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1901 2012
Prize category:
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The Nobel Prize in Chemistry 1974
Paul J. Flory
Autobiography
I was born on
19 June, 1910, in Sterling, Illinois, of Huguenot-German
parentage, mine being the sixth generation native to America. My
father was Ezra Flory, a clergyman-educator; my mother, nee
Martha Brumbaugh, had been a schoolteacher. Both were descended
from generations of farmers in the New World. They were the first
of their families of record to have attended college.
My interest in science, and in chemistry in particular, was
kindled by a remarkable teacher, Carl W. Holl, Professor of
Chemistry at Manchester College, a liberal arts college in
Indiana, where I graduated in 1931. With his encouragement, I
entered the Graduate School of The Ohio State
University where my interests turned to physical chemistry.
Research for my dissertation was in the field of photochemistry
and spectroscopy. It was carried out under the guidance of the
late Professor Herrick L. Johnston whose boundless zeal for
scientific research made a lasting impression on his
students.
Upon completion of my Ph.D. in 1934, I joined the Central
Research Department of the DuPont Company. There it was my good
fortune to be assigned to the small group headed by Dr. Wallace
H. Carothers, inventor of nylon and neoprene, and a scientist of
extraordinary breadth and originality. It was through the
association with him that I first became interested in
exploration of the fundamentals of polymerization and polymeric
substances. His conviction that polymers are valid objects of
scientific inquiry proved contagious. The time was propitious,
for the hypothesis that polymers are in fact covalently linked
macromolecules had been established by the works of Staudinger
and of Carothers only a few years earlier.
A year after the untimely death of Carothers, in 1937, I joined
the Basic Science Research Laboratory of the University of Cincinnati
for a period of two years. With the outbreak of World War II and
the urgency of research and development on synthetic rubber,
supply of which was imperiled, I returned to industry, first at
the Esso (now Exxon) Laboratories of the Standard Oil Development
Company (1940-43) and later at the Research Laboratory of the
Goodyear Tire and Rubber Company (1943-48). Provision of
opportunities for continuation of basic research by these two
industrial laboratories to the limit that the severe pressures of
the times would allow, and their liberal policies on publication,
permitted continuation of the beginnings of a scientific career
which might otherwise have been stifled by the exigencies of
those difficult years.
In the Spring of 1948 it was my privilege to hold the George
Fisher Baker Non-Resident Lectureship in Chemistry at Cornell University.
The invitation on behalf of the Department of Chemistry had been
tendered by the late Professor Peter J.W. Debye, then
Chairman of that Department. The experience of this lectureship
and the stimulating asociations with the Cornell faculty led me
to accept, without hesitation, their offer of a professorship
commencing in the Autumn of 1948. There followed a most
productive and satisfying period of research and teaching
"Principles of Polymer Chemistry," published by the Cornell
University Press in 1953, was an outgrowth of the Baker
Lectures.
It was during the Baker Lectureship that I perceived a way to
treat the effect of excluded volume on the configuration of
polymer chains. I had long suspected that the effect would be
non-asymptotic with the length of the chain; that is, that the
perturbation of the configuration by the exclusion of one segment
of the chain from the space occupied by another would increase
without limit as the chain is lengthened. The treatment of the
effect by resort to a relatively simple "smoothed density" model
confirmed this expectation and provided an expression relating
the perturbation of the configuration to the chain length and the
effective volume of a chain segment. It became apparent that the
physical properties of dilute solutions of macromolecules could
not be properly treated and comprehended without taking account
of the perturbation of the macromolecule by these intramolecular
interactions. The hydrodynamic theories of dilute polymer
solutions developed a year or two earlier by Kirkwood and by
Debye were therefore reinterpreted in light of the excluded
volume effect. Agreement with a broad range of experimental
information on viscosities, diffusion coefficients and
sedimentation velocities was demonstrated soon thereafter.
Out of these developments came the formulation of the
hydrodynamic constant called theta, and the recognition of the
Theta point at which excluded volume interactions are
neutralized. Criteria for experimental identification of the
Theta point are easily applied. Ideal behavior of polymers,
natural and synthetic, under Theta conditions has subsequently
received abundant confirmation in many laboratories. These
findings are most gratifying. More importantly, they provide the
essential basis for rational interpretation of physical
measurements on dilute polymer solutions, and hence for the
quantitative characterization of macromolecules.
In 1957 my family and I moved to Pittsburgh where I undertook to
establish a broad program of basic research at the Mellon
Institute. The opportunity to achieve this objective having been
subsequently withdrawn, I accepted a professorship in the
Department of Chemistry at Stanford University in 1961. In 1966, I was
appointed to the J.G. Jackson - C.J. Wood Professorship in
Chemistry at Stanford.
The change in situation upon moving to Stanford afforded the
opportunity to recast my research efforts in new directions. Two
areas have dominated the interests of my co-workers and myself
since 1961. The one concerns the spatial configuration of chain
molecules and the treatment of their configuration-dependent
properties by rigorous mathematical methods; the other
constitutes a new approach to an old subject, namely, the
thermodynamics of solutions.
Our investigations in the former area have proceeded from
foundations laid by Professor M.V. Volkenstein and his
collaborators in the Soviet Union, and were supplemented by major
contributions of the late Professor Kazuo Nagai in Japan. Theory
and methods in their present state of development permit
realistic, quantitative correlations of the properties of chain
molecules with their chemical constitution and structure. They
have been applied to a wide variety of macromolecules, both
natural and synthetic, including polypeptides and polynucleotides
in the former category. The success of these efforts has been due
in no small measure to the outstanding students and research
fellows who have collaborated with me at Stanford during the past
thirteen years. A book entitled "Statistical Mechanics of Chain
Molecules", published in 1969, summarizes the development of the
theory and its applications up to that date.
Mrs. Flory, the former Emily Catherine Tabor, and I were married
in 1936. We have three children: Susan, wife of Professor George
S. Springer of the Department of Mechanical Engineering at the
University of
Michigan; Melinda, wife of Professor Donald E. Groom of the
Department of Physics at the University of Utah; and Dr. Paul John Flory,
Jr., currently a post-doctoral Research Associate at the Medical Nobel
Institute in Stockholm. We have four grandchildren: Elizabeth
Springer, Mary Springer, Susanna Groom and Jeremy Groom.
From Les Prix Nobel en 1974, Editor Wilhelm Odelberg, [Nobel Foundation], Stockholm, 1975
This autobiography/biography was written at the time of the award and later published in the book series Les Prix Nobel/Nobel Lectures. The information is sometimes updated with an addendum submitted by the Laureate.
Paul J. Flory died on September 8, 1985.
Copyright © The Nobel Foundation 1974
MLA style: "Paul J. Flory - Autobiography". Nobelprize.org. 24 May 2013 http://www.nobelprize.org/nobel_prizes/chemistry/laureates/1974/flory-autobio.html
