριο Βιοστατιστικής. Έλεγχος Υποθέσεων. Παύλος Αγιανιάν Επικ. Καθηγητής ΔΠΘ

Υπολογιστική Φυσική Στοιχειωδών Σωματιδίων

VAR Series Zinc Oxide Varistor

Matrices and vectors. Matrix and vector. a 11 a 12 a 1n a 21 a 22 a 2n A = b 1 b 2. b m. R m n, b = = ( a ij. a m1 a m2 a mn. def

ΕΝ ΕΙΚΤΙΚΕΣ ΑΠΑΝΤΗΣΕΙΣ ΑΣΚΗΣΗΣ 2 (Εργαστήρια µαθήµατος «Στατιστικά Προγράµµατα», τµ. Στατ. & Ασφ. Επιστ., 04-05) (Επιµέλεια: Ελευθεράκη Αναστασία)

ΣΥΣΧΕΤΙΣΗ & ΠΑΛΙΝΔΡΟΜΗΣΗ

FORMULAS FOR STATISTICS 1

LED Flood Light BLP FL48W01. V(B) Range:-80-80DEG V(B) Interval: 5.0DEG Test System:EVERFINE GO-2000B_V1 SYSTEM V

LED Flood Light BLP FL16W01. V(B) Range:-80-80DEG V(B) Interval: 5.0DEG Test System:EVERFINE GO-2000B_V1 SYSTEM V

Photo-Induced Self-Assembly of Pt(II)-Linked Rings and Cages via the Photolabilization of a Pt(II) Pyridine Bond

LED Flood Light BLP FL36W01. V(B) Range:-80-80DEG V(B) Interval: 5.0DEG Test System:EVERFINE GO-2000B_V1 SYSTEM V

ΦΑΣΜΑΤΟΜΕΤΡΙΑ ΥΠΕΡΙΩΔΟΥΣ- ΟΡΑΤΟΥ, UV-Vis (ULTRAVIOLET- VISIBLE SPECTROMETRY) ΑΘΗΝΑ, ΟΚΤΩΒΡΙΟΣ 2015

ITU-R BT.1908 (2012/01) !" # $ %& '( ) * +, - ( )

Transcript:

Instrumental Deviations from the Beer-Lambert Law Measurement Spectral Absorber Maximum Absorption Unabsorbed stray Concentration Measured absorbance wavelength bandpass width Absorptivity Path length light 300 20 100 2 1 =0.0001*A23 0.01 =Sheet2.E46 0.2 =Sheet2.F46 Click the arrows above to change the values 0.5 =Sheet2.G46 0.7 =Sheet2.H46 1 =Sheet2.I46 1.2 =Sheet2.J46 1.4 =Sheet2.K46 1.6 =Sheet2.L46 1.8 =Sheet2.M46 2 =Sheet2.N46 Blue text indicates user input cells. 1 Absorption peak shape 1 Gaussian Lorentzian σ of errors =STDEV(Sheet2.E50:N50) Seite 1

Named variables W Wavelength amax Maximum absorptivity aw Absorber width (half-width of the absorption band) b Absorption path length Izero Incident intensity sl Stray light (fraction of incident light) sw Source width (spectral bandpass of monochromator) slope Slope of straight-line least squares fit to calibration curve intercept Intercept of straight-line least squares fit to calibration curve T. C. O'Haver, August 2, 2008 Seite 2

