BIOCHEMICAL
Vol. 73, No. 2,1976
AND BIOPHYSICAL
Quasielastic Light Scattering Biopolymers. Conformation Chromatin Multimers*
Barbara Ramsay Shaw Department of Chemistry Duke University Durham, North Carolina
RESEARCH COMMUNICATIONS
by of
27706
and Kenneth S. Schmitz Department of Chemistry University of Missouri-Kansas Kansas City, Missouri 64110 Received
July
City
26,1976
Abstract Chicken erythrocyte chromatin was partially digested with micrococcal nuclease and separated into multimeric subunit fractions by gel permeation chromatography. The fractions were characterized by their Svedberg constant, diffusion coefficient, circular dichroism, and electrophoresis pattern of the extracted DNA. The molecular weight dependence of the sedimentation coefficient was found to be S M-554. $:'Hh: K:::w:od The molecular weight dependence of f/f, is best represented theory by either a helical superstructure or a flexible coil with attractive ThFdimer calculations of f/f, suggest that interactions between nucleosome units. theeparticles are separated by spacer regions which contribute up to -20% of the frictional properties of the molecule. Introduction Partial (5)
nuclease
and other
periodically et al.
eukaryotes organized
(6, along
( 9) independently
of the histones (10-14) core
digestion
suggests particles,
wrapped
around
"beads-on-a-string" * Supported Research
of chromatin 7) suggests the
proposed
from mammals (l-3),
that
chromatin
strand.
models
i.e., the
40-60
base pairs
a DNA-histone eight-histone structure
in part by grants Corporation.
the repeat
complex as observed
(9,
15,
by electron
from NSF (GP-25551
Copyright 0 1976 by Academic Press, Inc. All rights of reproduction in any form reserved.
lb),
224
and two each evidence
DNA serve
to link
base pairs
thereby
are
Chemical
unit.
-140
plants
and Van Holde
DNA strand
accessible
in which
(4),
regions (8)
a short
of nuclease
complex
resistant Kornberg
in which
H2A, H2B, H3 and H4 comprise that
nuclease
yeast
giving
microscopy
and BMS 73-06819
of DNA is rise
(17-20). A02)
and
to a
BIOCHEMICAL
Vol. 73, No. 2, 1976
We report
herein
mers on molecular were
used
employed
in the
Bloomfield lattices.
a helix
friction
the
random
flight
of nucleosomes
helix,
using
of our
with
theory
was used
and,
polymer
multi-
hydrodynamic f/f,
values
of Filson
tetrahedral that
obtaining
interactions
for
results
space,
methods
(S) coefficients
to compute
suggest
compact,
attractive
(27)
the
in a free
investigations is
of chromatin
and sedimentation
on a string
in solution
coil
properties
(D) and Svedberg
The Kirkwood
polygon,
RESEARCH COMMUNICATIONS
scattering
the diffusion
beads
The results
or flexible
light
analysis.
planar
(21),
structure
Quasielastic
functional
regular
of hydrodynamic
respectively,
between
rod,
gonal
weight.
to obtain,
interaction rigid
the dependence
AND BIOPHYSICAL
the
and and hexa-
supramolecular
conformations
between
core
for
of either
particles.
Experimental -The preparation viously
(11,
was carried cooling
and isolation
12).
Digestion
of the nuclei
out at 37°C and terminated
on ice.
The nuclei
were
in 10 ml of lOmM TrisaHCl, on a Virtis
minutes
and the
homogenizer.
column,
90 x 2.5 cm, equilibrated
supernatant
fraction
Sedimentation at 30,030 scattering gravity-flow throughout temperature tial
decay
operating
rpm.
where
D is
were
facility
into
the
collection similar
clip
the solution
at 12000xg
debris
obtained
scattering interval
function, mode,
gradient
with
decay
A-5m
light Samples
by circulating
a Saicor constant
5°C.
E ultracentrifuge
(22-24).
(23).
