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NIST SPECIAL PUBLICATION 260-152

U. S. DEPARTMENT OF COMMERCE/Technology Administration

National Institute of Standards and Technology

Standard Reference Materials®

Certification of a Polystyrene

Synthetic Polymer, SRM 2888

Charles M. Guttman, William R. Blair, Bruno M. Fanconi,

Robert J. Goldschmidt, William E. Wallace,

Stephanie J. Wetzel, and David L. VanderHart

oc STal institute of Standards and Technology

^ tL^"^ Dgy Administration, U.S. Department of Commerce

*;(^0' 151

2003

NIST Special Publication 260-152

Standard Reference Materials®

Certification of a Polystyrene Synthetic Polymer,

SRM 2888

Charles M. Guttman, William R. Blair, Bmno M. Fanconi. Robert J. Goldschmidt, William E. Wallace, Stephanie J. Wetzel, and David L. VanderHart

Polymers Division

Materials Science and Engineering Laboratory

National Institute of Standards and Technology

Gaithersburg, MD 20899-8540

U.S. DEPARTMENT OF COMMERCE, Donald L. Evans, Secretary TECHNOLOGY ADMINISTRATION, Phillip J. Bond, Under Secretary of Commerce for Technology NATIONAL INSTITUTE OF STANDARDS AND TECHNOLOGY, Arden L. Bement, Jr., Director Issued November 2003
Certain commercial equipment, instruments, or materials are identified in this paper in order to specify the experimental procedure adequately. Such identification is not intended

to imply recommendation or endorsement by the National Institute of Standards and

Technology, nor is it intended to imply that the materials or equipment identified are necessarily the best available for the purpose.

National Institute of Standards and Technology Special Publication 260-152

Natl. Inst. Stand. Technol. Spec. Publ. 260-152, 51 pages (November 2003)

CODEN: NSPUE2

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Mail: Stop SSOP, Washington, DC 20402-0001
Certification of a Polystyrene Synthetic Polymer, SRM 2888

Charles M. Guttman, William R. Blair, Bruno M. Fanconi, Robert J. Goldschmidt,

William E. Wallace, Stephanie J. Wetzel and David L. VanderHart

Polymers Division National Institute of Standards and Technology

Gaithersburg, MD 20899

Certain commercial materials and equipment are identified in this paper in order to specify adequately the experimental procedure. In no case does such identification imply recommendation or endorsement by the National Institute of Standards and

Technology, nor does it imply necessahly the best available for the purpose.

According to ISO 31-8, the term "Molecular Mass" has been replaced by "Relative Molecular Mass," symbol H- Thus, if this nomenclature and notation were followed in this publication, one should write H,w instead of the historically conventional Mw for the weight average Molecular Mass with similar changes for Mn, Mz, and Mv. Mw would be

called the "Mass Average Relative Molecular Mass." The conventional notation, rather than the ISO notation has been used in this publication.
Table of Contents

Abstract 4

1 .0 Introduction 5 2.0 Preparation, Bottling, and Sampling of SRM 2888 5

2. 1 Preparation 5 2.2 Botding and Sampling of SRM 2888 5

3.1 Homogeneity Testing on SRM 2888 5 3.2 Statistical Method to Compare Chromatograms 6

3.2.1 Match Factor 6

4.0 M„ by NMR 7

4.1 Solution and Solvent Preparation , 7

4.2 NMR Methods 7

4.3 Analysis of NMR Data 8 5.0 Determination of Mw of SRM 2888 by Light Scattermg 9

5.1 Light Scattering on the Polystyrene Standard 9

5.1.1 Solution and Solvent Preparation 10

5.1.2 Determination of dn/dc 10

5. 1 .3 Refractive Indices of Solvent and Calibrant 11 5.1.4 Light Scattering Methods 12

5.2 Analysis of Light Scattering Data 12

5.3 Results for SRM 2888 13 5.4 Estimation of Uncertainties Due to Systematic Effects in the Light Scattering 14

5.4.1 Contribution to Uncertainty Resulting from the Presence of Two Low Molecular Mass

Impurities in SRM 2888 14

5.4.2 Indices of Refraction 17

5.4.3 Literature Value of dn/dc for Aqueous NaCl and Calibration of the Differential Refractometer 17

5.4.4 Value of dn/dc of SRM 2888 17

5.4.5 Wavelength of Radiation 18

5.4.6 Rayleigh Ratio of Benzene 18

5.4.7 Polarizer Uncertainties 18

5.4.8 Ratio of Working Standard Scattering to Sample Scattering 19

5.4.9 Solvent Density 19

5.4.10 Solvent and Solute Masses 19

5.4.1 1 Reflection Correction 19

5.4.12 Instrumental Misalignment 20

5.4.13 Refraction Correction 20

5.4.14 Anisotropy of Solute 20

5.4.15 Cutoff of Virial Expansion for SRM 2888 20

5.4.16 Solute Degradation 21

5.4.17 Summary 21

6.0 FTIR Determination of the t-Butyl End Groups 21

7.0 MALDI-TOF- MS Analysis of Molecular Mass Distribution 22

7.1 Introduction 22

7.2 Preliminary MALDI-MS Analysis at NIST 23

7.3 Interlaboratory Protocol 23

2
7.4 Estimators of the Molecular Mass Distribution (MMD) 24

7.5 Description Of Overall Data 24

7.5.1 Mean Moments and Histogram of MMD 24

7.5.2 Outliers 24

7.5.3 Low and High Molecular Masses in the MMD 24

7.5.4 Instrument Calibration 25

7.6 Effect Of Parameters On The MMD 25

7.6.1 Statistical Methods to Describe the Data 26

7.7 Discussion of MALDI-TOF-MS 27

8.0 Conclusions 28 Acknowledgment 28

9.0 References 30

Tables 33

Table 1: Source of Uncertainty for Light Scattering Measurements on SRM 2888 33

Table 2: Moments of MMD from interlaboratory Comparison using MALDI-ToF-MS 34

Figures 35 FT-IR Spectrum of SRM 2888 35 Mass Distribution of SRM 2888 by Mass Spectrometry 36

Secondary Series in Mass Spectrum of SRM 2888 37

Distribution of Mass of SRM 2888 38

Distribution of Mn Reported in Interlaboratory Comparison 39

Distribution of End Group Mass Reported in Interlaboratory Comparison 40

Appendices '. 41 Appendix 1: Participating Laboratories In Interlaboratory Comparison 41 Appendix II: Uncertainty in PS Low Mw due to dn/dc Varying as a Function of Molecular Mass 42 Appendix III: Estimation of (dn/dc) of a Small Amount of Cyclohexane in Toluene 44

Appendix IV: Certificate of Analysis, SRM 2888 45

3
Abstract

The certification of a polystyrene standard reference material, SRM 2888, is described. The Mw of SRM 2888 was determined by light scattering to be 7.19x10^"^ g/mol with a sample standard deviation of 0.14 x10^^ g/mol. A combined expanded uncertainty for

this light scattering Mw determination, including systematic and random uncertainties, was estimated to be 0.57 xlO*"^ g/mol. Mn was determined by nuclear magnetic resonance (NMR) analysis of the end groups and found to be 6.96 xlO^"^ g/mol with an

estimated expanded uncertainty of 0.40 x1 0^"^ g/mol. Fourier transform infrared spectroscopy (FTIR) and matrix-assisted laser desorption ionization time of flight mass

spectrometry (MALDI-TOF-MS) were used to analyze end groups on the polymer. The

polystyrene was analyzed by MALDI-TOF-MS for the number (Mn) and mass (Mw) averages of the molecular mass distribution (MMD), as well as the MMD. The bottle-to- bottle variation of the SRM was examined by size exclusion chromatography (SEC) and

found to be negligible. This polymer was also used in an interlaboratory comparison of the analysis of polystyrene by MALDI-TOF-MS. The interlaboratory comparison and its results are descnbed. Agreement between the MMD moments obtained by light scattehng and

NMR and the moments of the MMD obtained by MALDI-MS in the interlaboratory

comparison is found to be good overall. However, all the experimental values obtained by MALDI-MS were lower than the classical values.

4
1.0 Introduction

This report describes certification of the Mw of SRM 2888, a polystyrene (PS), by light scattering. As supplemental numbers, the Mp by NMR end group analysis and the Mw, Mn and the MMD by MALDI-TOF-MS are also given. SRM 2888 was prepared

commercially for NIST Polymers Division for use as a standard for Size Exclusion Chromatography and as a narrow distribution polymer standard with well-defined

classical molecular mass moments for comparative studies by MALDI-MS. This

material was specially prepared and characterized for well-defined end groups. After packaging of this material for future distribution, the Mw was determined by light scattering and Mn determined by solution NMR. End groups were further studied by FTIR and MALDI-TOF-MS. The MMD was studied by MALDI-TOF-MS. The bottle-tobottle homogeneity of this Standard Reference Material (SRM) was examined by size exclusion chromatography (SEC).

2.0 Preparation, Bottling, and Sampling of SRM 2888

2.1 Preparation

The PS used for this SRM was prepared commercially by Polymer Source (Dorval, Quebec, Canada). The polymer was specially prepared by anionic polymerization with well-defined styrene and tertiary butyl end groups. From the preparation chemistry, the polymer is expected to be an atactic polystyrene of the form: (CH3)3C[CH2-CHPh]n-CH2-CH2-Ph Ph = phenyl [2.1] The material was received in the form of a powder.

2.2 Bottling and Sampling of SRM 2888

In the following, the containers holding SRM 2888 will be referred to as vials. A total of about 450 samples of SRM 2888, about 0.3 g each, were bottled in amber vials. The

entire set of samples was divided into 12 subsets. One vial was randomly selected from each subset of SRM 2888 for homogeneity testing. The first and last bottles were also taken for study. Furthermore, two bottles containing about 15 g each for use in later experiments were sampled. These are called Division Supply SRM 2888 supply in the

following discussion.

3.1 Homogeneity Testing on SRM 2888

Homogeneity testing was accomplished using SEC. A Waters Alliance 2000 GPC

Liquid Chromatograph (Waters Corp., Milford, MA) with a differential refractive index

(DRI) detector and two Styragel 300 mm x 7.5 mm ID 10 i^m HT6-E columns and one

Styragel 300 mm x 7.5 mm ID 10 ^m HT-2 column (Waters Corp., Milford, MA) were

5
used in this study. The chromatography was run at 1 .0 mL/min solvent flow rate. The

injector and column compartment of the Alliance 2000 were controlled at 40 °C for all measurements. Tetrahydrofuran, THF, (Mallinkrodt Specialty Chemicals, Paris, KY)

with added antioxidant, 2,6-di-tert-butyl-4-methyl phenol (commonly known as butylated

hydroxytoluene or BHT), was used as the solvent. Toluene (Mallinkrodt Specialty

Chemicals, Paris, KY) at a concentration of 5 pL/mL of THF was added to the solutions as a SEC pump marker. Two solutions were made from each polymer sample vial. The polystyrene samples

were dissolved in THF at a concentration of approximately 1 .5 g/L. The order of preparing the solutions and the order of acquiring the chromatograms was randomized

[1]. SEC was performed on these solutions using two injections from each solution.

