BIOCHEMICAL
Vol.5, No.3,1961
AND BIOPHYSICAL
RESEARCH COMMUNICATIONS
DIFFUSION OF PROTEIN MOLECULES TRROLJGB HEMBRAN~ OF CONTROLLED PORE SIZE1 Eckhardt Fuchs of Chemistry, Stillwater,
Department
Received
May 22, 1961
Membrane sizes
have
teins
through
ison ing
protein
sions
; the
cules
which become
diffusion
separation that
membrane
sandwiched
definite
area
vals
tally. sizes
small and the
Experiments of 10,
New Bedford,
that
represented
to the
in Fig.
0.1
50 and 450-q
diameter,
rangsize
can
dimendiffusion.
of protein
volumes
protein
solution
as nearly
of protein three
When assembled,
Equal
portions
aliquot
1.
in the
ml.)
done with
and shape
cut
were
were
by free
A window
compartments
concentration
pore
molecular
volume,
A and B, respectively,
(ca.
their
of equal
solution.
and of 0.1-l%
of both
weight,
of appropriate
size
Compar-
apparatus.
attainable
the
of some pro-
molecular
with
pore
mole-
way.
two plates.
membrane
buffer
The contents
compartment,
simple
of two compartments between
in a simple
in accordance than
uniform
The diffusion
membranes
concerning
is
and nearly
of increasing
that
presumably
employed
in compartments
of time,
proteins
shows
in this
of the
of 0.02kJ phosphate
sible.
for
information
consists
definite
commercially.
is much sharper
may be obtained
cell
have
has been measured
to urease,
The apparatus
put
available
rates
molecules,
appears
fusion
supposedly
such membranes
lysozyme
sift
Thus it
filters
recently
of the from
and George Gorin Oklahoma State University Oklahoma
exposes
(usually buffer
were as pos-
At
appropriate
inter-
withdrawn
was determined of filter the
from
each
spectrophotometri-
membrane, Millipore
with Filter
pore Corp.,
Massachusetts.
“Work done under Contract of Naval Research.
Nonr-2595(02)
with
196
the
Biochemistry
a
8 ml.1
same time
were
from
by a filter
plates
in the
dif-
at the
stirred.
types
purchased
separated
the
Branch,
Office
Vol. 5, No. 3,, 1961
BIOCHEMICAL
AND BIOPHYSICAL
RESEARCH COMMUNICATIONS
cm. sq.
Fig.
1.
Partially
Diffusion struction In
cells,
which
necessary
phragm, given
similar
have been’used
these
first
cells
exploded diagram of apparatus. Cell lucite; A is 47-mm. filter membrane.
after
in principle
by other
which
by equation
the (1)
concentrations
in details
and discussed
sintered-glass
a state
(Gosting,
different
investigators
have a thick
to establish
though
is made of
of con-
by Gosting
(1956).
or alundum
diaphragm,
it
diffusion
in the
dia-
substance
in A and B are
of steady-state of diffusible
is
19561,
(1)
where
1 is the
concentration
time
elapsed
from
the
chosen
time,
g is
the
diffusion
at that
constant.
This
constant
accurately
known I), but
is best
starting
determined
can be related
to the 197
time,
coefficient, empirically characteristics
c
is
the
and fi is with
initial a’ cell
a substance of the
cell
of and
BIOCHEMICAL
Vol. 5, No. 3,1961 of
an idealized
of total (Gosting,
For
diaphragm.
crossection
AND BIOPHYSICAL a diaphragm
2 and length
RESEARCH COMMUNICATIONS
consisting
II, & is
given
of thin
by equation
straight
tubes
(21 (VA=
VB = V)
1956):
2a
e==
Owing
to the
of solution
thinness
and the
neglected, filled.
time
Equation
of the“Millipore”membrane,
time
and the
(1)
(2)
necessary interval
then
to attain
,0.0150
steady-state
can be determined
reduces
cm. * the
diffusion
from
the
time
amount’
can be the
cell
to (3):
$J _ 2cA _ - -$Dt
In
is
(3)
cl4
For
low values
of the
In (1 + x) 2’~
holds
fraction within
diffused, lU$,
and one obtains
‘A FA = -G
Thus
the
slope
initial
portion
proportional
to the
time
required
of the
to Q. for,
2 shows representative
seen
that
Table in duplicate
the results
I gives
(4):
_ ZfiDt 1
(4)
1% diffusion:
data
0.2 = -jE
obtained
are in qualitative
some numerical
or triplicate
expression
approximation
of F versus t should be linear and its A same token, D should be inversely proportional
T0.1
Fig.
the
plot
By the say,
FA =*CJCi,
(5)
with
450-w
agreement
data.
The values
experiments,
each with 198
membranes, with
equati.on
of To 1 were A a fresh filter
and it (3).
determined membrane,
is
Vol. 5, No.
BIOCHEMICAL
3, ‘1961
AND
BIOPHYSICAL
RESEARCH
COMMUNICATIONS
0. lI 5 Fig. 2.
I I 10 15 Time in hours
Diffusion (21 serum
through albumin;
I 20
450-w membranes: (11 urease; (31 ovalbumin; (4) lysozyme.
TABLE I VALUES OF To 1 WITH VARIOUS FILTER5 . in hours
T0.1 Substance
M. w.
-7 10
-
D -1 cm2 set
450~mp filter
50-nl)l filter
lo-nql filter
Lysozyme
14,000
10.0
2.5
3.5
4.4
Ovalbumin Serum albumin
45,000 69,000
7.3 6.8
3.9 6.6
5.5 18
7.9 oo+
480,000
3.4
10.2
oD*
-44
Urease
* < 1% in 24 hours
and found ters
to agree
are fairly
within
reproducible;
1%.