15
centrigugatior
by quasielastic
described
computed
for
to a Bio-Rad
at 5°C and temperature
was effected
has a homodyne
at 10,OOOxg
sucrose
described
previously
at medium
0.7mM EDTA, pH 7.5 at
determined
cells
resuspended
30 seconds
on a Beckman Model
were
(Worthington)
15 minutes,
and applied
by isopycnic
previously
to that
for
pre-
1OmM in EDTA and
was pelleted
1OmM Tris'HCl,
coefficients
autocorrelation
l/T
with
coefficients
the data
in the
Nuclear
described
nuclease
0.7mM EDTA and disrupted
purified
filtered
jacket
by making
was further
on the
were
by micrococcal
was made 7% in sucrose
Diffusion
methods
erythrocytes
centrifuged
pH 7.5,
setting
The dimer
of chicken
were
control ice
water
The single
in a
exponen-
43A autocorrelator l/r
given
by (25)
= 2D(4=n/h,)2sin2(0/2)
the d iffusion
coefficient,
(1.) n is
225
the
index
of refract
ion,
X, = 488 nm,
Vol. 73, No. 2,1976
BIOCHEMICAL
t Figure
least-squares
where
analysis
the
scattering
C(t)
of a single
K = (4m/Ag)sin(B/2)
and 0 is
Function
functions
C(t)
in the
present
exponential
decay
= A exp(-2DK2t) (cf.
angle.
of Chromatin
text
Multimers. study
with
were
analyzed
by
baseline,
+ B
for
definition).
A representative
(40 --<8<70) *
curve
is
given
in
1. Representation -The molecular
weight
was computed
M = (S/D)RT where for
(m,ll,seconds)
Autocorrelation
The autocorrelation
Data
RESEARCH COMMUNICATIONS
1 Representative
Figure
AND BIOPHYSICAL
S is the
in Svedbergs
chromatin
the two sets
the
Svedberg
equation,
x 10 -13/(l-;o)
(2)
and ;p = .68.
multimers
of data
from
A plot
and native
of In S vs In M is
DNA (26).
The empirical
given
in Figure
relationships
2
for
are
S = 0.011 20
M.554
(multimers)
S
M.Z80
(native
DNA)
of the
friction
(3)
and 20
The molecular Einstein
= 0.163 weight
dependence
(4) factor
ratio
f/f,,
using
the
relationship f = kT/D
(5)
226
Vol. 73, No. 2, 1976
Figure
BIOCHEMICAL
Weight
The molecular and sedimentation pH 7.5) lysine
rich
and Stoke's
nuclease
Chromatin
for
column
digested
Hl and H5).
were
computed
fractions
chicken
Multimers
(in
DNA values
(----I
s 20 = .Oll
M'554
(----)
S = .I63 20
Mm2"
and Native
from
chromatin were
DNA
the diffusion
1OmM Tris-
erythrocyte
The native
and Inman
0.7mM EDTA, (containing
reported
by Record,
(26).
equation
solvent
viscosity
expression f i,
the
of S20 for
of the multimers
coefficients
histones
n is the
theoretical
Dependence
weight
of partial
Woodbury
where
RESEARCH COMMUNICATIONS
2 Molecular
where
AND BIOPHYSICAL
and N is
of the Kirkwood
Avogadro's
theory
number,
was compared
with
the
(27)
nR = Rs(l+t
R is
a friction
bead
average
distance
between
C ) ij i#j radius, n is the number centers
of beads
227
of beads
i and j,
per
and Rs is
chain,
is 11 defined in Eq. (6)
Vol. 73, No. 2, 1976
Results
multimers
which
is
exhibit
a more compact
closely
represented
The three-dimensional
(28).
when
compared
parameters distance
are
involved
RESEARCH COMMUNICATIONS
Rs = 52;
ratio
f/f,
model
(B = 2R).
(cf.
= 1.85
radius,
apparent
inconsistency
particles
particle
ranging
"effective"
friction and spacer
20% of the
friction
was calculated of DNA in
models computed
region,
which
properties
using
of the
dimer
are presented from
values
and Bloomfield
contiguous
spheres.
in the
region
spacer
reported region,
represents
value the
an upper
in Table
I for
of u 12'
in units
(21)
and employed
n=l2.