Seite 3

Seite 4

Wavelength Inst. function 200 =1-200*ABS((A3-W)/(100))/(2*sw) =IF(B3<0;0;B3) =A3+5 =1-200*ABS((A4-W)/(100))/(2*sw) =IF(B4<0;0;B4) =A4+5 =1-200*ABS((A5-W)/(100))/(2*sw) =IF(B5<0;0;B5) =A5+5 =1-200*ABS((A6-W)/(100))/(2*sw) =IF(B6<0;0;B6) =A6+5 =1-200*ABS((A7-W)/(100))/(2*sw) =IF(B7<0;0;B7) =A7+5 =1-200*ABS((A8-W)/(100))/(2*sw) =IF(B8<0;0;B8) =A8+5 =1-200*ABS((A9-W)/(100))/(2*sw) =IF(B9<0;0;B9) =A9+5 =1-200*ABS((A10-W)/(100))/(2*sw) =IF(B10<0;0;B10) =A10+5 =1-200*ABS((A11-W)/(100))/(2*sw) =IF(B11<0;0;B11) =A11+5 =1-200*ABS((A12-W)/(100))/(2*sw) =IF(B12<0;0;B12) =A12+5 =1-200*ABS((A13-W)/(100))/(2*sw) =IF(B13<0;0;B13) =A13+5 =1-200*ABS((A14-W)/(100))/(2*sw) =IF(B14<0;0;B14) =A14+5 =1-200*ABS((A15-W)/(100))/(2*sw) =IF(B15<0;0;B15) =A15+5 =1-200*ABS((A16-W)/(100))/(2*sw) =IF(B16<0;0;B16) =A16+5 =1-200*ABS((A17-W)/(100))/(2*sw) =IF(B17<0;0;B17) =A17+5 =1-200*ABS((A18-W)/(100))/(2*sw) =IF(B18<0;0;B18) =A18+5 =1-200*ABS((A19-W)/(100))/(2*sw) =IF(B19<0;0;B19) =A19+5 =1-200*ABS((A20-W)/(100))/(2*sw) =IF(B20<0;0;B20) =A20+5 =1-200*ABS((A21-W)/(100))/(2*sw) =IF(B21<0;0;B21) =A21+5 =1-200*ABS((A22-W)/(100))/(2*sw) =IF(B22<0;0;B22) =A22+5 =1-200*ABS((A23-W)/(100))/(2*sw) =IF(B23<0;0;B23) =A23+5 =1-200*ABS((A24-W)/(100))/(2*sw) =IF(B24<0;0;B24) =A24+5 =1-200*ABS((A25-W)/(100))/(2*sw) =IF(B25<0;0;B25) =A25+5 =1-200*ABS((A26-W)/(100))/(2*sw) =IF(B26<0;0;B26) =A26+5 =1-200*ABS((A27-W)/(100))/(2*sw) =IF(B27<0;0;B27) =A27+5 =1-200*ABS((A28-W)/(100))/(2*sw) =IF(B28<0;0;B28) =A28+5 =1-200*ABS((A29-W)/(100))/(2*sw) =IF(B29<0;0;B29) =A29+5 =1-200*ABS((A30-W)/(100))/(2*sw) =IF(B30<0;0;B30) =A30+5 =1-200*ABS((A31-W)/(100))/(2*sw) =IF(B31<0;0;B31) =A31+5 =1-200*ABS((A32-W)/(100))/(2*sw) =IF(B32<0;0;B32) =A32+5 =1-200*ABS((A33-W)/(100))/(2*sw) =IF(B33<0;0;B33) =A33+5 =1-200*ABS((A34-W)/(100))/(2*sw) =IF(B34<0;0;B34) =A34+5 =1-200*ABS((A35-W)/(100))/(2*sw) =IF(B35<0;0;B35) =A35+5 =1-200*ABS((A36-W)/(100))/(2*sw) =IF(B36<0;0;B36) =A36+5 =1-200*ABS((A37-W)/(100))/(2*sw) =IF(B37<0;0;B37) Seite 5

=A37+5 =1-200*ABS((A38-W)/(100))/(2*sw) =IF(B38<0;0;B38) =A38+5 =1-200*ABS((A39-W)/(100))/(2*sw) =IF(B39<0;0;B39) =A39+5 =1-200*ABS((A40-W)/(100))/(2*sw) =IF(B40<0;0;B40) =A40+5 =1-200*ABS((A41-W)/(100))/(2*sw) =IF(B41<0;0;B41) =A41+5 =1-200*ABS((A42-W)/(100))/(2*sw) =IF(B42<0;0;B42) =A42+5 =1-200*ABS((A43-W)/(100))/(2*sw) =IF(B43<0;0;B43) Izero Total intensity =SUM(C3:C43)+sl*SUM(C3:C43) Measured absorbance (y) Theoretical absorbance Seite 6

