flowbeads: Bead Normalisation in Flow Cytometry

Similar documents
BD LSRFortessa X-20. Special Order Product. Designed for limited space and boundless potential

Technical Bulletin. Guide for Using BD Cytometric Bead Array (CBA) Flex Sets with the BD Accuri C6 Flow Cytometer. Introduction

Flow cytometer instrument set up

Průtokový cytometr CytoFLEX

PAVING THE ROAD TO UTOPIA VIA INSTRUMENT STANDARDIZATION

BD LSRFortessa X-20. Special Order Product. Designed for limited space and boundless potential

quantiflash Calibration Light Source for Cytometry

capabilities today. Flexibility for tomorrow.

Setup Procedure for Beckman Coulter CytoFLEX Flow Cytometer

ab Firefly Cytometer Setup Particles

Perform instrument startup and verification check following the manufacturer s recommendations.

BD FC Beads 7-Color Kit

Perform instrument startup and verification check following the manufacturer s recommendations.

Cytometry tutorial: The impact of adjusting PMT voltages on spillover and compensation

COMPENSATION: AN INTRODUCTION

BD OneFlow Setup Beads

BD FC Beads 7-Color Kit

K 223 Angular Correlation

SP6800 Spectral Analyzer

Operation Guide for the Leica SP2 Confocal Microscope Bio-Imaging Facility Hunter College October 2009

(Quantitative Imaging for) Colocalisation Analysis

Trademarks Cytek, the Cytek logo, and all other trademarks are property of Cytek Biosciences Cytek

AbC Total Antibody Compensation Bead Kit

Using the Normalized Image Log-Slope, part 2

ScanArray Overview. Principle of Operation. Instrument Components

Homework Set 3.5 Sensitive optoelectronic detectors: seeing single photons

Chapter 6 Introduction to Statistical Quality Control, 6 th Edition by Douglas C. Montgomery. Copyright (c) 2009 John Wiley & Sons, Inc.

Quick Guide. NucleoCounter NC-3000

Experiment 2. 2 Current Flow in the BJT. 2.1 Summary. 2.2 Theory. ELEC 3908 Experiment 2 Student#:

DSP First Lab 08: Frequency Response: Bandpass and Nulling Filters

Leica_Dye_Finder :53 Uhr Seite 6 Dye Finder LAS AF

Using Administrative Records for Imputation in the Decennial Census 1

Manual Rosetta Calibration v

Autocorrelator Sampler Level Setting and Transfer Function. Sampler voltage transfer functions

Agilent Cary 610/620 FTIR microscopes and imaging systems RESOLUTION FOR EVERY APPLICATION

GenePix Application Note

Determination of the Focal Width with the Focal Width Script

Enabling Legendary Discovery. LEGENDplex. LEGENDplex. Mul -Analyte Flow Assay Kit

LEGENDplex Mul -Analyte Flow Flow Assay Kit Kit

The Relationship Between Annual GDP Growth and Income Inequality: Developed and Undeveloped Countries

Exercise questions for Machine vision

Regression: Tree Rings and Measuring Things

2 Gain Variation from the Receiver Output through the IF Path

Zeiss 780 Training Notes

Chem466 Lecture Notes. Spring, 2004

Statistical Evaluation of Confocal Microscopy Images

BD Trucount Controls IVD

LEGENDplex. Please read the entire manual before running the assay. BioLegend.com. Please read the entire manual before running the assay.

Nikon D2x Simple Spectral Model for HDR Images

We attempted to separate the two dyes by acquiring images using a single excitation wavelength and just two emission wavelengths.

Confocal Microscopy. Kristin Jensen

Enabling Legendary Discovery. LEGENDplex. LEGENDplex. Mul -Analyte Flow Assay Kit. Mul -Analyte Flow Assay Kit

Supplementary Materials for

a Beckman Coulter Life Sciences: White Paper

Experiment 9 Bipolar Junction Transistor Characteristics

LEGENDplex. Cat. No Human Cytokine Panel 2 (13-plex) Please read the entire manual before running the assay.

ISIS A beginner s guide

Biosensors and Instrumentation: Tutorial 3

LEGENDplex. Cat. No Human CD8/NK Panel (13-plex ) Please read the entire manual before running the assay.