( > f'fo = (L&4)(1 These values
(estimated
of the
limit.
region
of adjacent
coil
bead
equivalent R' = 62; The the
(RI-R)/R'). pairs
a core an
accounts
(12)
for
core for
up to
Since
62A
the length
to the frictional
Comparison
The random
from
in length.
20% contribution
between
we calculate
of both
of 40 base
core this
regions
of radius
from
bead
estimated
= 136;,
spacer
The
We interprete
contribution the
con-
contiguous
of spacer
of 112;
unknown
(S20 = 16.2).
estimates
beads
from
fraction,
The hydrodynamically
chains
that
dimer
dimer
of B at 236;,
friction
implies
inferred
a helical
18, 29-31).
friction
weights
several
for the
support
DNA
center-to-center
reported
of 40 x 3.4;
spacer the
is Since
from
15, 17,
the value
of the
the minimum
the erythrocyte
11,
evidence
frictionless represents
(7).
chromatin
molecular
of 5.3 x lo5
the
R' of R' = 62;.
bead
of native
of R = 73; in the
to "effective"
corresponds
by semiflexible
particle
properties
radius
that
diameter
weight
than
(9,
If we fix
bead
the
(i.e.,
estimated
a value
50-55:
of 50; and a spacer
therefore,
"effective"
yields
as physical
friction
first
the molecular
from
Eq.
and fiber
pitch,
is much larger
in solution.
radius
connected
value
than
that
rod at these
employing
R and B are
the dimer
This
conformation
the macrostructure
R, R,,
Eq. 6) for for
particle
dimer,
beads,
suggests
of the polynucleosomes
structures
in describing
the parameters
where
core
model
weight
as a rigid
conformation
with
B of adjacent
formation),
for
of S20 on molecular
dependence
(a = .554)
(a = .280),
f/f,
AND BIOPHYSICAL
and Discussion
The power
Filson
BIOCHEMICAL
of f/f,
calculations
separation,
for
several
were reported
by
in the equation, +(u12/2)) were converted
228
(8) to the
"spacer
region"
model
CONFORMATION
sphere
model
from
by using
The value n = 12 is an average number computed sample and the dimer weight of 5.3 x 105.
from the contiguous calculations).
2.446 2.459 2.330
and Bloomfield
(d)
by Filson
estimated (cf. rod
reported
(cl
from
calculated
(b)
study
present
12
12 12
--1.984 1.925 1.892
2.618
the
the
average
conversion
(21)
2.28
f/f,
molecular
factor
-+ .07
weight
3.8
(c) (c) (c)
of
: 3.0
3.057 3.074 2.913
(c)
(c)
the multimer
2 1.25
B = 236;
2.397 2.480 --2.365
3.4
3.8
R = 62;;;
FOR n = 12 BEADS
B = 148;;
3.019
R = 741;
MODEL COMPARISON OF f/f,
(a)
al2
lattice
Experimental (d) (M = 3.2 x 106)
Random Walk (b) Free Tetrahedral space Cubic lattice
12 12 12 12
Helix elements/turn elements/turn elements/turn elements/turn
Contact 5 6 5 4
(a) (b) (a) (b)
12
Polygon
Regular
(a)
12
n
Rod (a)
---____
-
TABLE I.
Vol. 73, No. 2, 7 976
by the
conversion
regular
polygon
factor
feature
conformations
in either
in which
with
the
with
experiment,
friction
helix
thereby
increasing
model,
which
agreement 5 x lo5
the
all
- 5 x 106
set
of parameters,
are
of the
attractive
flexible
coil
The molecular spacer
model
Assuming core
(19)
a core
we have a total partially This
5.7 x lo4
rich
histone
spacer
as the protein
regions.
weight per
"tails" weight
core
(5.3
helix bead,
out
particles
is
in good
weight
do not
for
yield rule
radius,
in the spacer
in the helical
pair
(the
x lo5
minimum
at each end since of -4.73
105.