Absorptivity =IF(PeakShape="2";amax*(1/(1+((A3-300)/(0.5*aw))^2))+amax*(1/(1+((A3-150)/(0.5*aw))^2));amax*EXP(-1*((A3-300)/(0.6006*aw))^2)+amax*EXP(-1*((A3-150)/(0.6006*aw))^2)) =IF(PeakShape="2";amax*(1/(1+((A4-300)/(0.5*aw))^2))+amax*(1/(1+((A4-150)/(0.5*aw))^2));amax*EXP(-1*((A4-300)/(0.6006*aw))^2)+amax*EXP(-1*((A4-150)/(0.6006*aw))^2)) =IF(PeakShape="2";amax*(1/(1+((A5-300)/(0.5*aw))^2))+amax*(1/(1+((A5-150)/(0.5*aw))^2));amax*EXP(-1*((A5-300)/(0.6006*aw))^2)+amax*EXP(-1*((A5-150)/(0.6006*aw))^2)) =IF(PeakShape="2";amax*(1/(1+((A6-300)/(0.5*aw))^2))+amax*(1/(1+((A6-150)/(0.5*aw))^2));amax*EXP(-1*((A6-300)/(0.6006*aw))^2)+amax*EXP(-1*((A6-150)/(0.6006*aw))^2)) =IF(PeakShape="2";amax*(1/(1+((A7-300)/(0.5*aw))^2))+amax*(1/(1+((A7-150)/(0.5*aw))^2));amax*EXP(-1*((A7-300)/(0.6006*aw))^2)+amax*EXP(-1*((A7-150)/(0.6006*aw))^2)) =IF(PeakShape="2";amax*(1/(1+((A8-300)/(0.5*aw))^2))+amax*(1/(1+((A8-150)/(0.5*aw))^2));amax*EXP(-1*((A8-300)/(0.6006*aw))^2)+amax*EXP(-1*((A8-150)/(0.6006*aw))^2)) =IF(PeakShape="2";amax*(1/(1+((A9-300)/(0.5*aw))^2))+amax*(1/(1+((A9-150)/(0.5*aw))^2));amax*EXP(-1*((A9-300)/(0.6006*aw))^2)+amax*EXP(-1*((A9-150)/(0.6006*aw))^2)) =IF(PeakShape="2";amax*(1/(1+((A10-300)/(0.5*aw))^2))+amax*(1/(1+((A10-150)/(0.5*aw))^2));amax*EXP(-1*((A10-300)/(0.6006*aw))^2)+amax*EXP(-1*((A10-150)/(0.6006*aw))^2)) =IF(PeakShape="2";amax*(1/(1+((A11-300)/(0.5*aw))^2))+amax*(1/(1+((A11-150)/(0.5*aw))^2));amax*EXP(-1*((A11-300)/(0.6006*aw))^2)+amax*EXP(-1*((A11-150)/(0.6006*aw))^2)) =IF(PeakShape="2";amax*(1/(1+((A12-300)/(0.5*aw))^2))+amax*(1/(1+((A12-150)/(0.5*aw))^2));amax*EXP(-1*((A12-300)/(0.6006*aw))^2)+amax*EXP(-1*((A12-150)/(0.6006*aw))^2)) =IF(PeakShape="2";amax*(1/(1+((A13-300)/(0.5*aw))^2))+amax*(1/(1+((A13-150)/(0.5*aw))^2));amax*EXP(-1*((A13-300)/(0.6006*aw))^2)+amax*EXP(-1*((A13-150)/(0.6006*aw))^2)) =IF(PeakShape="2";amax*(1/(1+((A14-300)/(0.5*aw))^2))+amax*(1/(1+((A14-150)/(0.5*aw))^2));amax*EXP(-1*((A14-300)/(0.6006*aw))^2)+amax*EXP(-1*((A14-150)/(0.6006*aw))^2)) =IF(PeakShape="2";amax*(1/(1+((A15-300)/(0.5*aw))^2))+amax*(1/(1+((A15-150)/(0.5*aw))^2));amax*EXP(-1*((A15-300)/(0.6006*aw))^2)+amax*EXP(-1*((A15-150)/(0.6006*aw))^2)) =IF(PeakShape="2";amax*(1/(1+((A16-300)/(0.5*aw))^2))+amax*(1/(1+((A16-150)/(0.5*aw))^2));amax*EXP(-1*((A16-300)/(0.6006*aw))^2)+amax*EXP(-1*((A16-150)/(0.6006*aw))^2)) =IF(PeakShape="2";amax*(1/(1+((A17-300)/(0.5*aw))^2))+amax*(1/(1+((A17-150)/(0.5*aw))^2));amax*EXP(-1*((A17-300)/(0.6006*aw))^2)+amax*EXP(-1*((A17-150)/(0.6006*aw))^2)) =IF(PeakShape="2";amax*(1/(1+((A18-300)/(0.5*aw))^2))+amax*(1/(1+((A18-150)/(0.5*aw))^2));amax*EXP(-1*((A18-300)/(0.6006*aw))^2)+amax*EXP(-1*((A18-150)/(0.6006*aw))^2)) =IF(PeakShape="2";amax*(1/(1+((A19-300)/(0.5*aw))^2))+amax*(1/(1+((A19-150)/(0.5*aw))^2));amax*EXP(-1*((A19-300)/(0.6006*aw))^2)+amax*EXP(-1*((A19-150)/(0.6006*aw))^2)) =IF(PeakShape="2";amax*(1/(1+((A20-300)/(0.5*aw))^2))+amax*(1/(1+((A20-150)/(0.5*aw))^2));amax*EXP(-1*((A20-300)/(0.6006*aw))^2)+amax*EXP(-1*((A20-150)/(0.6006*aw))^2)) =IF(PeakShape="2";amax*(1/(1+((A21-300)/(0.5*aw))^2))+amax*(1/(1+((A21-150)/(0.5*aw))^2));amax*EXP(-1*((A21-300)/(0.6006*aw))^2)+amax*EXP(-1*((A21-150)/(0.6006*aw))^2)) =IF(PeakShape="2";amax*(1/(1+((A22-300)/(0.5*aw))^2))+amax*(1/(1+((A22-150)/(0.5*aw))^2));amax*EXP(-1*((A22-300)/(0.6006*aw))^2)+amax*EXP(-1*((A22-150)/(0.6006*aw))^2)) =IF(PeakShape="2";amax*(1/(1+((A23-300)/(0.5*aw))^2))+amax*(1/(1+((A23-150)/(0.5*aw))^2));amax*EXP(-1*((A23-300)/(0.6006*aw))^2)+amax*EXP(-1*((A23-150)/(0.6006*aw))^2)) =IF(PeakShape="2";amax*(1/(1+((A24-300)/(0.5*aw))^2))+amax*(1/(1+((A24-150)/(0.5*aw))^2));amax*EXP(-1*((A24-300)/(0.6006*aw))^2)+amax*EXP(-1*((A24-150)/(0.6006*aw))^2)) =IF(PeakShape="2";amax*(1/(1+((A25-300)/(0.5*aw))^2))+amax*(1/(1+((A25-150)/(0.5*aw))^2));amax*EXP(-1*((A25-300)/(0.6006*aw))^2)+amax*EXP(-1*((A25-150)/(0.6006*aw))^2)) =IF(PeakShape="2";amax*(1/(1+((A26-300)/(0.5*aw))^2))+amax*(1/(1+((A26-150)/(0.5*aw))^2));amax*EXP(-1*((A26-300)/(0.6006*aw))^2)+amax*EXP(-1*((A26-150)/(0.6006*aw))^2)) =IF(PeakShape="2";amax*(1/(1+((A27-300)/(0.5*aw))^2))+amax*(1/(1+((A27-150)/(0.5*aw))^2));amax*EXP(-1*((A27-300)/(0.6006*aw))^2)+amax*EXP(-1*((A27-150)/(0.6006*aw))^2)) =IF(PeakShape="2";amax*(1/(1+((A28-300)/(0.5*aw))^2))+amax*(1/(1+((A28-150)/(0.5*aw))^2));amax*EXP(-1*((A28-300)/(0.6006*aw))^2)+amax*EXP(-1*((A28-150)/(0.6006*aw))^2)) =IF(PeakShape="2";amax*(1/(1+((A29-300)/(0.5*aw))^2))+amax*(1/(1+((A29-150)/(0.5*aw))^2));amax*EXP(-1*((A29-300)/(0.6006*aw))^2)+amax*EXP(-1*((A29-150)/(0.6006*aw))^2)) =IF(PeakShape="2";amax*(1/(1+((A30-300)/(0.5*aw))^2))+amax*(1/(1+((A30-150)/(0.5*aw))^2));amax*EXP(-1*((A30-300)/(0.6006*aw))^2)+amax*EXP(-1*((A30-150)/(0.6006*aw))^2)) =IF(PeakShape="2";amax*(1/(1+((A31-300)/(0.5*aw))^2))+amax*(1/(1+((A31-150)/(0.5*aw))^2));amax*EXP(-1*((A31-300)/(0.6006*aw))^2)+amax*EXP(-1*((A31-150)/(0.6006*aw))^2)) =IF(PeakShape="2";amax*(1/(1+((A32-300)/(0.5*aw))^2))+amax*(1/(1+((A32-150)/(0.5*aw))^2));amax*EXP(-1*((A32-300)/(0.6006*aw))^2)+amax*EXP(-1*((A32-150)/(0.6006*aw))^2)) =IF(PeakShape="2";amax*(1/(1+((A33-300)/(0.5*aw))^2))+amax*(1/(1+((A33-150)/(0.5*aw))^2));amax*EXP(-1*((A33-300)/(0.6006*aw))^2)+amax*EXP(-1*((A33-150)/(0.6006*aw))^2)) =IF(PeakShape="2";amax*(1/(1+((A34-300)/(0.5*aw))^2))+amax*(1/(1+((A34-150)/(0.5*aw))^2));amax*EXP(-1*((A34-300)/(0.6006*aw))^2)+amax*EXP(-1*((A34-150)/(0.6006*aw))^2)) =IF(PeakShape="2";amax*(1/(1+((A35-300)/(0.5*aw))^2))+amax*(1/(1+((A35-150)/(0.5*aw))^2));amax*EXP(-1*((A35-300)/(0.6006*aw))^2)+amax*EXP(-1*((A35-150)/(0.6006*aw))^2)) =IF(PeakShape="2";amax*(1/(1+((A36-300)/(0.5*aw))^2))+amax*(1/(1+((A36-150)/(0.5*aw))^2));amax*EXP(-1*((A36-300)/(0.6006*aw))^2)+amax*EXP(-1*((A36-150)/(0.6006*aw))^2)) =IF(PeakShape="2";amax*(1/(1+((A37-300)/(0.5*aw))^2))+amax*(1/(1+((A37-150)/(0.5*aw))^2));amax*EXP(-1*((A37-300)/(0.6006*aw))^2)+amax*EXP(-1*((A37-150)/(0.6006*aw))^2)) Seite 7