Developments in Electromagnetic Inspection Methods II

Leica TCS SP8 Quick Start Guide

LEGENDplex. Please read the entire manual before running the assay. BioLegend.com. Please read the entire manual before running the assay.

Performance evaluation methodology

Examination, TEN1, in courses SK2500/SK2501, Physics of Biomedical Microscopy,

Measurement and alignment of linear variable filters

Spectral Line Bandpass Removal Using a Median Filter Travis McIntyre The University of New Mexico December 2013

contents TABLE OF The SECOM platform Applications - sections Applications - whole cells Features Integrated workflow Automated overlay

PMT tests at UMD. Vlasios Vasileiou Version st May 2006

Experiment 2B Integrated Laboratory Experiment DETERMINATION OF RIBOFLAVIN: A COMPARISON OF TECHNIQUES PART B. MOLECULAR FLUORESCENCE SPECTROSCOPY

Leica TCS SP8 Quick Start Guide

The Phased Array Feed Receiver System : Linearity, Cross coupling and Image Rejection

In our previous lecture, we understood the vital parameters to be taken into consideration before data acquisition and scanning.

Mach 5 100,000 PPS Energy Meter Operating Instructions

IE 361 Module 36. Process Capability Analysis Part 1 (Normal Plotting) Reading: Section 4.1 Statistical Methods for Quality Assurance

A Kalman-Filtering Approach to High Dynamic Range Imaging for Measurement Applications

Imaging Particle Analysis: The Importance of Image Quality

LEGENDplex. Cat. No Human Proinflammatory Chemokine Panel (13-plex) Please read the entire manual before running the assay.

Enabling Legendary Discovery. LEGENDplex. LEGENDplex. Mul -Analyte Flow Assay Kit. Please read the entire manual before running the assay.

CytoFLEX Flow Cytometer Platform. Join the Resolution REVOLUTION

Section 2: Lithography. Jaeger Chapter 2 Litho Reader. The lithographic process

Introduction p. 1 Review of Radar Principles p. 1 Tracking Radars and the Evolution of Monopulse p. 3 A "Baseline" Monopulse Radar p.

Supplemental Figure 1: Histogram of 63x Objective Lens z axis Calculated Resolutions. Results from the MetroloJ z axis fits for 5 beads from each

FLAT FIELD DETERMINATIONS USING AN ISOLATED POINT SOURCE

LASER Transmitters 1 OBJECTIVE 2 PRE-LAB

Presented by Jerry Hubbell Lake of the Woods Observatory (MPC I24) President, Rappahannock Astronomy Club

Multifluorescence The Crosstalk Problem and Its Solution

Section 2: Lithography. Jaeger Chapter 2 Litho Reader. EE143 Ali Javey Slide 5-1

Improved 100GBASE-SR4 transmitter testing

Precision Flash Lamp Current Measurement Thermal Sensitivity and Analytic Compensation Techniques

Y11-DR Digital Radiography (DR) Image Quality

Supplemental Method Information Zeiss LSM710

ALTERNATIVE METHODS OF SEASONAL ADJUSTMENT

Mindfulness, non-attachment, and emotional well-being in Korean adults

CEPT/ERC Recommendation ERC E (Funchal 1998)

Multivariate Regression Algorithm for ID Pit Sizing

IBIL setup operation manual for SynerJY software version

Experiment 6: Multirate Signal Processing

EVLA Scientific Commissioning and Antenna Performance Test Check List

RGB Laser Meter TM6102, RGB Laser Luminance Meter TM6103, Optical Power Meter TM6104

Bi Imaging. Multicolor Imaging: The Important Question of Co-Localization. Anna Smallcombe Bio-Rad Laboratories, Hemel Hempstead, UK