x
difference since
Nonetheless
2 .25 x 105)
composition
of 2.10
to the presence
content
bead
range
are an outside
These
a decrease
between
friction
the
calculations
We cannot
as well
dalton
these
consistent
between
in the molecular
of -4.7".
values.
is not
as
distance
the friction
conformations
of the dimer
attributed
for
defined
can be made to coincide
can be compensated
weight
particle
pair
touch,
repre-
helix
constitute radius,
a which
by increasing
f/f,
values
the
possibility
the
higher
than that
causing
a slight
shrinkage
is
also
consistent
with
dimer
fraction
(32).
conformation.
DNA at 660 daltons
and 20 base
and
polygon
helix,
The contact
of f/f,
since
interactions
turns
to 2 times
radius
shielding,
experimental
of rod
to adequately
center-to-center
l-112
The random walk
ratio
or regular
contact
bead helix
the
used in
rod
models
the
helical
of inclination
in more hydrodynamic
the corresponding
that
to the solvent.
however,
of inclination.
or spacer
clear
between
The parameters
unique
there
also
values
to the
of the
The contiguous
experimental
limit
inability
bead
a more realistic
of 300A and an angle
angle
ths
in adjacent
exposure
RESEARCH COMMUNICATIONS
I).
by increasing
radius
results
is
to a value
employs
with
It
results.
turns
Table
I is
beads
however,
as a --lower
contiguous
data.
experimental
adjacent
(cf.
the
AND BIOPHYSICAL
obtained
of Table
the experimental
a helix
1.25,
conformations
A salient
sent
BIOCHEMICAL
and a minimum
80 base pairs
40 base pairs
for
these
are not
The remaining of lysine-rich
may be regarded
up to an additional these
of the
calculations
230
the spacer
limit-digest
-5.7 histones
as an upper 20 base
pairs
support
the
x lo4
of nonregion
samples daltons
can be
in the dimer limit
for
particle.
the
lysine-
DNA may be in the concept
that
(ll)),
lysine-
the
Vol. 73, No. 2, 1976
rich
histones
BIOCHEMICAL
are associated
with
AND BIOPHYSICAL
dimer
particles
RESEARCH COMMUNICATIONS
as postulated
(11,
32).
coefficient
on the
Conclusions 1) weight
The power
dependence
(a = . 554) suggests
of the sedimentation that
the supramolecular
structure
molecular
of the. nucleosomes
is
compact. 2) f/f,
Model
calculations
as a function
of molecular
polygon,
random
possible
conformations
3)
walk,
either
interactions 4)
Analysis regions
nucleosomes
Dr.
is
friction
interpreting
lysine-rich
(NSF GP-25551,
We are
indebted
(K.S.S.))
to Ms. Georgia
regular
(since
of
planar
f/f,+l)
as
that,
in low ionic polymer
by the chromatin f/f,
for
with
attractive
multimers.
the dimer
hydrodynamic
strength
suggests
properties
that
of poly-
histones.
K. E. Van Holde
Schurr
ratio
dependence
in our samples.
-or a flexible-coil obtained
the
rod,
structures
suggests
factor
in
to analyze
the rigid
spherical
herein
particles
are important
We thank
eliminates
conformation
core
theory
by polynucleosomes
presented
of the
containing
weight
obtained
a helical
between
the Kirkwood
and closest-packed
The calculations
solutions,
spacer
using
(NSF BMS 73-06819 for
Reidel
financial
support
and Ms. Leslie
A02,
(B.R.S.))
and Dr.
and use of their Lewis
for
technical
J. M.
facilities. assistance.
--References 1. 2. 3. 4. 5. 6. 7. 8. 9. 10. 11. 12. 13. 14. 15.