=IF(PeakShape="2";amax*(1/(1+((A38-300)/(0.5*aw))^2))+amax*(1/(1+((A38-150)/(0.5*aw))^2));amax*EXP(-1*((A38-300)/(0.6006*aw))^2)+amax*EXP(-1*((A38-150)/(0.6006*aw))^2)) =IF(PeakShape="2";amax*(1/(1+((A39-300)/(0.5*aw))^2))+amax*(1/(1+((A39-150)/(0.5*aw))^2));amax*EXP(-1*((A39-300)/(0.6006*aw))^2)+amax*EXP(-1*((A39-150)/(0.6006*aw))^2)) =IF(PeakShape="2";amax*(1/(1+((A40-300)/(0.5*aw))^2))+amax*(1/(1+((A40-150)/(0.5*aw))^2));amax*EXP(-1*((A40-300)/(0.6006*aw))^2)+amax*EXP(-1*((A40-150)/(0.6006*aw))^2)) =IF(PeakShape="2";amax*(1/(1+((A41-300)/(0.5*aw))^2))+amax*(1/(1+((A41-150)/(0.5*aw))^2));amax*EXP(-1*((A41-300)/(0.6006*aw))^2)+amax*EXP(-1*((A41-150)/(0.6006*aw))^2)) =IF(PeakShape="2";amax*(1/(1+((A42-300)/(0.5*aw))^2))+amax*(1/(1+((A42-150)/(0.5*aw))^2));amax*EXP(-1*((A42-300)/(0.6006*aw))^2)+amax*EXP(-1*((A42-150)/(0.6006*aw))^2)) =IF(PeakShape="2";amax*(1/(1+((A43-300)/(0.5*aw))^2))+amax*(1/(1+((A43-150)/(0.5*aw))^2));amax*EXP(-1*((A43-300)/(0.6006*aw))^2)+amax*EXP(-1*((A43-150)/(0.6006*aw))^2)) Total transmitted intensity Measured absorbance = amax*b*c= Predicted concentration = Concentration error (real-predicted) Concentration error as % of max concentration Standard deviation of arrors Seite 8