After baseline subtraction, the SEC chromatograms were normalized to unit peak height

and compared initially by overlaying to decide if there were visible differences outside

the noise. The chromatograms from different solutions all superimposed on each other. This preliminary comparison showed that polymer samples taken from all the vials produced identical chromatograms. Statistical analysis on the chromatographic results, reported in Section 3.2, confirmed the visual observations.

3.2 Statistical IVIethod to Compare Chromatograms

3.2.1 IVIatch Factor

In previous SEC studies of SRMs the match factor was used to compare one

chromatogram with all the others. In this study, the match factor for chromatogram i is defined as the correlation coefficient between chromatogram i and the average chromatogram of the entire testing series. Huber [2] defined the match factor as Match Factor = 10^ {3x*y-(3x*3y)/p}2/[{3x^-3x*3x/p}{3y2-3y*3y/p}]. [3.1] The value of x is the measured signal in the ith chromatogram and y is the measured

signal from the average chromatogram at the same elution time; p is the number of data

points in the chromatogram. The sums are taken over all data points. At the extremes, a match factor of zero indicates no match and 1000 indicates an

identical chromatogram. Generally, values above 990 indicate that the chromatograms

are similar. Values between 900 and 990 indicate some similarity between

chromatograms, but the result should be interpreted with care. All values below 900 are

interpreted as an indication of different chromatograms [2,3,4]. The chromatograms were acquired in groups of eight solutions on different days. Match

factors against the average chromatogram of all the runs were obtained for both the main SRM 2888 peak and the pump marker peak of toluene. Match factor analysis on measurements taken on one particular day revealed that both the pump marker peak

and the main peak drifted a small amount during the day. This was assumed to result

6
from a small drift in the flow rate. During any day the maximum effect was less than

0.1 cm^ in the about 30 cm^ of elution volume of the pump marker peak. To

compensate for this, the chromatograms were shifted so that the pump marker peak for each chromatogram was always at the same elution volume. Applying this shift, all chromatograms from the main SRM 2888 peak in this study had match factors against

the mean chromatogram of greater than 0.998. An ANOVA study using OMNITAB [5] made on the match factors obtained from the chromatograms indicated that the match

factors of chromatograms from vials of SRM 2888 were not different using a

significance level with 0.05. The vials of SRM 2888 are indistinguishable from one another based on the above

considerations.

4.0 Mn by NMR

4.1 Solution and Solvent Preparation

Two samples of SRM 2888 were weighed into separate, clean 5-mm NMR tubes. After loading the samples, the tubes were then constricted near their tops for ease of subsequent flame sealing. Then the tubes were placed on a vacuum line and pumped

for about 5 min for drying, even though the SRM 2888 powder was not expected to pick up significant moisture (less than 0.0001 g change in the mass was found in a 0.3 g sample upon sitting in a balance in humid air for 20 min). Attached to this vacuum line was another vessel with degassed benzene-d6 (Mallinckrodt Specialty Chemicals,

Paris, KY). Sufficient benzene-d6 was then distilled into each NMR tube so that the

resulting SRM 2888 solutions were about 5 % and 13 % by mass fraction. Benzene-d6 was also distilled into an empty tube for examination of the solvent impurities. After

distillation, the samples were frozen, using a liquid nitrogen bath. Then nitrogen gas was introduced into the tubes at a pressure of about 50,000 Pa (0.5 atm); this partial pressure of nitrogen helps to prevent refluxing of the solvent during measurement. The

tubes were then flame sealed. Other 5 % solutions of SRM 2888 in CDCI3 were made by simply adding 0.6 mL of CDCI3 to the SRM 2888 powder in a 5 mm NMR tube. These solutions were

investigated by NMR mainly to ascertain the chemical identity of the 2 major impurities

residing in the SRM 2888 powder, (see additional discussion in Section 5.4.1). 4.2 NMR Methods

Proton NMR spectra at 400 MHz were acquired at ambient temperature on a WM-400

spectrometer manufactured by Bruker Instruments, Inc. Resolution was found to be adequate for evaluating the integrals of interest, for both the 5 % and the 13 %

solutions, under these conditions.

7
Spectra were taken with single pulse excitation and a pulse tip angle of 30° in order to

limit the influence of slower longitudinal relaxation times on signal amplitudes. Delay

between pulses was set at 20 s, confirmed to be conservatively long for giving

quantitative results for all protons. Resonances of the SRM 2888 were centered in a

total spectral width more than twice the range of the PS resonances in order to avoid amplitude biases from the analogue filters in the signal channel. Signal accumulations

after 64 scans had adequate signal-to-noise in the Fourier transform spectra for evaluating the integrals of interest. The Fourier transforms were made large enough, by

zero-filling, so that the relative integrals, for even the narrowest lines, were not limited by digital resolution. No tetramethylsilane (TMS) was added to these samples as a chemical shift standard.

It was deemed more important to have reliable integrals in the high-field region of the

spectra, rather than accurate chemical shifts. For a chemical shift reference, a very weak impurity line, resonating at the highest-field position, was selected. Its shift was

designated to be 0.1 ppm, presuming that it derived from a contaminant associated with vacuum greases of the polysiloxane variety. This reference gave shifts for the other resonances in reasonable agreement with expectations for PS resonance positions.

The chemical shifts that will be quoted have relative uncertainties less than 0.03 ppm,

but absolute uncertainties of 0.20 ppm.

4.3 Analysis of NMR Data

Integrals of the NMR spectra of the SRM 2888 in CeDe were measured. The assumed

structure for SRM 2888 of {CH3)3-C-[CH2-CHPh]n-CH2-CH2-Ph and the integrals (of both aromatic and aliphatic PS protons plus the end-group methyl protons) measured

from the NMR, yielded an Mn of 7.05x10^ g/mol based on measurements from the 5 %

solution and an Mn of 6.95 x10"^ g/mol, based on the measurements of the 13 %

solution. The 13 % solution spectrum had slightly inferior resolution, as expected from a more concentrated solution, but smaller corrections, arising from protonated solvent

species, had to be made to the measured aromatic integrals than for the 5 % solution. Thus, similar confidence levels were estimated for the two solutions. The above values

of Mn are based on averages of the integrals of the aliphatic and aromatic proton

spectral regions. As a comment on self-consistency, for each sample, there is less than a ±0.6 % variation in Mn if the aliphatic or aromatic integrals were used by themselves

for calculating Mn. This provides some perspective on the integration corrections to the PS resonances discussed in the following two paragraphs. These corrections involve

interfering resonances associated with both the two principal impuhties in the SRM

2888 and the protonated solvent species.

The interfering resonances in the region of the aromatic protons of PS include a weak,

solvent-related singlet associated with benzene-ds-hias well as the aromatic multiplets associated with the toluene impurity (see Section 5.4.1 ). The total intensity of the latter multiplets can be estimated from the chemical formula of toluene and the integrated

intensity of the toluene methyl protons at 2.12 ppm. The intensity of the benzene-ds-hi peak can be estimated from the fact that the pure benzene had two major proton peaks.

8
one at 7.15 ppm (benzene-d5-h1) and another unidentified peak at 0.41 ppm. Since the

latter peak occurred in all spectra and could be cleanly integrated, the benzene-ds-hi peak could be estimated based on the ratio of the 2 peaks in the spectrum of the pure

solvent. In any case, the contribution of this latter peak to the aromatic integral was less than 0.6 %. The region of the aliphatic protons of PS overlaps two narrow impurity peaks (see Section 5.4.1) which show sharp, single resonances at 1.41 (methyl protons of toluene)

and 2.12 ppm (cyclohexane). The former is situated on the upfield wing of the methylene proton resonance and the latter is found in the central resonance region of the methine protons. Because of the significant line width differences, it was possible to integrate separately the narrower impurity and broader PS lineshape contributions in spite of the overlap. Based on signal integration the total number of protons involved in these 2 impurity peaks is 0.010 times the total number of styrene protons. The spectrum of the pure solvent gave no significant impurity peaks in the vicinities of the aliphatic PS proton resonances or the end-group methyl resonances. It is worth

mentioning that Mn values were also obtained from the CDCI3 solutions of SRM 2888. While these spectra contained more interfering solvent-borne impurities, including an H2O peak that overlaps the PS aliphatic region, similar corrections to the pertinent

integrals can be applied. For 3 independent samples, the Mn values were

(6850, 6980, and 6950) g/mol, in excellent agreement with the Mn values in the CeDe

solutions. The ratio of the corrected aliphatic and aromatic integrals was always within 0.5 % of its theoretical value in these spectra; this is taken as a strong indication that the integral corrections applied were appropriate with very small systematic bias. From the above considerations a conservative estimate of the NMR-determined Mp is (6.96 + 0.20/-0.50)x10^ g/mol where the uncertainty represents the total expanded

uncertainty. While 0.20x1 O^g/mol represents the uncertainty associated with repeatable

integral measurements and absolute impurity/solvent corrections, the larger negative

uncertainty of 0.50x10^ g/mol includes a possible systematic uncertainty arising from

the fact that the range of integration of the end-group methyls is more limited than that

of the PS resonances. Resonances associated with the polymer, in contrast to those of the solvent molecules and low-molecular-mass impurities, tend to have wider wings. For weaker resonances, such as the end-group resonances, it is more difficult to identify the widest components compared to the widest components of a very strong line, e.g. the PS aliphatic line. By limiting the integral range, the very widest components are

eliminated; hence, there may be a slight, up to 4 % in this case, underestimate of the end-group integral and a consequent overestimate of Mn.

5.0 Determination of Mw of SRM 2888 by Light Scattering

5.1 Light Scattering on the Polystyrene Standard

9
5.1.1 Solution and Solvent Preparation

The polystyrene samples were weighed on an analytical balance with 0.01 mg

resolution in mass indication. Buoyancy corrections were applied.

Samples of SRM 2888 were not subjected to special drying before or during weighing

since PS powder is not generally considered to take up moisture. Less than 0.0001 g change in the mass was found in a 0.3 g sample after exposure to humid air for 20 min. The response of the balance was tested by weighing a 50 mg standard balance mass. The balance appeared to arrive at equilibrium mass within 1 min after the 50 mg

standard mass had been loaded onto the pan, and maintained the same indicated apparent mass within + 0.00001 g random variation.

Analytical reagent grade toluene (Mallinckrodt Specialty Chemicals, Paris, KY) was

used as the solvent without modification. The amount of solvent added was determined

gravimetrically on a top loading balance with 0.01 g resolution. The SRM 2888 sample was placed in solvent the afternoon before the light scattering measurements were made. The solution bottles were quiescent over night, then stirred with magnetic stirrers for about 30 min the next morning. The partial specific volume for PS in toluene tabulated as 0.917 mL/g by Brandrup and Immergut [6], and toluene

density versus temperature tabulated from several sources by Riddick and Bunger [7], were applied to compute solution concentrations at 25.0 °C. Solvent and solution samples were filtered into light scattering cells. The solvent and

solution samples were filtered through filtering assemblies with double thickness of

Millipore Fluoropore membrane (Millipore Corp., Bedford, MA) with 0.22 |am average

pore size.