This
indicates
no attempt 199
the
was made,
characteristics in these
of
preliminary
the filex-
Vol. 5, No. 3, 1961
periments, (all
BIOCHEMICAL
to determine
filters
with high precision
were from one lot).
from the literature be exactly
(Edsall,
appropriate
for the present
Equation
1956); while used, their
(3) predicts
that
accuracy should suffice
is a rather
small fraction
but not an unreasonable
The important
free diffusion
of the protein
of the surface
crossectional
area available
protein,
like
This indicates
large enough to pass this
of nearly
serum albumin,
that
protein,
interesting
the same molecular
of D for these proteins
(6.25 cm2>
i.e.
are quite
they would do so at nearly
there are no pores in the membrane that 2 becomes
essentially
and, if
zero.
A
membranes.
between two proteins
allowed to diffuse
the same speed; however, the 10-w 200
out”
is passed in the
ovalbumin and serum albumin.
close,
in the denser
appears to be “sifted
to note the difference
weight,
with the membranes
for free diffusion,
is observed with urease and the 50-w
It is especially
h = 0.015 cm., V = 8 cm3);
l’ike lysozyme, To 1 inA be ascribed to a decrease in
by the 10-w membrane; only a very small amount of protein
effect
From the
molecule,
creases by a small amount, which might reasonably
course of 24 hours.
manner.
exposed to diffusion
are those obtained
to be noted
For a small protein
But a larger
(2);
molecules
value.
results
pore size.
“normal”
0.4 cm2 (equation
24
cmS2), not in
However, the agreement is
these membranes in a nearly
values of 1 one can calculate
similar
the values may not
from 2.5 to 4.5 (X 10e6 X l/3600
agreement with the prediction.
takes place through
filters.
in the Table are taken
that the product TO 1D should be constant for mem& Actually, the experimental data obtained with 450-q
good to indicate
4, the effective
of & values
purpose.
good quantitative
of smaller
the repeatibility
1952; Gosting,
membranes give values ranging
sufficiently
RESEARCH COMMUNICATIONS
The values of & listed
for the conditions
branes of the same type.
this
AND BIOPHYSICAL
The values freely,
%illipore”
mem-
BIOCHEMICAL
Vol. 5, No. 3,1961
separates
brane
them sharply.
by no means certain
AND BIOPHYSICAL
It has been suggested (Low, 19521, though it
(Loeb and Scheraga,
albumin molecule might be a prolate and it
is easy to visualize
the membrane. geometric
inter
known particle
alia,
size,
The results
19601.
interactions
these matters;
of polystyrene
“mesh size.”
indicate
it to be a large mole-
weight reported
of molecular
(Sumner -*et al I 1936 ;
through
some dif-
of this
The present
molecular
results
weight would
50- and even lo-rnp membranes, contrary illustrates
of an
to what has been
how diffusion
experiments
may be utilized
to advantage for purposes other than the direct
determination
of molecular
observed.
This result
weight 17,000.
particles
of
to “calibrate”
Several years ago, Hand (1939) reported
subunit
it
latices
on the basis of which he suggested the existence
active
readily
on a
play a part in the diffusion
with respect to their
are not in accord with ‘that report: diffuse
specific
by means of which it might be possible
experiments,
enzymatically
doubtless,
with urease clearly
from passing
of molecules
in progress to clarify
in accordance with the molecular
fusion
sifting
to measure the diffusion
obtained
Creeth and Nichol,
that
involved;
are currently
the membranes empirically
cule,
with a major axis 150 61 long,
and the membrane material
Experiments
is planned,
ellipsoid
is
19571 that the serum
how such a molecule would be prevented
basis is the only effect
process.
1956; Tanford,
It would be naive to believe
between the molecules
RESEARCH COMMUNICATIONS
size and shape.
The work described Craig and co-workers We believe
19601. easily
operated
straightforwardly tage,
bears a close relationship
with dialysis the apparatus
in a precisely related
found it
necessary’to
junction
with proteins
“stretch-
(Goldstein
used in this controlled
to the
however, is the larger
tubing
diffusion
to that recently and Craig,
manner, and the results equations.
tubing
above ca. 30,000 molecular 201
1960; Craig,
work had some advantages;
advan-
whereas Craig et al.
before utilizing weight,
it is
can be,
The principal
range of pore sizes available; dialysis
done by
it
in con-
there is no upper
Vol. 5, No. 3,196l
limit
BIOCHEMICAL
AND BIOPHYSICAL
to the range of the filter
not all desirable
intermediate
RESEARCH COMMUNICATIONS
membranes commercially
available
(even though
sizes may be available).
REFEEENCB Methods of Protein Chemistry” (Alexander, P., L. C., in “Analytical B. J,, eds.1 Vol. I, p; 104-119, Pergamon Press, New York,
Craig,
and Block, (1960).
Creeth,
J. M., and Nichol,
C. W., Biochem. J.,
77, 230 (1960).
Edsall, J. T., in “The Proteins” (Neurath, il., and Bailey, p. 634-9, Academic Press, New York, (19531. Goldstein, Gosting,
J.,
and Craig,
I... J.,
L. C., J. Am. Chem. Sot.,
Adv. Protein
P. .B.,
J. Am. Chem. Sot.,
Loeb,
G. I.,
and Scheraga, H. A.,
Low, B. W., J. Am. Chem. Sot.,
61,
74,
3180
I,
82, 1833 (19601.
(1939).
J. Phys. Chem., 60, 1633 (19561. 4830
(1952).
N., and Eriksaon-Quensel,
(1938).
Tanford,
eds.1 Vol.
Chem., 11, 429 (19561.
Hand,
Sumner, J. B., Gralen,
K.,
C., J. Phys. Chem., 61,
1023 (1957).
202
I.,
J. Biol.
Chem., 125, 37