Concentration =Sheet1.H3 =Sheet1.H4 =Sheet1.H5 =Sheet1.H6 =Sheet1.H7 =Sheet1.H8 =Sheet1.H9 =$C3*10^(-$D3*b*E$2) =$C3*10^(-$D3*b*F$2) =$C3*10^(-$D3*b*G$2) ### =$C4*10^(-$D4*b*E$2) =$C4*10^(-$D4*b*F$2) =$C4*10^(-$D4*b*G$2) ### =$C5*10^(-$D5*b*E$2) =$C5*10^(-$D5*b*F$2) =$C5*10^(-$D5*b*G$2) ### =$C6*10^(-$D6*b*E$2) =$C6*10^(-$D6*b*F$2) =$C6*10^(-$D6*b*G$2) ### =$C7*10^(-$D7*b*E$2) =$C7*10^(-$D7*b*F$2) =$C7*10^(-$D7*b*G$2) ### =$C8*10^(-$D8*b*E$2) =$C8*10^(-$D8*b*F$2) =$C8*10^(-$D8*b*G$2) ### =$C9*10^(-$D9*b*E$2) =$C9*10^(-$D9*b*F$2) =$C9*10^(-$D9*b*G$2) ### =$C10*10^(-$D10*b*E$2) =$C10*10^(-$D10*b*F$2) =$C10*10^(-$D10*b*G$2) ### =$C11*10^(-$D11*b*E$2) =$C11*10^(-$D11*b*F$2) =$C11*10^(-$D11*b*G$2) ### =$C12*10^(-$D12*b*E$2) =$C12*10^(-$D12*b*F$2) =$C12*10^(-$D12*b*G$2) ### =$C13*10^(-$D13*b*E$2) =$C13*10^(-$D13*b*F$2) =$C13*10^(-$D13*b*G$2) ### =$C14*10^(-$D14*b*E$2) =$C14*10^(-$D14*b*F$2) =$C14*10^(-$D14*b*G$2) ### =$C15*10^(-$D15*b*E$2) =$C15*10^(-$D15*b*F$2) =$C15*10^(-$D15*b*G$2) ### =$C16*10^(-$D16*b*E$2) =$C16*10^(-$D16*b*F$2) =$C16*10^(-$D16*b*G$2) ### =$C17*10^(-$D17*b*E$2) =$C17*10^(-$D17*b*F$2) =$C17*10^(-$D17*b*G$2) ### =$C18*10^(-$D18*b*E$2) =$C18*10^(-$D18*b*F$2) =$C18*10^(-$D18*b*G$2) ### =$C19*10^(-$D19*b*E$2) =$C19*10^(-$D19*b*F$2) =$C19*10^(-$D19*b*G$2) ### =$C20*10^(-$D20*b*E$2) =$C20*10^(-$D20*b*F$2) =$C20*10^(-$D20*b*G$2) ### =$C21*10^(-$D21*b*E$2) =$C21*10^(-$D21*b*F$2) =$C21*10^(-$D21*b*G$2) ### =$C22*10^(-$D22*b*E$2) =$C22*10^(-$D22*b*F$2) =$C22*10^(-$D22*b*G$2) ### =$C23*10^(-$D23*b*E$2) =$C23*10^(-$D23*b*F$2) =$C23*10^(-$D23*b*G$2) ### =$C24*10^(-$D24*b*E$2) =$C24*10^(-$D24*b*F$2) =$C24*10^(-$D24*b*G$2) ### =$C25*10^(-$D25*b*E$2) =$C25*10^(-$D25*b*F$2) =$C25*10^(-$D25*b*G$2) ### =$C26*10^(-$D26*b*E$2) =$C26*10^(-$D26*b*F$2) =$C26*10^(-$D26*b*G$2) ### =$C27*10^(-$D27*b*E$2) =$C27*10^(-$D27*b*F$2) =$C27*10^(-$D27*b*G$2) ### =$C28*10^(-$D28*b*E$2) =$C28*10^(-$D28*b*F$2) =$C28*10^(-$D28*b*G$2) ### =$C29*10^(-$D29*b*E$2) =$C29*10^(-$D29*b*F$2) =$C29*10^(-$D29*b*G$2) ### =$C30*10^(-$D30*b*E$2) =$C30*10^(-$D30*b*F$2) =$C30*10^(-$D30*b*G$2) ### =$C31*10^(-$D31*b*E$2) =$C31*10^(-$D31*b*F$2) =$C31*10^(-$D31*b*G$2) ### =$C32*10^(-$D32*b*E$2) =$C32*10^(-$D32*b*F$2) =$C32*10^(-$D32*b*G$2) ### =$C33*10^(-$D33*b*E$2) =$C33*10^(-$D33*b*F$2) =$C33*10^(-$D33*b*G$2) ### =$C34*10^(-$D34*b*E$2) =$C34*10^(-$D34*b*F$2) =$C34*10^(-$D34*b*G$2) ### =$C35*10^(-$D35*b*E$2) =$C35*10^(-$D35*b*F$2) =$C35*10^(-$D35*b*G$2) ### =$C36*10^(-$D36*b*E$2) =$C36*10^(-$D36*b*F$2) =$C36*10^(-$D36*b*G$2) ### =$C37*10^(-$D37*b*E$2) =$C37*10^(-$D37*b*F$2) =$C37*10^(-$D37*b*G$2) ### Seite 9