5.1.2 Determination of dn/dc

The differential refractive index for SRM 2888 in toluene at 25 °C for light of 632.8 nm

wavelength was determined using a LDC/Milton Roy Chromatix KMX-16 (ThermoSeparation Products, Sunnyvale, CA) differential refractometer. The differential refractometer was calibrated against aqueous NaCI solutions.

Refractive increments versus concentration for several aqueous electrolyte solutions at several wavelengths of light were reported by Kruis [8]. Refractive increments for the same solutions at the He-Ne laser wavelength, X = 632.8 nm, have been determined

from interpolation of the data in the Kruis tables [9,10]. A cubic equation for these

refractive increments as a function of NaCI concentration in aqueous solution at 25 °C is given in the manual for the differential refractometer. This equation was used to compute the refractive increments of the aqueous NaCI solutions prepared as standards

in calibrating the differential refractometer.

10
Mallinckrodt analytical reagent NaCI was dried in a vacuum oven at 90 °C for three days

in preparation to be used as a calibrant. The dried NaCI was then maintained in a vacuum desiccator except while taking salt samples to prepare solutions. Distilled water was degassed by boiling and left to cool to ambient temperature overnight in storage bottles tightly capped with zero headspace. The storage bottles had been

leached out with several changes of boiling distilled water before being used to contain the degassed distilled water. Both salt and water components of each solution were measured gravimethcally, and atmosphehc buoyancy corrections were applied to compute the concentrations as g NaCI/100 g H2O. Measurements in the differential refractometer were conducted on seven solutions ranging in concentration from 0.5 g NaCI/100 g H2O to 2.0 g NaCI/100g H2O in intervals of 0.25 g NaCI/100 g H2O. The

calculated refractive increments of the solutions were fitted to their average image

displacements, dn/dx, to generate a linear calibration equation of refractive increment versus image displacement.

Refractive increments between solvent and solutions of SRM 2888 in toluene were

determined on solutions that had been prepared on the morning of each day during

which the measurements were conducted. The solutions were prepared by the procedure described in Section 5.1 .1

.

Image displacement measurements were conducted on four toluene solutions of SRM

2888 varying in concentration from approximately 3 g/L to 24 g/L at 25 °C. An average was taken from eight individual image displacement measurements for each solvent versus solvent and solution versus solvent pair. The average image displacement

determined for each solution was bracketed by the determination of average solvent versus solvent image displacements before and after that of the solution. The

incremental image displacement by each solution was obtained by subtracting the mean

of the bracketing solvent average image displacements from the average image

displacement by the solution. The refractive increment of each solution was computed

by application of the calibration equation to the incremental image displacement of the

solution. Linear regression analysis of the refractive increments versus the concentrations of the solutions yielded a differential refractive index, dn/dc = 0.103 mL/g

for SRM 2888 in toluene with a standard deviation of the mean of 0.0009 mU g. The differential refractive index at 632.8 nm for other comparable polystyrenes in toluene had also been determined earlier by others with values ranging from 0.081 mL/g

to 0.108 mL/g [11,12]. Applying the formula of Hadjichristdis and Fetters [12] yielded an

estimate of 0.1 05 mL/g for the dn/dc of SRM 2888. The value of 0.1 08 mL/g obtained

for SRM 2888 is considered acceptable given the fact that end group differs from the polystyrene reported [11]. 5.1.3 Refractive Indices of Solvent and Calibrant The refractive indices of toluene and of benzene, the latter used as the Rayleigh

scattering standard, were derived from tabulated values for the He-Ne laser wavelength, 632.8 nm, at 23 °C by Kaye and McDaniel [13].

11
5.1.4 Light Scattering IVIethods

Light scattering measurements on the SRM 2888 solutions in toluene were made on a Brookhaven Instrument Model BI-200 (Brookhaven Instrument Corp., Ronkonkoma, NY)

light scattering apparatus equipped with a 10 mw He-Ne laser light source. The Vv

polarization is selected for the scattered light intensity since the laser beam is vertically polarized and a vertical polarizer is used in the detector optics.

The temperature was controlled at 23.0 °C in all experiments with SRM 2888 in toluene.

In all experiments, the intensity measuring system was calibrated with the intensity of the light scattered from the beam at 90° angle by a benzene standard cell. 5.2 Analysis of Light Scattering Data

Light scattering data at Vv polarization from polymer solutions of concentration c and

scattering angle 0 may be analyzed by fitting the scattering signal 1(0, c) to [14]

In eq. [5.1], Ig is the scattering signal from the benzene working standard at 0 = 90°. We must first decide how many terms on the right-hand side must be included to provide an adequate fit to the expehmental data. The dependence of c/lc, where

Ic = sin0[l(0,c)-l(0,O)]/lG, upon c and upon sin^(0/2) reflects solute-solvent interactions and solute size, respectively. At the low molecular mass of SRM 2888 no measurable

size dependence was expected. Preliminary measurements over angles from 37.5° to 142.5° confirmed this. Thus, angle-averaged values of the Zimm function (the left hand

side of eq [5.2]) were used for analysis at any one concentration. Also angles from 60°

to 120° were taken on all further measurements.

c/lc versus a power series in c up to c^ was looked at to see if it would provide an adequate fit. The analysis revealed that the linear approximation was adequate at concentrations below 20 g/L for SRM 2888(see below).

Thus the analysis assumed the normal Zimm form

The coefficients in eq. [5.2] are related to the Mw, mean-square radius of gyration of the polymer, Rq^, and the second virial coefficients, A2, by [14]:

l(0,c) = l(0,O)+c Ig/ {(sin 0)Xij ds\r)^\e/2)} [5.1]

c Ig /[ sin 0 {l(0,c) - 1(0,0)}] = (Coo + CioC +C2oC^) [5.2]

Mw = (K'Coo)"

.-1 [5.3] A2 = 2 K'Cio [5.4]

12
As =K C20/ 3 [5.5]

K' = 47r2nB^(dn/dc)^/(VNAVv^) [5.6] where:

Xo is the wavelength in vacuum of the scattered light, 632.8 nm in this work, n and ne are the indices of refraction of the solvent and benzene taken as 1.494 and 1.497, respectively calculated as described in 5.1.3, dn/dc is the differential refractive index of the solution, measured as described in 5.1.2, Na is Avogadro's number, taken as

6.022 X 10^^ /mol, Vv^ is the Rayleigh ratio for the vertically polarized scattering of

vertically polarized light from benzene, used for calibration and obtained as described in the following paragraph.

The "vertical-vertical" Rayleigh ratio Vv is related to the Rayleigh ratio Rv for the unpolarized scattering of vertically polarized He-Ne laser and the depolarization ratio pv

for polarized light by:

Vv^ = Rv^/(1+Pv) [5.7] Using the published [13] values for benzene

Rv^ = 12.63 X 10-^ cm-^ and pv = 0.265, yields Vv^ = 9.98x 10"^cm"^

5.3 Results for SRM 2888

Six sets of light scattering solutions were made from SRM 2888 using toluene as

solvent. Each set consisted of four to five independently made up solutions. The light scattehng on each solution set was run twice, usually on consecutive days. The

polymer for each solution within each set was taken from a sample vial or from a

container designated Division Supply SRM 2888, Intensities initially were measured at ten scattering angles in the range from 37.5° to 142.5°. These measurements showed

that there was no angle dependences arising from a radius of gyration; subsequent

intensities were measured at ten scattering angles in the range from 60.0° to 120.0°. The angle averaged scattering intensities combined data from all the runs from

concentrations in the concentration range from 0.0025 g/mL to 0.040 g/mL.

A preliminary fit by least squares was made to eq. [5.2] and the results were used to calculate Mw, A2, and A3 using eq. [5.3]-[5.7]. Light scattering gave a Mw of 7.1 1x10^

g/mol with a standard uncertainty of 0.06 x 10^ g/mol, an A2 value of 0.0008 mol mL/g^

with a standard uncertainty of 0.0001 mol mL /g^ and an A3 value of 0.006 mol mL/g^

with a standard uncertainty of 0.002 mol mL /g

13
Next the data were fit over a limited concentration range dropping the A3 term. Using a bootstrap analysis with the A2 and A3 from the estimations made above, it was shown

that the effects of nonlinearity in concentration on the computed Mw started at .02 g/mL.

Thus, all data for concentrations below 0.02 g/mL were fit to an equation linear in concentration which yielded a Mw of 7.19 x 10^ g/mol with a standard uncertainty of 0.060 X 10^ g/mol, and an A2 value of 0.00096 mol mL/g^ with a standard uncertainty of 0.00005 mol mL /g^. This linear fit is taken to best represent the data, and this value of Mw is chosen as the certified value. Both this fit and the fit including the A3 term are well within the estimated uncertainty of each fit so from the point of view of the data the two numbers are indistinguishable.

The value of A2 from this fit is in good agreement with that given by the formula

obtained by Fetters et al. [15] in their review of thermodynamic properties of polymer

solutions. Using Mw of 7.19 x 10^ g/mol, an A2 value of 0.00103 mol mL/g^ is derived from the Fetters et al. formula.

In compliance with the NIST policy [16] on reporting uncertainties in measurement, the standard uncertainty reported above is multiplied by a coverage factor of 2 to obtain the component of expanded uncertainty listed in Table 1

.

5.4 Estimation of Uncertainties Due to Systematic Effects in the Light Scattering

The likeliest sources of systematic uncertainty in the determination of the Mw of SRM

2888 by light scattering were described in the preceding sections. Upper limits for their magnitudes were estimated using a scheme similar to that used in reference [14] for the estimation of systematic uncertainties in SRMs 1482, 1483 and 1484. These

uncertainties are listed in Table 1 for SRM 2888.