Transcription:

flowbeads: Bead Normalisation in Flow Cytometry April 30, 2018 Abstract The flowbeads package is an extension of flowcore for bead data. It provides basic functionality for loading, gating and doing normalisation with bead data. Beads specially manufactured to known fluoresence, defined in terms of standard units of fluorescence, are routinely run in flow cytometry for the purpose of instrument quality control and normalisation. The transformation of measured intensity (Mean Fluorescence Intensity) to standard units of fluorescence, Molecules of Equivalent Fluorochrome, allows for sensible comparison of data acquired on different days and on different instruments. The parameters of the transform also correspond to basic quality control estimates of the detector linearity and the background. 1 Theory The expected fluorescent signal of a bead is determined by: ˆ the amount of fluorochrome carried by the bead ˆ the properties of the excitation source (wavelength of laser) ˆ the properties of the detector channel (bandpass and voltage) Given these properties, the Molecules of Equivalent Fluorochrome (MEF) or Molecules of Equivalent Soluble Fluorochrome (MESF) standard unit of fluorescence is calculated by the manufacturer. This theoretical value provides an absolute scale for measuring fluorescence to compare samples analysed at different times or under different laser/detector configurations (Schwartz et al., 1996; Dendrou et al., 2009). The transform from relative fluorescence to standard fluorescence is a linear transform which is estimated by linear regression of the Mean Fluorescence Intensity (MFI) of beads belonging to a number (usually six) of different populations of increasing brightness against their expected MEF fluorescence. Since the MEF of the bead populations scales multiplicatively, a chosen transform f is appropriate to linearise the data. In the case of FCS2 data, f is log 10, and in the case of FCS3, the default choice is the logicletransform of the flowcore package. On the f linearised fluorescence scale the transform is therefore: f(mef) = β f(mfi) + α MEF = f 1 (β f(mfi) + α) In the special case where the transform f is log 10, this can be further simplified to: MEF = 10 α MFI β Provided the linearity of the detector is good, the β parameter, representing the slope, is generally close to one. When the beads are run on different days, the MFIs of the bead populations move little relative to each other but 1

instead shift together as a whole, thus the intercept α, which can be interpreted as the background fluorescence, varies more than the the slope β. In order to apply the MEF transform, the MEF of the beads for a given laser/detector setup, as supplied by the manufacturer, needs to be matched to the laser/detector configuration provided in the FCS bead file. However, since not all required laser/detector properties are stored as part of the FCS 2 or 3 file format, we rely instead on the names of the detectors channels in the FCS file matching those in the MEF configuration file. As part of the flowbeads package, there is support for Dakocytomation FluoroSpheres beads (see Table 1) and ThermoFischer Scientific Cytocal for the standard LSRII and LSRFortessa laser/detector setup, but any other type of bead can be supported provided the MEF configuration file is specified. And to load the Dakocytomation configuration file into the current workspace: > data(dakomef) FITC PE PE.CY5 APC PE.TEXAS.RED 1 2 2500 1500 750 4100 552 3 6500 4400 2100 10300 2014 4 19000 14500 6900 25500 6975 5 55000 43800 22100 67300 20685 6 150000 131200 77100 139100 71888 Table 1: FluoroSpheres from Dakocytomation. The Molecules of Equivalent Fluorochromes (MEF) values for the six bead populations as provided by the manufacturer for the LSRII. The first bead population are blank as they contain contain no flurochrome by design. To load the Cytocal configuration file into the current workspace: > data(cytocalmef) Note that the underlying assumption in using beads as a reference is that the physical MEF property of these beads is more stable than the detected MFI of the bead population as reported by the instrument. For this to be true, the quality of the beads must not be compromised by age or poor storage conditions. Also it is important to keep in that in mind that if any properties of the laser/detector change, for example the voltage of the detector, then the beads need to be run again to recompute the correct transform. 2 Loading Bead Files Two example FCS 3 bead files, Dakocytomation beads ran on two different days, are included as part of the flowbeads package. These files may be loaded like so: > beads1 <- BeadFlowFrame(fcs.filename=system.file('extdata', 'beads1.fcs', package='flowbeads'), + bead.filename=system.file('extdata', 'dakomef.csv', package='flowbeads')) > beads2 <- BeadFlowFrame(fcs.filename=system.file('extdata', 'beads2.fcs', package='flowbeads'), + bead.filename=system.file('extdata', 'dakomef.csv', package='flowbeads')) Here are a few ways of extracting information from BeadFlowFrame objects: > show(beads1) 2