=$C38*10^(-$D38*b*E$2) =$C38*10^(-$D38*b*F$2) =$C38*10^(-$D38*b*G$2) ### =$C39*10^(-$D39*b*E$2) =$C39*10^(-$D39*b*F$2) =$C39*10^(-$D39*b*G$2) ### =$C40*10^(-$D40*b*E$2) =$C40*10^(-$D40*b*F$2) =$C40*10^(-$D40*b*G$2) ### =$C41*10^(-$D41*b*E$2) =$C41*10^(-$D41*b*F$2) =$C41*10^(-$D41*b*G$2) ### =$C42*10^(-$D42*b*E$2) =$C42*10^(-$D42*b*F$2) =$C42*10^(-$D42*b*G$2) ### =$C43*10^(-$D43*b*E$2) =$C43*10^(-$D43*b*F$2) =$C43*10^(-$D43*b*G$2) ### =SUM(E3:E43)+sl*$C$45 ### =SUM(G3:G43)+sl*$C$45 ### =LOG(Izero/E45;10) =LOG(Izero/F45;10) =LOG(Izero/G45;10) ### =E2*$D$23*b =F2*$D$23*b =G2*$D$23*b =H2*$D$23*b =I2*$D$23*b =J2*$D$23*b =K2*$D$23*b =(E46-intercept)/slope =(F46-intercept)/slope =(G46-intercept)/slope ### =E2-E48 =F2-F48 =G2-G48 =H2-H48 =I2-I48 =J2-J48 =K2-K48 =E49/$N$47 =F49/$N$47 =G49/$N$47 =H49/$N$47 =I49/$N$47 =J49/$N$47 =K49/$N$47 =STDEV(E50:N50) slope= =SLOPE(E$46:N$46;E$2:N$2) Intercept= =INTERCEPT(E$46:N$46;E$2:N$2) R2= =RSQ(E$46:N$46;E$2:N$2) Seite 10

=Sheet1.H10 =Sheet1.H11 =Sheet1.H12 Seite 11

=L2*$D$23*b ### =N2*$D$23*b =L2-L48 =M2-M48 =N2-N48 =L49/$N$47 =M49/$N$47 =N49/$N$47 Seite 12