5.4.1 Contribution to Uncertainty Resulting from the Presence of Two Low

IVIolecular Mass Impurities in SRM 2888

Solution-state proton NMR indicated the presence of two low molecular mass impurities

in the SRM 2888 material. These impurities are also discussed in Section 4.3. The mass fractions of the impurities, derived from measured proton fractions that are normalized to the total amount of polystyrene protons, are obtained as follows: a) The

proton NMR spectrum of impurity 1 in a 5 % SRM 2888 solution in CDCI3 at ambient

temperature consists of a singlet resonance at a chemical shift of 1.43 ppm with respect

to tetramethylsilane (TMS); in CeDe, this impurity appears at 1.41 ppm. This resonance,

in CeDe, is situated near the upfield edge of the broader PS CH2 resonance; hence, the

integral of the impurity can be separated reasonably well from that of the PS. The

impurity is identified as cyclohexane from its singlet character and its chemical shifts in both solvents. Cyclohexane is difficult to remove by heating at temperatures below the glass transition of SRM 2888. The relative amount of cyclohexane can be estimated by

evaluating its integral along with the total PS integral. The fact that cyclohexane has a proton/carbon ratio of 2:1, relative to 1:1 for PS allowed determination of relative mass

14
fractions from the relative proton intensities. Considering measurement uncertainties as

well as variations in cyclohexane content from sample to sample yielded a maximum

cyclohexane mass fraction in the samples studied of 0.22 % by mass fraction. Owing to uncertainties in establishing the proper separation between cyclohexane and PS NMR

resonances, the cyclohexane integration has an uncertainty of 15 % of its value,

b) Impurity 2 also exhibits singlet resonances at a chemical shift of 2.34 ppm in CDCI3

and at 2.12 ppm in CeDe. These singlets almost certainly anse from the methyl protons

of toluene. In principle, this assignment could be verified by the aromatic spectral

fingerpnnt of toluene, which has several bands in the 7.15 ppm to 7.30 ppm range. However, that is not so easy because of the high multiplicity and subsequent weakness

of these lines plus the fact that there is strong overlap with the aromatic PS resonance and the resonances from the residual protonated-solvent species. The assignment was

based, finally, on 2 observations. First, toluene was intentionally added in two small increments to the CDCI3 solution and observed that the added intensity, for the methyl

protons, appeared at the very same shift that was present before. Even the weak

aromatic features were enhanced in a way consistent with the impurity being toluene. Second, the 2.34 ppm shift in CDCI3 and the 2.12 ppm peak in CeDe agree with published tables for the methyl protons of toluene in each solvent. Based on this chemical assignment and integrations of the methyl peak as well as the total PS

intensity, the maximum value of the mass fraction of toluene was 0.42 % by mass. The estimated uncertainty in Mw rising from the presence of the two low molecular mass

impurities was determined from the relationship derived from eq. [5.2], [5.3] and [5.6], namely,

Mw = Limit as c approaches zero of [ K*/{Cp(dn\dc)p^ )}] [5.8]

In the above equation, terms in (dn/dc) and c in eq. [5. 2], [5. 3] and [5.6] were replaced

with terms referring directly to the polymer, Cp and (dn\dc)p since it is the uncertainty

caused by the replacement of Cp , the actual polymer concentration, with Cm , the measured concentration of polymer, which is object of the discussion here. The only terms affected by the presence of low mass impurities are the change in concentration of polymer, Cp, and the change in refractive index with concentration of the polymer, (dn/dc)p. Thus

5Mw/ Mw = - 5Cp/Cp -2 8(dn/dc)p/(dn/dc)p [5.9] The contribution from each of these was estimated and added to the overall corrections

in the appropriate sections The contribution to the uncertainty from the term §Cp/Cp in the above equation may be

estimated as follows: the effect of mass is simply proportional i.e. a 1 % uncertainty in the mass of the polymer due to an impurity leads to a 1 % uncertainty in the Mw- Thus

15
this uncertainty leads to a 0.67 % uncertainty in mass. This contribution will be

considered in Section 5.4.10 where the uncertainty in the solute mass determination is discussed.

In the remaining discussion in this section, the uncertainties contributing to the term in 5(dn/dc)p are considered in some detail. The measured change in the refractive index in a dilute solution of concentration Cm, 5nm, niay be written as §nm = Cm(dn/dc)m [5.10] For the dilute solutions considered here, 5nm may be expressed as the sum of contributions from each component, the polymer (Snp), impurity 1 (5ni), and impurity 2

(5n2). Thus,

5nm = Snp + 5ni + 5n2 [5.11] and

Cm(dn/dc)m = Cp (dn/dc)p + Ci (dn/dc)i + C2 (dn/dc)2 [5.12] where

Cp = true concentration of polymer,

(dn/dc)p = change of refractive index with polymer concentration in toluene,

Ci = concentration of impurity 1 , cyclohexane,

(dn/dc)i = change of refractive index with concentration of impurity 1 in toluene,

C2 = concentration of impurity 2, toluene, and

(dn/dc)2 = change of refractive index with concentration of impurity 2 in toluene. Then dividing by Cp in eq [5.12] and letting yi = q /Cp yields,

(1+yi + y2) (dn/dc)m = (dn/dc)p + yi (dn/dc)i + y2 (dn/dc)2 [5.13] Rearranging the above equation gives,

(dn/dc)p - (dn/dc)m = yi {(dn/dc)m-(dn/dc)i} + y2 {(dn/dc)m - (dn/dc)2} [5.14] where 5 (dn/dc) = (dn/dc)p - (dn/dc)m

Since impurity 2 is toluene then (dn/dc)2 = 0.0. From the NMR y2 = 0.0042 so the

contribution from the term + y2 {(dn/dc)m -(dn/dc)2} is 0.103 * 0.0042 or 0.00044, where

for this work a value of 0.103 is taken for (dn/dc)m

To evaluate the term yi {(dn/dc)m -(dn/dc)i} an estimate of -0.09 (see Appendix ii) is used for (dn/dc)i of impunty 1 , cyclohexane, versus toluene. Thus the term {(dn/dc)m -

16
(dn/dc)i} is 0.193 and multiplying by the mass fraction y^ = 0.0022 obtained from the NMR gives 0.00043 for this term. Adding together both contributions to the 5(dn/dc) uncertainty, the total fractional uncertainty in dn/dc is 0.85 % from the impurities. The fractional uncertainty in Mw is 1.7 % or 0.13 g/mol. Since all the above are estimates of the maximum uncertainties in each component, this uncertainty is taken to be the expanded uncertainty. This

contribution is given in Table 1.

5.4.2 Indices of Refraction

Following reference [14], an estimate of 0.1 % is a proper upper limit for systematic

uncertainties in Mw arising from uncertainties in the literature values of solvent index of

refraction.

5.4.3 Literature Value of dn/dc for Aqueous NaCI and Calibration of the

Differential Refractometer

Calibration of the differential refractometer required interpolation of the data of reference

[10] to the 632.8 nm wavelength used for the light-scattering measurements. An

estimate for the uncertainty in the interpolated values of dn/dc is 0.6 %, due primarily to uncertainties in the interpolation process. The calibration factor determined for the

differential refractometer had a relative standard deviation (rsd) of 0.097 %. Combining

the above uncertainties with an allowance for possible linear uncertainties in the

refractometer, gives an estimate of 1 % for the proper upper limit for uncertainty to dn/dc from this contribution. Considered as a 95 percent confidence interval estimate,

this quoted uncertainty provides an expanded uncertainty in dn/dc of 1 % [16] which

would conthbute 2 % or 0.14 x 10^ g/mol expanded uncertainty in Mw determination.

5.4.4 Value of dn/dc of SRM 2888

5.4.4.1 Uncertainty Arising From Measured Value

The differential refractive index dn/dc of SRM 2888 in toluene at a temperature of 23 °C. was determined as described in 5.1.2. The mean value obtained for dn/dc was 0.103

mL/g, with a standard deviation of the mean of 0.0009 mL/g or 0.87 %. As the dn/dc appears raised to the second power in the Mw calculation, the uncertainty in the

calculated Mw resulting from the standard deviation in the mean of dn/dc is estimated as

twice the estimated standard uncertainty in the dn/dc, or 1.7 %. The expanded

uncertainty from this measurement is 3.4 % or 0.24 x 10^ g/mole.

5.4.4.2 Uncertainty Arising from dn/dc Variation with Molecular Mass

The differential refractive index dn/dc of low molecular mass polymers shows a molecular mass dependence arising from the effects of end groups. Generally this variation is shown to be in the form

17
dn/dc = A + B/M [5.15]

Details of the contribution due to this effect are given in Appendix ii. For this polymer

from the classical measurement an estimate Mp-Mw = -0.230 x 10^ g/mol is obtained and

choosing A from Hadjichristidis and Fetters as 0.108 mL/g yields the correction on the order of 0.023 x 10^ g/mol. The contribution to the overall expanded uncertainty from

this effect is negligible.

5.4.5 Wavelength of Radiation

For the He-Ne laser employed in this work, uncertainties in the wavelength of the

radiation are completely negligible compared with uncertainties from other sources.

5.4.6 Rayleigh Ratio of Benzene

For benzene at 632.8 nm, reference [13] gives: Rv,v+h = 12.63x10'^ cm'^ and pv = 0.265,

giving Rv,v = Rv,v+h/(1 + pv) = 9.98x10'^ cm"\ In the following discussion Rv,v+h and pv are abbreviated by R and p, respectively. The R-values reported in reference [13] are accurate to 2 % (systematic) and the relative standard uncertainty for the R-value of benzene is given as 0.21/12.63, or 1 .7 %. No estimates of either accuracy or precision

for values of p were given in reference [13]. However, p is obtained as the ratio of two

intensities, the larger of which is, or is close to, the intensity measured for the determination of R. The photomultiplier detectors were apparently operated in the

current mode, and it seems reasonable to suppose that the absolute uncertainty in the smaller intensity is the same as that of the larger, and that the relative uncertainty in the

larger is the same as that in R. Then if r is the relative standard deviation (rsd) of R, the standard deviation in p becomes sd(p) = r%(1 + p^) and rsd(1+p) = [r/(1+p)]%(1 + p^). Combining this with the rsd in R results in rsd(Rv,v) = [r/(1+p)]%2(1 + p + p^) , which is about 1.3rfor p = 0.265. The product, 1.3r = 1.3x1.7 % yields a standard uncertainty

2.2 %. This standard uncertainty combined (by root-sum-squares) with the stated standard uncertainty of 2 % for the R-values [13] yields a standard uncertainty of 3 % or 0.21 X lO'^g/mol. Applying the coverage factor of 2 to this standard uncertainty results in an expanded uncertainty of 0.42 x 10^ g/mol.

5.4.7 Polarizer Uncertainties

There are four polarizers to consider: First, the "vertically polarized" laser beam actually contains "horizontally polarized" components for two reasons: First, the polarizer inside the laser head lets through a small fraction c of the "wrong" polarization; Second, the

principal axis of polarization of the light from the laser may not be exactly perpendicular

to the plane of the incident and scattered beams. Both will cause light assumed to be

vertically polarized to contain a small admixture of horizontally polahzed light. The

effect upon scattering signals from SRM 2888 will be slight, but the effect upon the benzene calibration signals is to change the effective Rayleigh ratio that should have

been used from the Rw value toward the Rv,v+h value. The resulting uncertainty in Mw

18
is ps/(1-s) for the first effect and ptan^a, where a is the angular missetting, for the second. The uncertainty from both effects together is p[8/(1-s) + tan^a]. Second, in an exactly analogous way, the analyzing polarizer in front of the detector may be nonideal and/or mispositioned. In this case, let 5 be the contribution from the

nonideality of the polarizer, and let be the angle of missetting. The resulting

expression for the uncertainty is then: p[5/(1-5) + tan^li].

Finally, since all these uncertainties are of the same sign they are added to get:

p[s/(1-£) + tan^a + 5/(1-5) + tan^li]. From the manufacturers' specifications e and 6 are estimated to be 1/500. The uncertainty in missetting the angle of the laser is estimated as less than a = 5°. The alignment of the polarization analyzer is assumed as better than R, = 3°. Using p = 0.265 the uncertainty is 0.265[.0020 + .0077 + .0020 +

.0027] = 0.0038 = 0.4 % with at least a 95 % level of confidence considering the liberal boundaries assigned to the constituent uncertainties and their combination by linear summation instead of root-sum-of-squares. This quoted uncertainty provides an

estimated expanded uncertainty of 0.4 % or 0.03 x 10^ g/mol.