BeadFlowFrame object '9de89faa-c6fe-4d82-ad9b-ae64a02c3122' from 2008-01-21 with 5144 beads and 8 observables: name desc range minrange maxrange $P1 FSC <NA> 262144 0.00 262143 $P2 SSC <NA> 262144 0.00 262143 $P3 ALEXA.488 <NA> 262144-82.08 262143 $P4 PE.CY7 <NA> 262144-87.78 262143 $P5 APC <NA> 262144-26.60 262143 $P6 PE <NA> 262144-111.00 262143 $P7 ALEXA.700 <NA> 262144-77.90 262143 $P8 PACIFIC.BLUE <NA> 262144 0.00 262143 146 keywords are stored in the 'description' slot Beads MEF FITC PE PE.CY5 APC PE.TEXAS.RED 1 NA NA NA NA NA 2 2500 1500 750 4100 552 3 6500 4400 2100 10300 2014 4 19000 14500 6900 25500 6975 5 55000 43800 22100 67300 20685 6 150000 131200 77100 139100 71888 > length(beads1) [1] 5144 > getdate(beads1) [1] "2008-01-21" > getparams(beads1) [1] "ALEXA.488" "PE.CY7" "APC" "PE" "ALEXA.700" [6] "PACIFIC.BLUE" > getmefparams(beads1) [1] "FITC" "PE" "PE.CY5" "APC" "PE.TEXAS.RED" Once the bead files are loaded we can gate them to identify the distinct populations and compute the MEF transform. 3 Gating Bead Data Gating of bead data is straightforward as the number of bead populations is specified in the MEF configuration file or is known a priori. We know from the MEF file that the beads belong to six populations of increasing brightness. All channels are gated with the number of expected clusters set to the number of bead populations reported in the bead type file, which is six in the case of Dakocytomation beads. The cluster assignment is done separately on each fluorescent channel using the kmeans function and then each event is assigned to the cluster on which most channels agree on: 3

> gbeads1 <- gatebeads(beads1) > gbeads2 <- gatebeads(beads2) The initial centers for kmeans are chosen based on the assumption that there is a similar number of beads in each cluster. gbeads1 and gbeads2 are GatedBeadFlowFrame objects which contain the results of the gating. To visualise the results of the gating (see Figure 1 for gbeads1 and Figure 2 for gbeads2): > plot(gbeads1) Individual channels can be plotted like so (Figure not shown): > plot(gbeads1, 'APC') Clustering statistics are also calculated and stored in the clustering.stats slot as a three way array indexed by statistic (count, mean, standard deviation, coefficient of variation), channel (ALEXA.488, PEC.Y7, APC, PE, ALEXA.700 and PACIFIC.BLUE) and bead population (one to six). For example, the clustering stats of bead population one (the blank beads): > getclusteringstats(gbeads1)[,,1] ALEXA.488 PE.CY7 APC PE ALEXA.700 PACIFIC.BLUE count 802.00000 802.000000 802.00000 802.000000 802.00000 802.0000 mean.fi 14.89818 3.078853 119.83267 9.890424 39.53042 265.7600 sd.fi 42.92031 47.723361 71.65818 51.802289 71.06223 1435.5420 cv 288.09100 1550.037140 59.79853 523.762074 179.76592 540.1647 The GatedBeadFlowFrame defines mef.transform slot which contains a list indexed by channel name, where each element is a list containing the transformation function to apply as well as the coefficients of the transform. As we do not have MEF values for all detector channels, we only define an MEF transform for ones with matching names in the bead configuration file (in this case APC). See Figure 3 for absolute normalisation of the APC channel for gbeads1 and gbeads2. > mef.transform <- getmeftransform(gbeads1) > names(mef.transform) [1] "APC" "PE" Each MEF transform defines the parameters of the affine transform (alpha and beta): > mef.transform$apc$alpha [1] 0.321 > mef.transform$apc$beta [1] 0.948 As well as the transform itself (fun): > mef.transform$apc$fun function (x) inv.trans(b * trans(x) + a) <environment: 0x93c5ef0> The tomef function takes a GatedBeadFlowFrame and a flowframe and normalises the channels for which there is an MEF transform defined: > tomef(gbeads1, flow.data) 4