Rill, R. and Van Holde, K. E. (1973) J. Biol. Chem., 248, 1080-1083. Sahasrabuddhe, C. G. and Van Holde, K. E. (1974) J. Biol. Chem., 249, 152-156. Nell, M. (1974) Nature, 251, 249-251. Lohr, D. and Van Holde, K. E. (1975) Science, 188, 165-166. McGhee, J. D. and Engel, J. D. (1975) Nature, 254, 449-540. Gorovsky, M. A. and Keevert, J. B. (1975) Proc. Natl. Acad. Sci, 72, 3536-3540. Honde, B. M., Baillie, D. L., Candido, E. P. M. (1974) FEBS Letters, 48, 156-159 Kornberg, R. D. (1974) Science, 184, 868-871. Van Holde, K. E., Sahasrabuddhe, C. G. and Shaw, B. Ramsay (1974) Nucl. Acids Res. , 1, 1579-1586. Van Holde, K. E. and Isenberg, I. (1975) Accounts Chem. Res., 8, 327-335. Van Holde, K. E., Shaw, B. Ramsay, Lohr, D., Herman, T. M. and Kovacic, R. T. (1975) Proc. Tenth FEBS Meeting, 57-72. Shaw, B. Ramsay, Herman, T. M., Kovacic, R. T.. Beaudreau, G. S. and Van Holde, K. E. (1976) Proc. Natl. Acad. Sci. USA, 73, 505-509. Sollner-Webb, B. and Felsenfeld, G, (1975) Biochemistry 14, 2915-2920; Axel, R. (1975) Biochemistry 14, 2921-2925. Simpson, R. T. and Whitlock, Jr., J. P. (1976) Nucl. Acids Res., 3, 117-128. Pardon, J. F., Worcester, D. L., Wooley, J. C., Tatchell, K., Van Holde, K. E. and Richards, B. M. (1975) Nucl. Acids Res., 2, 2163-2176.
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Vol. 73, No. 2,1976
16. 17. 18. 19. 20. 21. 22. 23. 24. 25. 26. 27. 28. 29. 30. 31. 32.
BIOCHEMICAL
AND BIOPHYSICAL RESEARCH COMMUNICATIONS
Bram, S., Butler-Brown, G., Bradbury, E. M., Baldwin, J. P., Reiss, C. and Ibel, K. (1974) Biochimie, 56, 987-994. A. L. and Olins, D. E. (1974) Science, 183, 330-332. Olins, Woodcock, C. L. F. (1973) J. Cell Biol., 59, 737a. Van Holde, K. E., Sahasrabuddhe, C. G.. Shaw, B. Ramsay, Van Bruggen, E. F. J. and Arnberg, A. C. (1974) Biochem. Biophys. Res. Comm., 60, 1365-1370. Oudet, P., Gross-Bellard, M. and Chambon, P. (1975) Cell, 4, 281-300. Filson, D. P. and Bloomfield, V. A. (1967) Biochimica et Biophysical Acta, 155, 169-182. Schurr, J. M. and Schmitz, K. S. (1973) Biopolymers, 12, 1021-1045. Schmitz, K. S. and Schurr, J. M. (1973) Biopolymers, 12, 1543-1564. Lee, W. I. and Schurr, J. M. (1974) Biopolymers, 13, 903-908. Berne, B. J. and Pecora, R. (1974) Ann. Rev. Phys. Chem., 25, 233-254. Record, Jr., M. T., Woodbury, C. P. and Inman, R. B. (1975) Biopolymers, 14, 393-408. Kirkwood, J. G. (1954) J. Poly Sci., 12, l-14. 11, 2109-2124. Ding, D.-W. , Rill, R., and Van Holde, K. E. (1972) Biopolymers Carlson, R. D. and Olins, D. E. (1976) Nucl. Acids Res., 3, 89-100. Bram, S., Butler-Brown, G., Baudy, P. and Ibel, K. (1975) Proc. Natl. Acad. Sci. USA, 72, 1043-1045. Finch, J. T. and Klug, A. (1976) Proc. Natl. Acad. Sci. USA, 73, 1897-1901. Shaw, B. Ramsay, Herman, T. M., Kovacic, R. T., and Van Holde, K. E. (1976) in Molecular Mechanisms in the Control of Gene Expression, Ed. by I!. P. Nierlich & W. J. Rutter, Academic Press (in press)
232