5.4.8 Ratio of Working Standard Scattering to Sample Scattering

Since photon counting techniques were employed, there should be no systematic

uncertainties from this source. Random uncertainties are reflected in the overall random uncertainty of the Mw

5.4.9 Solvent Density

The density of toluene at 25 °C, 0.86231 g/mL, given in reference [7], is estimated to be

accurate to 0.1 %, or better. The resulting expanded uncertainty on Mw is just 0.1 % or

less than 0.01 x 10^ g/mol. 5.4.10 Solvent and Solute Masses

Solvent masses in the determinations for SRM 2888 were chosen so that the solute's mass was always about 0.05 g. Using the uncertainty limit of 0.1 mg normally assigned

to the balance used to weigh the SRM 2888 samples yields uncertainties in the solute masses of 0.2 % (and negligible uncertainties in solvent masses). The resulting

expanded uncertainty in Mw is about 0.2 % or less than 0.02 x 10^ g/mol. This must be

added to the contribution to the uncertainty of Mw arising from the small molecule

impurities as discussed in Section 5.4.1 . This contnbution is about 0.67 % or 0.053 x 10^ g/mol. The two contributions together give by a sum of squares 0.060 x 10^ g/mol.

5.4.11 Reflection Correction

The refractive index of toluene at 23 °C and 632.8 nm wavelength is given [13] as

1 .4940. The refractive index of the sample cell is given by the vendor as 1 .474 at the 589 nm wavelength. Although the temperature of the toluene, and the wavelength for

19
the refractive index of the cell, in this case are not correct for our experiments, these values should be adequate to estimate what will turn out to be an extremely small

uncertainty. Substitution of these two refractive indices into Fresnel's equation for reflection from an interface between two transparent dielectrics [17] yields a reflectance

factor f = 2 X

10'"^. Comparison calculations of Mw with and without this correction for SRM 2888 show the resulting uncertainty to be less than 0.01 % or less than

0.01 X 10^ g/mol. 5.4.12 Instrumental Misalignment

For the geometry of the Brookhaven light scattering instrument, it is expected that any

deviation from constancy of I sin(0) is indicative of instrument misalignment. The I sin(0) measurements show a maximum uncertainty of 1 .0 % in the intensity compared

to the intensity at 90 degrees as a function of angle. The maximum misalignment

estimated from this is at most 1 .0°. Examination of four data sets, expanding the range

of (0.002 g/mol to 0.02) g/mol, showed that a systematic angle variation of ±1 .0° produced variations in Mw of less than 0.1 %. Since the uncertainty in alignment seems

more random than consistent, the correction is expected to be less. Thus, the expanded uncertainty arising from instrument misalignment is estimated to be less than

0.1 % or 0.01 X 10^ g/mol for SRM 2888.

5.4.13 Refraction Correction

A detailed analysis of the optical geometry of the light scattering instrument employed in this work can not be carried out, since the main detector optics unit was inaccessible. However, rough analyses based on assumptions about the internal geometry of the detector unit lead to an uncertainty of about 0.3 %. A reasonable uncertainty limit might then be about twice this, or 0.6 %, which would give an expanded uncertainty of 0.6 %

or 0.04 X 10~^ g/mol on Mw due to refraction uncertainty. 5.4.14 Anisotropy of Solute We know of no reported optical anisotropy of polystyrenes in toluene.

5.4.1 5 Cutoff of Virial Expansion for SRM 2888

As described in Section 5.2, the data fit included both linear and quadratic functions of concentration. The solution concentration range of the measurements was from

(0.002 to 0.04) g/mL. The coefficients and their uncertainties of the fits for the entire range and for limited ranges are given in Table 1 . Solution concentrations used for the

final analyses were limited to the region where linear terms in c appeared to suffice. However, as is seen from the analyses in Table 1 fitting with linear or quadratic terms had little effect on Mw. If the linear fit is used over the entire range of the data, then the

fit does not account for the curvature in the data. An estimate of the uncertainty in the calculated Mw caused by not including A3 in the data fit is given by the change in Mw

when the linear fit is made over the extended concentration range. The uncertainty in

20
estimating Mw is about 100 g/mol; the expanded uncertainty is twice this value, or 200 g/mol. Another estimation of the expanded uncertainty is made by fitting the data over

concentrations from (0.002 to 0.02) g/mol with and without the including of the quadratic

terms. These two fits give Mw that differ by no more than 100 g/mole, well within our

predicted expanded uncertainty.

Finally, an angle-average Zimm function was developed assuming Mw of 7.19x 10^ g/mol and estimating A2 and A3 from the quadratic fit described in Section 4.3. A2 is estimated to be 0.0008 mol mL/g^ and A3 is estimated to be 0.006 mol mL/g^

(Notice these values are in very good agreement with the Yamakawa estimation of the A3 = kf (A2)^Mw where kf is about 1 .0). Using this function and concentration data at the

points of our experimental points, we fit a linear functional form from (0.002 to 0.02) g/mol and found an Mw that differed from the true Mw of about 70 g/mol, much less than

the 200 g/mol in our estimate of the expanded uncertainty arising from this contribution.

5.4.16 Solute Degradation

By their nature, light scattering experiments are of short duration. A number of solutions can be prepared and examined by light scattering in a single day. Solutions were made

up one day and often run the next day. The second run on the same solutions often occurred the following day or a few days later. Allowing the solutions to sit around for many days had no noticeable effect. Furthermore, the SEC studies on SRM 2888

solutions produced no indication of degradation of the polymer over pehods of weeks. As long fresh solutions were prepared and examined within a day or two no solute degradation is apparent. As this was the procedure followed in the entire series of light scattering experiments there is no uncertainty arising from degradation.

5.4.17 Summary

The standard deviation of the mean of the determined Mw values, from analysis of variance of the experimental data, and the systematic uncertainties obtained from

Section 5.4.1 through 5.4.16 are listed in Table 1 for SRM 2888. The combined expanded uncertainties of SRM 2888 are computed as root-sum-of- squares of the component expanded uncertainties following the formal NIST policy for evaluating and expressing uncertainty in measurements [16]. The combined expanded

uncertainty of SRM 2888 is 0.57 x 10^ g/mol.

6.0 FTIR Determination of the t-Butyl End Groups

Infrared spectroscopic analysis was used to confirm the identity of the end groups and

to identify the existence of minor chemical impurities that may be present at detectible

21
levels in the as-received material. According to the synthesis, each polystyrene

molecule should contain a t-butyl group at one end and a hydrogen atom at the other end (as seen in 4.1 ). Whereas the latter group is difficult to discern in the infrared spectrum, the t-butyl group is easily identified at the 1 :70 molar ratio with styrene repeat

unit expected with this polystyrene. The FT-IR spectrum of the SRM 2888, average of 200 scans at 1.0 cm'^ resolution, is shown as the top trace in Figure 1. As a model infrared spectrum of polystyrene terminated by a t-butyl group, the infrared spectrum of neopentyl benzene, 2,2'-dimethylpropyl benzene, was recorded and shown

as the bottom trace in Figure 1. Two bands, at 1365 cm'^ and 1393 cm"\ are present in this spectrum that are identified with motions of the methyl groups of the t-butyl group

[18]. Another intense band, also attributable to the t-butyl group, occurs at 1475 cm"\

All three of these bands are evident in the infrared spectrum of the SRM 2888, top trace

in Figure 1 . To enhance visualization of conthbutions to the infrared spectrum from end

groups of SRM 2888, or chemical impurities to the extent that they exist at concentrations comparable to end groups, the spectrum of high molecular mass

polystyrene, SRM 1479 (Mw = 1,050,000 u), was recorded and subtracted from the spectrum of the sample polystyrene to remove the 'normal' polystyrene contributions. The resultant difference spectrum appears as the middle trace in Figure 1 . The infrared difference spectrum between the SRM 2888 and SRM 1479 contains three bands at 1365 cm"\ 1393 cm'^ and 1475 cm"^ that are characteristic of the t-butyl group. Although the difference spectrum contains several other bands of comparable

magnitude these appear at frequencies identical to normal infrared bands of polystyrene, and for this reason these bands cannot be unambiguously assigned to end

groups, or impurities. The absence of other bands in the difference spectrum at comparable or greater intensities suggests no chemical impurities are present with concentrations greater than 1 %.

7.0 MALDI-TOF- MS Analysis of Molecular Mass Distribution

7.1 Introduction

Matrix-assisted laser desorption/ionization time-of-flight mass spectrometry (MALDITOF-MS) [19-22] is a new and important technique in characterization of synthetic

polymer molecular mass distribution (MMD)[23-30]. In this method, the sample is prepared by mixing the analyte with a UV absorbing matrix material, organic acids are common, and a cationizing salt, such as silver trifluoroacetate, in a common solvent and

depositing the mixture on a sampling plate. A pulsed nitrogen laser ablates the sample

mixture into the gas phase producing cationized species of the analyte for traditional time-of-flight mass spectrometry analysis. Much is still unknown about the repeatability

and accuracy of the molecular mass distribution as measured by the MALDI-TOF-MS

instruments. As the number of polymer analyses by MALDI-MS has increased, scrutiny

of the MALDI-MS results in comparison to classically-obtained values for Mw and Mn has

shown they do not always agree [22,23,25,31]. For this reason, the MMD of SRM 2888

determined by MALDI-MS is presented here as supplemental data, rather than certified

22
results. To assess the repeatability of the method, the NIST Polymers Division initiated an interlaboratory comparison of SRM 2888 by MALDI-MS. This section describes the MALDI-MS analysis results of twenty-three respondents (laboratories) that participated

in the interlaboratory comparison. A fuller discussion, including participating laboratories, is given in reference [32]. In this reference, SRM 2888 is referred to as

polystyrene of nominal molecular mass 7000 u. The outline of this section is as follows. In Section 7.2 a discussion of a preliminary

MALDI-MS of the polymer is given as well as references to further research on the MALDI-MS of the polymer. In Section 7. 3, a bnef description of the protocol for the

interlaboratory comparison is given. In Section 7.4, two kinds of descriptors of the data

are defined, including traditional polymer moments of Mn, Mw and Mz. The statistical analysis of all the data using these descriptors is given in Section 7.5. The effects of various parameters are described in Section 7.6, including the distinction between and

within laboratory and the effects of choice of mathx materials. Finally, in Section 7.7 summarizes some conclusions from the interlaboratory comparison.