4 Relative Normalisation The MEF provides an absolute reference but we can still normalise in the absence of MEF provided we can align the MFIs across days. An advantage of relative normalisation is that we can also align the blank bead population as we do not require the MEF. Let MFI 1 be the MFI obtained from the beads on day one, and MFI 2 be the MFI obtained from the beads on day two, then the relative normalisation to compare samples from day one to day two is: f(mfi 2 ) = β f(mfi 1 ) + α To compute the transform: MFI 2 = f 1 (β f(mfi 1 ) + α) > relative.transforms <- relativenormalise(gbeads1, gbeads2) > names(relative.transforms) [1] "ALEXA.488" "PE.CY7" "APC" "PE" "ALEXA.700" [6] "PACIFIC.BLUE" We can then apply the transform, see Figure 4 for result of applying relative normalisation to gbeads1 and gbeads2. > fun <- relative.transforms$apc$fun > mfi1 <- gettransformfunction(gbeads1)(getclusteringstats(gbeads1)['mean.fi','apc',]) > mfi2 <- gettransformfunction(gbeads2)(getclusteringstats(gbeads2)['mean.fi','apc',]) > fun.mfi1 <- fun(mfi1) 5 Generating a Report Once the bead data has been gated it is possible to generate an HTML report from a template written using Markdown. These reports can then be viewed as web pages and linked to from a summary page which shows timeline data. This function is not strictly necessary as one may easily implement his own template. > generatereport(gbeads1, output.file='report.html') 5

Number of beads: 5144 Date: 2008 01 21 defaultlogicletransform(alexa.488) 0 60 defaultlogicletransform(mef) defaultlogicletransform(mef) 0 2 4 0 2 4 0 15 30 defaultlogicletransform(pe.cy7) 0.0 0.5 1.0 1.5 2.0 2.5 3.0 defaultlogicletransform(apc) defaultlogicletransform(mef) = 0.948 defaultlogicletransform(apc MFI) + 0.321 defaultlogicletransform(pe) defaultlogicletransform(mef) = 1.009 defaultlogicletransform(pe MFI) + 0.457 defaultlogicletransform(alexa.700) 0 40 defaultlogicletransform(pacific.blue) 0 40 Figure 1: Plot of gbeads1. On each detector channel, six bead populations are clustered. The MEF transform is only computed for APC since it is the only channel for which we have MEF values. 6

Number of beads: 5596 Date: 2008 03 14 defaultlogicletransform(alexa.488) 0 60 defaultlogicletransform(pe.cy7) defaultlogicletransform(mef) defaultlogicletransform(mef) 0 2 4 0 2 4 0 20 0.0 0.5 1.0 1.5 2.0 2.5 3.0 3.5 defaultlogicletransform(apc) defaultlogicletransform(mef) = 0.954 defaultlogicletransform(apc MFI) + 0.493 defaultlogicletransform(pe) defaultlogicletransform(mef) = 1.016 defaultlogicletransform(pe MFI) + 0.422 defaultlogicletransform(alexa.700) 0 15 defaultlogicletransform(pacific.blue) 0 40 Figure 2: Plot of gbeads2. The α for APC is higher than in Figure 1 which implies a higher background. The bead populations on APC are aslo noisier which implies a poorer signal-to-noise ratio on the APC channel on this day. 7

APC MFI Beads Day 2 5 APC MEF Beads Day 2 5 5 APC MFI Beads Day 1 5 APC MEF Beads Day 1 Figure 3: The result of the MEF transform is to align the MFI of the five (non-blank) bead populations across days. Notice that that the alignment of the blank bead population is not perfect since it is not used in estimating the normalisation parameters (α and β). APC MFI Beads Day 2 5 APC MFI Beads Day 2 5 5 APC MFI Beads Day 1 5 APC MFI Beads Day 1 (Relative Normalisation) Figure 4: The result of the relative MFI transform is to align the MFI of the six bead populations across both days. Note that after relative normalisation, the MFIs from all bead populations are perfectly aligned since they are all used in estimating the normalisation parameters. 8

References Calliope A Dendrou, Erik Fung, Laura Esposito, John A Todd, Linda S Wicker, and Vincent Plagnol. Fluorescence Intensity Normalisation: Correcting for Time Effects in Large-Scale Flow Cytometric Analysis. Advances in Bioinformatics, 2009:1 6, 2009. A Schwartz, EF Repollet, R Vogt, and JW Gratama. Standardizing flow cytometry: Construction of a standardized fluorescence calibration plot using matching spectral calibrators. Cytometry Part A, 26(1):22 31, 1996. 9