7.2 Preliminary MALDI-MS Analysis at NIST

A preliminary MALDI analysis on SRM 2888 was conducted at NIST on a Bruker REFLEX II MALDI-TOF-MS (Billerica, MA) to ascertain that the polystyrene was

consistent with the structure shown in [2.1]. The spectral main peaks. Figure 2, from a

calibrated instrument agreed well with the structure in [2.1]. However, the MALDI mass

spectrum revealed an unexpected secondary series of peaks, also with 104 u mass

separations, in addition to the expected main series ions; see Figure 3. One possibility was that some of these intermediate peaks indicated end groups not seen in the FTIR. However, additional experimentation on the polystyrene sample revealed that the secondary series peak position changed with respect to the main series peaks when

different matrices were used. Post-source decay [33] was used to determine that the secondary peaks arose from two sources: either adducts of the matrix and/or cations

with the polymer or fragmentation of the polymer along the main chain. The matnx salt adducts caused the secondary peaks to shift when different matrices were used. None

of the secondary peaks were attributable to additional end groups. Details of how these

attributions were established are given in reference [33]. 7.3 Interlaboratory Protocol

Each participating laboratory was instructed to perform MALDI-MS using two protocols

involving different sample preparations. The first protocol required retinoic acid for the matnx and AgTFA for the salt [28]. The second protocol allowed each laboratory to use

a sample preparation of their choosing. Each laboratory was asked to produce three MALDI spectra for each protocol to check for intralaboratory variability. Six spectra are obtained from two sample preparations for each laboratory. Each laboratory reported Mn and Mw for each spectrum as well as the integrated mass intensity signal for each

separate peak of the PS mass spectrum with the cation mass subtracted from the peak

masses. The Mn and Mw values used in the following discussions were obtained from

23
the analysis of reported integrated signal peak intensities, rather than reported values of Mn and Mw owing to discrepancies in the methods used by some of the participants to determine values of Mn and Mw

7.4 Estimators of the Molecular Mass Distribution (MMD)

To facilitate the analysis of the data, particularly in the tails of the mass distribution where issues of cut-off and baseline may influence the determined moments of the

distribution, the integrated peak intensities of each data set were separated into eleven mass divisions, or bins, before comparison. The bins are taken to be six PS repeat

units, 625 u, in width, except for bins 1 and 1 1 , which contain the remaining area of the

tails. The bin area of the distribution is then used for the statistical comparison.

7.5 Description Of Overall Data

7.5.1 Mean Moments and Histogram of MMD

The mean number-average molecular mass (Mn) of the entire data set, using all instruments and both protocols, was found to be 6609.89 u. The standard deviation (o) was found to be 120.64 u, and the standard uncertainty of the mean (o/VN) was 11.77 u

[36] where N is 105. The standard deviation is approximately equivalent to one repeat

unit of polystyrene, 104 u, giving a very narrow distribution of data. The mean of the moments Mn, Mw, and Mz, the standard deviations and the standard uncertainty of the mean are given in Table 2. These data are also represented in Figure 4, which illustrates the mean distribution of the bins for the data obtained using protocol 1 . The bins are normalized, therefore

indicating the fraction of the total MMD that they contain. The bin means show that bins

1 and 2 make up less than 4 % of the MMD. Also bins 9, 10 and 1 1 make up less than 4 % of the MMD. The histogram of the mean bins in Figure 4 is Gaussian.

7.5.2 Outliers A statistical analysis of Mn values was used to identify data sets that contributed to erroneous evaluations (outliers). These data sets were deleted in subsequent analysis

to prevent erroneous influences. Since the Mn distribution is normally distributed, a normal distribution can be used to identify the outliers of the distribution. Three

standard deviations of a normal disthbution contain 99.8 % of the data; any values that

lie outside of this range are considered outliers [35]. Figure 5 shows the distribution of the Mn data and the fitted normal curve for these data. Three laboratories reported mass distributions, which yielded moments that fell outside of three standard deviations

of the mean of the normal distribution. For the purposes of this analysis, these data

points were classified as outliers and excluded from further data analyses.

7.5.3 Low and High Molecular Masses in the MMD

24
Due to the method of assigning bins, some laboratories' results contained no data in the

bins representing the tail regions of the MMD. For the low mass tail of the distribution 55 % of the laboratohes reported no data in bin 1, and 10 % reported no data in bin 2. The missing data were more extreme in the high mass tail, presumably due to a loss of instrument sensitivity in the high mass region. In bin 10, 45 % of the laboratories' resulting data sets contained no data, and 85 % of data sets contained no data in bin

1 1 . The loss of data in the tail regions may be a result of instrument sensitivity and

resolution, or may be a result of baseline correction and integration. Each of the

different instrument types produced data sets that lacked data in the tails of the

distribution. Based on examination of the above-mentioned outlier data, it appears that some missing data are attributable to the influence of the integration methodology.

Depending on the software used, peaks in the tail regions with baseline noise are very

easily missed by peak selection software.

7.5.4 Instrument Calibration The accuracy of the instrument calibration of each laboratory was assessed by

calculation of the end group mass. The masses of the end groups of SRM 2888 were

calculated by taking the difference between the mass of the maximum signal of the

distribution and the calculated mass from the number of repeat units; the cation mass

has already been subtracted. Figure 6 shows the distribution of the calculated end

group masses. The end groups are tert-butyl and hydrogen (as seen in [2.1]) and have

a total mass of 58.14 u. The calibration of most TOF mass spectrometers are expected

to be accurate to less than 3 u, but as can be seen in Figure 6, some laboratories' calibrations were off over 40 u. Consideration was given to whether the inaccuracy of the instrument calibrations would cause uncertainties in the data analysis. When compensations were made to Mp due to these calibration discrepancies, the value of the mean Mn was only slightly altered, and

the variance of the Mn values decreased slightly. When the corrected Mn was analyzed,

the results of analysis presented in the following sections were not altered. Therefore, the corrections were not continued in the statistical analysis described below.

7.6 Effect Of Parameters On The MMD

In the analysis of the interlaboratory comparison data, several parameters were

considered as possible influences on the SRM 2888 molecular mass distribution. The

parameters examined were reporting laboratory, sample preparation method,

instrument manufacturer, and TOF-MS instrument mode (reflectron or linear). Whether

the laboratory in which the polymer is examined has an influence on the MMD is an

important test of the consistency of the MALDI-TOF-MS method of polymer

characterization. The type of matrix used in sample preparation of the polymer for MALDI analysis may also be a significant parameter. The two matrices preparations

compared in this analysis were all-trans retinoic acid and dithranol. Other matrix preparations were used, but not by a sufficient number of laboratories for statistical comparison. The parameter "instrument" classifies by instrument manufacture, not the

25
model of the instrument. The mode of the instrument, linear or reflectron, was not evaluated owing to insufficient data.

7.6.1 Statistical Methods to Describe the Data

Analysis of variance (ANOVA), a standard statistical analysis tool, was used to make

inferences about the data populations [35]. Both one-way and two-way ANOVA tests were used with the latter assessing effects of two parameters on the response variable. The two-way ANOVA considers that effects due to one parameter may mask the effects due to the second parameter. The effects of each factor are called main effects and

one, both, or neither may turn out to be significant. In addition to these main effects (and independent of them) there may be an effect due to their interaction that accounts

for how simultaneous changes in the two parameters affect the response variable.

7.6.1 .1 Effect of Laboratory on the MMD

The statistical analysis of the reporting laboratory included only data that were taken

using protocol 1 for sample preparation. Since each participating laboratory prepared

samples a positive laboratory effect may be due also to a sample preparation effect. After outliers were identified and removed, as well as laboratories that did not include three mass spectra repeats of the polystyrene, 16 laboratories were included in the

analysis.

A one-way ANOVA of the moments for the laboratory parameter showed a significant effect on the molecular mass distribution. The ANOVA of the bins for the laboratory

parameter revealed a significant effect on each of the bins of the molecular mass

distribution. Surprisingly, even the center bins, which are expected not to be as

sensitive to the moments as the bins representing the tails, showed a large variation among laboratohes. But the one-way ANOVA of the laboratory parameter does not give conclusive results, because the instrument parameter and laboratory parameter are confounded. The

confounding exists because each laboratory used only one instrument type. Therefore,

two-way ANOVA was used to differentiate the two effects. The two-way ANOVA first accounts for the effect of instrument and then the effect of laboratory. Because of the confounding of the instrument and laboratory parameters,

the data set was reduced to include only those instruments run by multiple laboratories,

leaving 13 laboratories in the statistical analysis. In the two-way ANOVA, when the instrument parameter is accounted for, the laboratory parameter is found to have a

significant effect on all of the moments and all of the bins representing the molecular mass distribution of polystyrene. 7.6.1.2 Effect of Instrument on the MMD

The instrument variable considers all instruments from the same manufacturer together as one parameter, regardless of the model of the instrument. The six different

26
instrument types represented in our study were Bruker, PerSeptive, Physical

Electronics' Trift, Micromass, ThermoBioanalysis Vision, and several homemade

instruments. Of these, only three instrument types were used by more than one

laboratory; only the 13 laboratories that ran one of these three instrument types were

included in the analysis. As well, only data reported from the defined sample

preparation protocol were considered in the statistical analysis.

In order to determine the effect of instrument on the molecular mass distribution, the

influence of the laboratory parameter must be removed. This was achieved by taking the mean of the three determinations of moments (or bins) from each laboratory. These

laboratory means can then be analyzed by a one-way ANOVA for the instrument parameter.

The ANOVA of the mean laboratory moments for the instrument parameter yielded no

significant effect of instrument on the molecular mass distribution. The variation within instrument type was not significantly less than the variation among instruments. When

the bins were examined by this method, only bin 8 was significantly influenced by the instrument parameter. Bin 8 represents 7 % of the MMD and represents the high mass

tail of the distribution. Overall, the instrument has little influence on the molecular mass

distribution.

7.6.1.3 Effect of Different Matrices on the MMD

For analysis of sample preparation, only the 6 laboratories that ran both dithranol and

retinoic acid as matrices, were considered in the analysis. A two-way ANOVA of the data accounted first for laboratory effects, and then assessed the influence of the matrix on the moments and bins of the molecular mass distribution. The instrument parameter

is also considered in this statistical method, because the instrument parameter is accounted by the laboratory parameter.

The two-way ANOVA results revealed that the matrix used in the sample preparation

did not significantly influence the moments of the molecular mass distribution. When

the bins were analyzed, only bin 3 was significantly influenced by the matrix parameter.

Bin 3 includes data in the low mass tail of the polymer molecular mass distribution that represents 6 % of the MMD. Thus the matrix type may have an effect on the low mass

tail of the polymer distribution.

7.7 Discussion of MALDI-TOF-MS

The Mw and Mn obtained by MALDI-TOF-MS for the interlaboratory companson were

found to be 6.74 x10"^ g/mol and 6.61 xlO^ g/mol, respectively, with a standard deviation

of 0.1 1 xlO^ g/mol for Mw and 0.12 xlO^ g/mol for Mn. The MALDI-MS gives lower Mn

and Mw than determined by classical methods. The estimated expanded uncertainties

of the classical methods encompass the Mn and Mw averages obtained by MALDI-MS

However, the estimated expanded uncertainty of the classical methods includes systematic uncertainty evaluated as type B uncertainty. The MALDI-MS data does not

27
have an estimated systematic uncertainty. In fact, much of the research directed at MALDI-TOF-MS is aimed at estimating and lowering the systematic uncertainty, or type B uncertainty. However, it is noteworthy that the Mn and Mw values obtained by MALDI- MS in every reporting laboratory were lower than the Mn and Mw obtained by classical methods. The largest value of Mn reported was still 200 u less than the Mn obtained from NMR. The disagreement of the Mn and Mw obtained by MALDI-MS and the

classical methods may be too great to be attributed to instrumental and statistical uncertainties alone, particularly since the bulk of the uncertainty in NMR and light scattering arise from very different causes. This combined with the fact that the standard statistical uncertainty from the MALDI-MS is so small, leads to the possibility that the systematic uncertainties in MALDI-TOF-MS may be biased in one direction. Discussion of possible sources of systematic uncertainties is given in reference [32].

8.0 Conclusions

The Mw of SRM 2888, the same material used in a MALDI-TOF-MS Interlaboratory

Comparision, was certified by light scattering to have a value of Mw of 7.19 x 10^ g/mol

with a sample standard deviation of 0.14 x 10^ g/mol and an estimated expanded

uncertainty of 0.57 x 10"^ g/mol. The Mn, measured by end group analysis by NMR, was

found to be 6.96 x 10^ g/mol with an estimated expanded uncertainty of 0.40 X lO'^ g/mol. This is reported here as a supplemental number. The uncertainty estimates for the certified value of Mw by light scattering included both repeatability, a

type A evaluation of uncertainty, and systematic uncertainties, a type B evaluation of uncertainty [17]. The Mw and Mn obtained by MALDI-TOF-MS for the interlaboratory

comparison were found to be 6.74 x 10^ g/mol and 6.61 x 10"^ g/mol, respectively, with a standard deviation of 0.11 x 10^ g/mol for Mw and 0.12 x 10^ g/mol for Mn. These are

also reported here as supplemental values, as well as the MMD reported in Figure 4. NMR and FTIR analysis confirmed that SRM 2888 has only one pair of end groups, as

expected from the method of polymer synthesis. This is consistent with MALDI-MS

results obtained at NIST. Bottle-to-bottle variability on the SRM 2888 vials was found to be below detectable levels by size exclusion chromatography.

For the MALDI-TOF-MS Interlaboratory Comparison, the ANOVA analysis of the data showed that the variation among participating laboratories was significant. The type of instrument used in obtaining the MMD had little influence on the data Only the bin data

for one bin showed an influence of instrument type. The matrices that were used in the sample preparation of the polystyrene for MALDI-MS-TOF analysis did not have a

significant influence on the molecular mass distribution. Acknowledgment

The authors thank participants from laboratories that contributed to the interlaboratory

comparison. S.J.W. thanks the National Science Foundation for the Chemometric

Fellowship, Prof. Nancy Flournoy of American University, and NIST for the research

28
capabilities. C.IVl.G. and S.J.W. thank Dr. Mark Levenson of the NIST Statistical Engineering Division for assistance with the statistical analysis of the MALDI-MS data.

29
9.0 References

[I] M.G. Natrella, "Experimental Statistics", National Bureau of Standards Handbook 91, U.S. Department of Commerce, 1963.

[2] L. Huber, "Application of the Diode-Array Detector in HPLC", Hewlett Packard,

France, 08/89, pg. 89-100

[3] B.J. Bauer, B. Dickens and W.R. Blair, "Chromatographic Examination of Intaglio Inks, Resins and Varnishes", NISTIR 4949, 1991

[4] CM. Guttman, W.R. Blair, J.R. Maurey, "Recertification of SRM 1482a, a

Polyethylene", NISTIR 6054, 1997, available from National Technical Information

Service, Technology Administration, U.S. Department of Commerce, Springfield, VA

22161

[5] "PC-OMNITAB: An Interactive System for Statistical and Numerical Data Analysis," available from National Technical Information Service, Technology Administration, U.S. Department of Commerce, Springfield, VA 22161

[6] J. Brandrup and E.H. Immergut, editors, "Polymer Handbook, Third Edition", John

Wiley and Sons, New York, 1989, section VIII pg. 93

[7] J. A. Riddick and W. B. Bunger, "Organic Solvents, Physical Properties and Methods

of Purification," Wiley-lnterscience, New York, 1970, Table 58, pg 145. or Table 30, pg 107.

[8] A. Kruis, Z. Physik. Chem. B 34, 13-50 (1936).

[9] R. J. Anderson, Appl. Opt. 8, 1508-1509 (1969).

[10] LDC Analytical, "Instruction Manual for KMX-16 Laser Differential Refractometer"

Section 5.3, "Calculation of Calibration Constant," Riviera Beach, PL, USA

[II] K. Matsuo, W.H. Stockmayer, F. Bangerter, Macromolecules 18, 1346-1348 (1985)

[12] N. Hadjichristidis, L.J. Fetters, Jour. Poly. Sci. Poly Phys. Ed 20, 2163-2166 (1982)

[13] W. Kaye and J. B. McDaniel, Appl. Opt. 13, 1934-1937 (1974)

[14] Charles C. Han, Herman L. Wagner, and Peter H. Verdier, "The Characterization of Linear Polyethylene SRM's 1482, 1483, and 1484 III Weight-Average Molecular Masses by Light Scattering." NBS Special Publication 260-61 , P.H. Verdier and

H.L. Wagner ed. December 1978 or National Bureau of Standards, Journal of Research 83, 5-193 (1978)

30
[15] L.J. Fetters, N. Hadjichristidis, J.S. Linder, and J.W. Mays, Journal of Physical and

Chemical Reference Data 23^ 619-640(1994)

[16] B. N. Taylor and C. E. Kuyatt, "Guidelines for Evaluating and Expressing the Uncertainty of NIST Measurement Results." NIST Technical Note 1297, January

1993, available from National Technical Information Service, Technology

Administration, U.S. Department of Commerce, Springfield, VA 22161

[17] Brookhaven Instrument Corp., "Instruction Manual for Laser Light Scattering

Goniometers," May 1984, Third Printing

[18] A.S. Wexler, Spectrochim. Acta 21, 1725-1742 (1965).

[19] M. Karas, F. Hillenkamp, Anal. Chem. 60, 2299-2301 (1988)

[20] K. Tanaka, H. Waki, Y. Ido, S. Akita, Y. Yoshido, T. Yoshido, Rapid Commun.

Mass Spectrom. 2, 151-153 (1988)

[21] F. Hillenkamp, M. Karas, R.C. Beavis, B.T. Chait, Anal. Chem. 63, 1193 (1991)

[22] U. Bahr, A. Deppe, M. Karas, F. Hillenkamp, U. Giessman, Anal. Chem. 64, 2866

(1992)

[23] G. Montaudo,M.S. Montaudo, C. Puglisi, F. Samperi, Rapid Commun. Mass

Spectrom. 9, 453-460 (1995)

[24] G. Montaudo, D. Garozzo, M.S. Montaudo, C. Puglisi, F. Samperi, Macromolecules

28,7983-7989(1995)

[25] P.O Danis, D. E. Karr, W.J. Simonsick, D.T. Wu, Macromolecules 28, 1229-1232

(1995)

[26] G. Montaudo, M.S. Montaudo, C. Puglisi, F. Samperi, Rapid Commun. Mass

Spectrom. 9, 1158-1163(1995)

[27] G. Montaudo, E. Scamporrino, D. Vitalini, P. Mineo, Rapid Commun. Mass

Spectrom. 10, 1551-1559 (1996)

[28] D.C. Schriemer, L. Li, Anal. Chem. 68, 2721-2725 (1996)

[29] M.W.F. Nielen, S. Malucha, Rapid Commun. Mass Spectrom. 11,1194-1204

(1997)

[30] H.Zhu, T. Yalcin, L. Li, J. Am. Soc. Mass Spectrom. 9, 275-2819 (1997).

31
[31] H.M. Burger, H.M. Muller, D. Seebach, K.O. Burnsen, M. Schar, H.M. Widmer,

Macromolecules 26, 4783 (1993).

[32] CM. Guttman, S.J. Wetzel, W.R. Blair, B.M. Fanconi, J.E. Girard, R.J. Goldschmidt, W.E. Wallace, and D.L. Vanderhart, Anal. Chem. 73, 1252-1262

(2001)

[33] R.J. Goldschmidt, S.J. Wetzel, W.R. Blair, CM. Guttman, J. Am. Soc. Mass

Spectrom. 11, 1095-1 106 (2000)

[34] J. Devore, R. Peck, "Statistics: The Exploration and Analysis of Data" Belmont,

California: Wadsworth Publishing Co., 1997.

[35] R. E. Kirl<, "Experimental Design: Procedures for the Behavioral Sciences" Pacific Grove, California: Brool<s/Cole Publishing Co., 1995.

32
Tables

Table 1: Source of Uncertainty for Light Scattering Measurements on SRM 2888

Contribution as Expanded Uncertainty Uncertainty [10^ g/mol ] Standard Deviation of Mean of Measurement 0.12 Solvent Index of Refraction 0.01

Effect of Small Molecule Impurties on dn/dc 0.13

Calibration of Refractometer 0.14

Differential Refractive Index 0.24 Wavelength of Liglnt 0 Rayleigh Ratio of Scattering Standard, benzene 0.42

Light Polarizers 0.03 Solvent Density 0.01 Solute Masses and Solvent Masses 0.06

Reflection Correction 0.01 Instrumental Misalignment 0.01 Refraction Correction 0.04 Anisotropy of Polymer in Solution 0.01 Cutoff of Virial Expansion 0.2 Solute Degradation 0

Square root of sum of squares 0.57

33
Table 2: Moments of MMD from interlaboratory Comparison using MALDI-ToF-MS

Mn (g/mol) Mw (g/mol) Mz (g/mol)

Total Mean 6610 6740 6860

Standard Deviation 120 110 100

Standard Uncertainty 11.8 10.5 10.1

34
Figures

FT-IR Spectrum of SRM 2888

o<

1700 1550 1400 1250 1 100 950 800

Frequency (cm- 1

)

Figure 1. The FT-IR spectrum of SRM 2888 (A), neopentyl benzene (C), and the

difference spectrum: SRM 2888 - SRM 1479 (B). Peaks identifying the tert-bu{y\

end groups are 1365 cm"\ 1393 cm"\ and 1475 cm"\

35
Mass Distribution of SRM 2888 by Mass Spectrometry

1350 -

2000 4000 6000 8000 10000

m/z

Figure 2. MALDI-TOF-MS MMD of Interlaboratory Comparison Polystyrene

(SRM 2888) using the specified recipe of retinoic acid and AgTFA.

36
Secondary Series in Mass Spectrum of SRM 2888

1400

1000 -

Figure 3. MALDI-TOF-MS MMD of PS expanded to show the secondary peak

series.

37
Distribution of Mass of SRM 2888

0.25

0.2 -

0.15 - o

c

o

o 0.1

CD

0.05 o

o

O

^ ON O o

o q

o

I

DQ CQ CD PQ DQ CQ CQ PQ CQ OQ OQ

Figure 4. Histogram of the distribution of the mean bins. The fraction of the MMD is given on the histogram as well.

38
Distribution of IVIn Reported in Interlaboratory Comparison

0.4

6000 6100 6200 6300 6400 6500 6600 6700 6800 6900

Mn

Figure 5. Histogram representing the distribution of Mn. The graphed

line represents the normal distribution for the data, and the outliers are seen at 6200 u.

39
Distribution of End Group Mass Reported in Interlaboratory Comparison

0.25

0.15

0.05

Figure 6. Distribution of the end group masses, which were calculated from

the maximum peak values. The end groups, which are hydrogen and tert- butyl, should have a mass of 58 u.

40
Appendices

Appendix I: Participating Laboratories In Interlaboratory Comparison

Botten, David S.; Lab Connections Inc. Carmen, Howard S.; Spectrometry Applications Research Laboratory

Goldschmidt, Robert; Polymers Division, NIST

Hanton, Scott D.; Air Products and Chemicals, Inc. Haverkamp, J.; Faculty of Chemistry, Utrect University, Bijvoet Center for Biomolecular

Research

Mehl, John; Hercules, David; Chemistry Department, Vanderbilt University

Jackson, Tony; Molecular Spectroscopy Team, ICI Technology

Ji, Hellen; Mays, Jimmy; Department of Chemistry, University of Alabama-Birmingham

Kowalski, Paul; Bruker Daltonics

Lattimer, Robert; BF Goodrich

Li, Liang; Department of Chemistry, University of Alberta McCarley, Tracy, Department of Chemistry, Louisiana State University

McEwen, Charles; Dupont Corporate Center for Analytical Sciences, Central Research & Development

Montaudo, Maurizio; Department of Chemistry, CNR-lnstitute for Chemistry and

Technology of Polymeric Materials Powell, Brian; Analytical Sciences Group -Spectroscopy, Zeneca Specialties

Price, Phillip C; Union Carbide Corp., Central Research and Development

Schmidt, M.; Maskos, Michael; University Mainz

Wallace, William; Polymers Division, NIST

Weidner, Steffen; BAM - Federal Institute for Material Research & Testing

Weil, David A.; 3 M Corporate Research Labs

Wetzel, Stephanie; Girard, James E.; Department of Chemistry, American University,

and Polymers Division, NIST

Wilkerson, Charles W. Jr.; Analytical Chemistry, Los Alamos National Laboratory

Wu, Kuang Jan; Analytical Research, Charles Evans & Associates

41
Appendix II: Uncertainty in PS Low Mw due to dn/dc Varying as a Function of Molecular Mass

Following Bushuk and Benoit for the variation of light scattering from a copolymer with varying composition we obtain by their eq 5 R = K X (dn/dc)2 Mi Ci (A1)

where (dn/dc)i is the refractive index change from molecule of mass Mi and

concentration Ci. If (dn/dc)i is independent of i we get

R = K (dn/dc)o^ X M, c, = K (dn/dc)o^ Mw Co (A2)

where Co = X Ci, the normal result for light scattering. Now for varying dn/dc with end

groups we assume

(dn/dc), = A + B/Mi (A3) With this functional form and eq A1 for the light scattering

R/K = A^ X Mi Ci + 2 A B X Ci + B^ X cMi (A4)

R/K = A^ Mw Co + 2 A B Co + B^ X Q/Mi (A5) But X Ci/Mi = Co/Mn (A6) so that R/K = A^ Mw Co + 2 A B Co + Blco/Mp (A7)

This an be rewritten as R/K = a2(Mw- Mn ) Co + Mn Co ( (dn/dc)ave f (A8)

where average dn/dc for the molecule is

(dn/dc)ave = A + B/ Mn (A9)

and difference between (dn/dc)ave and dn/dc for large molecular mass species is + B/Mn

Modifying eq (A8) one more step

42
R/K = A' (Mw - Mn ) Co - (Mw - Mn ) ( {dn/dc)ave )' Co + Mw ( (cln/clc)ave )' Co (A10)

The measured R/K gives an apparent Mw_app

R/K = Mw_app Co ((dn/dc)ave )' (M 1

From A1 1 and the above equations, we obtain

Mw-app = Mw + (Mw - Mn ) (A2/((dn/dc)ave)' " 1) (A12)

This is the final result. For SRM 2888: A = 0.108

(dn/dc)ave = 0.103 (Mw - Mn ) = 140 g/mol (from classical methods)

(Mw - Mn ) = 130 g/mol (from MALDI MS)

Taking the value 140 g/mol for (Mw - Mn) the last term on the right hand side of eq. (A12)

yields a value of 23 g/mol. This is then the estimate of the uncertainty arising from using an average (dn/dc) in the

light scattering equations, rather than a varying one.

References W. Bushuk, H. Benoit, Can Jour of Chem 36 (1958) pg 1616-26; also in 'Light Scattering from Dilute Polymer Solutions", ed Mclntyre and F. Gornick, Gordon and Breach (1964)

43
Appendix III: Estimation of (dn/dc) of a Small Amount of Cyclohexane in Toluene

Estimating the refractive index change upon mixing two organics liquids has been much

studied [1 ,2]. Most equations work well on solutions of organic liquids. The simplest

equation provided by Nelson [1] taking, as usual, £ = n^

ni2 = ni Vi + r\2 V2 where ni = the analyte refractive index

Vi = the analyte volume fraction n2 = the solvent refractive index

V2 = the solvent volume fraction ni2 = the refractive index of the mixture and

vi = Vi/ (Vi + V2

)

where Vj is the total volume of i with i =1 for analyte and 2 for solvent.

dni2/dvi = (ni - n2

)

but for a dilute solution of analyte in a solvent Ci = Vi*di/(Vi + V2) = vi di, where di is the density of the analyte.

Then dni2/dci = (ni - n2) /di For toluene as solvent and cyclohexane as analyte we obtain (ni-n2) = 1.4262-1.4969

di = 0.7785 g/mL

dni2/dci = -0.0707/0.7785 = -0.0908

[1] S.O. Nelson, IEEE Trans, on Elect. Insulation 26, 845-869 (1991)

[2] C.J.F. Bottcher, "Theorv of Electric Polarization", Elsevier Publishing Co.. 1952. Amsterdam

44
Appendix IV: Certificate of Analysis, SRM 2888

(See following pages.)

45
http ://ts . n i St. gov/ts/h td ocs/230/2 32/232. htm

Standard Reference Material® 2888

Polystyrene

(Mw, 7 190 g/mol)

This Standard Reference Material (SRM) is intended primarily for use in calibration and performance evaluation of

instruments used to determine the molar mass and molar mass distribution by size exclusion chromatography (SEC). A unit of SRM 2888 consists of approximately 0.3 g of polystyrene powder.

Certified Uncertainties: The certified measurement uncertainty is expressed as a combined expanded uncertainty with a coverage factor k 2, calculated in accordance with NIST procedure [2]. Type A and Type B contributions

to the expanded uncertainty of the measured mass-average molar mass include the uncertainties in Rayleigh ratio of

the scattering standard, optical alignment, and calibration of the differential refractometer. Expiration of Certification: The certification of SRM 2888 is valid, within the measurement uncertainties

specified, until 31 January 2010, provided that the SRM is handled in accordance with the storage instructions given in this certificate. This certification is nullified if the SRM is modified or contaminated. Maintenance of SRM Certification: NIST will monitor this SRM over the period of its certification. If substantive technical changes occur that affect the certification before expiration of this certificate, NIST will notify the purchaser. Return of the attached registration card will facilitate notification.

Technical coordination leading to certification of this SRM was provided by B.M. Fanconi of the NIST Polymers

Division.

Technical measurement and data interpretation were provided by CM. Guttman, W.R. Blair, B.M. Fanconi,

R.J. Goldschmidt, W.E. Wallace, S.J. Wetzel, and D.L. Vanderhart of the NIST Polymers Division.

Statistical consultation for this SRM was provided by S.D. Leigh of the NIST Statistical Engineering Division. The support aspects involved in the preparation, certification, and issuance of this SRM were coordinated through

the Standard Reference Materials Program by B.S. MacDonald of the NIST Measurement Services Division.

Certified Value

Mass-average molar mass (M^ ): 7.19x10' g/mol ± 0.57x10' g/moI Expressed as molar mass, previously expressed as weight average molecular weight [1],

Eric J. Amis, Chief Polymers Division

Gaithersburg, MD 20899

Certificate Issue Date: 09 May 2003

John Rumble, Jr., Chief Measurement Services Division

SRM 2888 Page 1 of 3
Storage: The SRM should be stored in the original bottle with the lid tightly closed under nonnal laboratory

conditions. Homogeneit> and Characterization: The homogeneity of SRM 2888 was tested by SEC analysis of solutions in tetrahydrofuran at 40 °C. The further characterization of this polymer is described in reference 3. Supplemental Information: The number-average molar mass (Mp) was determined by nuclear magnetic resonance (NMR) analysis of the end groups and found to be 6.96 x lO^g/mol with an estimated uncertainty of 0.40 x 10^ g/mol. Fourier transfonn infrared spectroscopy (FTIR) and matri.x-assisted laser desorption ionization time of flight mass spectrometry (MALDI-TOF-MS) were used to analyze end groups on the polymer. Only one set of end groups was found on the polymer. This polystyrene was also used in an interlaboratory comparison for the measurement of

molecular mass distribution by MALDI-TOF-MS. The MALDI-TOF-MS interlaboratory comparison yielded an Mn

of 6.61 X 10"' g/mol with a standard deviation of 0.12 x 10' g/mol and M,, of 6.74 x 10' g/mol with a standard

deviation of 0.1 1 x 10' g/mol. Twenty-three laboratories took part in this study [4]. A representative MALDI-TOF- MS spectrum of SRM 2888 is given in Figure 1. NIST Certification Method: The certified value for M,, was measured on SRM 2888 using static light scattering in toluene as solvent at 23 °C [3].

REFERENCES

[1] Taylor. B.N.; Guide for the Use of the Intenmtkmal System of Units (SI); NIST Special Publication 811, 1995

Ed. (April 1995).

[2] Guide fu the Expression of Uncertainty' in Measurement: ISBN 92-67-10188-9, 1st Ed. ISO; Geneva.

Switzerland, (1993); see also' Taylor, B.N.; Kuyatt, C.E.; Guidelines for Evaluating and Expressing the Uncertaint}- of NIST Measurement Resuhs\ NIST Technical Note 1297, U.S. Government Printing Office. Washington, DC (1994); available at http://phvsics.nist.gov/Pubs/. [3] Guttman, CM.; Blair,W.R.; Fanconi, B.M.; Goldschmidt. R.J.; Wallace. W.E.; Wetzel, S.J.; Vanderhart, D.L.;

Certification ofa Polystirene Synthetic Polymer, SRM2888; NIST Special Publication 260-152 (in press).

[4] Guttman, CM.; Wetzel, S.J.; Blair, W.R^; Fanconi, B.M.; Girard, J.E.; Goldschmidt, R.J.; Wallace, W.E.;

VanderHart, D.L.; NIST-Sponsored Interlaboratoiy Comparison of Polystyrene Molecular Mass Distribution Obtained bv Matrix-Assisted Laser Desorption/Ionization Time-of-Flight Mass Spectrometty: Statistical Analysis; Analytical Chemistry, Vol. 73, pp. 1252-1262 (2001).

Users of this SRM should ensiwe that the certificate in their possession is current. This can be accomplished by

contacting the SRM Program at: telephone (301) 975-6776: fax (301) 926-4751: e-mail srminfo@nist.gov: or via the Internet http://www. nist. sov/srm.

SRM 2888 Page 2 of 3
1350 -

-50 -1 - ^ " — 2000 4000 6000 8000 10000

m/z

Figure 1. Mass spectrum of SRM 2888 measured by matrix assisted laser desorption/ionization mass spectrometry. Retinoic acid was used as the matrix and silver trifluoroacetate as the catonization salt.

SRM 2888 Page 3 of 3