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Transcript
Eur. J . Biochem. 128. 565-575 (1982)
.?, FEBS 1982
Structural Prediction of Membrane-Bound Proteins
Patrick ARGOS, J . K. Mohana RAO. and Paul A. HARGRAVE
Department of Biological Sciences, Purdue University, West Lafayette. Indiana; and
School of Medicine and Departmcnt of Chemistry and Biochemistry, Southern Illinois University at Carbondale
(Received April 1Y :July 6, 1982)
A prediction algorithm based on physical characteristis of the twenty amino acids and refined by comparison
to the proposed bacteriorhodopsin structure was devised to delineate likely membrane-buried regions in the
primary sequences of proteins known to interact with the lipid bilayer. Application of the method to the sequence
of the carboxyl terminal one-third of bovine rhodopsin predicted a membrane-buried helical hairpin structure.
With the use of lipid-buried segments in bacteriorhodopsin as well as regions predicted by the algorithm in other
membrane-bound proteins, a hierarchical ranking of the twenty amino acids in their preferences to be in lipid
contact was calculated. A helical wheel analysis of the predicted regions suggests which helical faces are within
the protein interior and which are in contact with the lipid bilayer.
X-ray diffraction studies of crystalline soluble proteins
have resulted in nearly one-hundred known tertiary structures
[l, 21. With their advent have come many secondary-structure
prediction methods which require only a knowledge of the
amino acid sequence (cf. 13 - 51). These techniques generally
rely on a statistical or informational analysis of the frequency
with which the 20 amino acids appear within the observed
secondary structures (a-helices, p-strands, and reverse turns).
Since their data base is composed of only soluble protein
structures, the prediction algorithms may not be applicable
to primary sequences of proteins that are in contact with a
membrane. The only membrane-bound polypeptide topology
known to a reasonably high resolution has been determined
by electron-scattering techniques for the purple-membrane
protein of Halobacterium halobium [6,7] whose seven rods
of electron density are believed to be a-helical segments that
traverse the membrane [8]. Such a structure should be predictable from the amino acid sequence alone through utilization of the physico-chemical characteristics of the residues
interacting with the uniquely apolar membrane environment.
A prediction algorithm based on the physical characters was
developed in the present work and refined by application to
the bacteriorhodopsin primary structure. The correlation
between the predicted helical and turn regions and those of
the model structure suggested by Engelman et al. [8] was 0.69,
a value at least comparable to the prediction accuracy of
techniques devised for soluble proteins [5,9,10]. The prediction method was then applied to the known C-terminal
sequence of bovine rhodopsin and to the primary sequences
of other membrane-bound proteins. Two turn segments and
two helical regions were predicted for bovine rhodopsin.
The algorithm clearly delineated likely membrane-bound
regions within the amino acid sequence of the other proteins.
A hierarchical ranking of the twenty amino acids in their
preference to membrane buried was then determined. A helical
‘wheel’ analysis of the predicted regions indicated the helical
faces within the protein interior and in contact with the lipid
bilayer.
Etqwes. Adcnosinetriphosphatase (EC 3.6.1.3). superoxide dismutase (EC 1.15.1.1); lysozyme (EC 3 2.1.17); ribonuclease (EC 3.1 27 5);
adenylate kinase (EC 2.7.4.3).
MATERIALS AND METHODS
The physical parameters used to characterize the twenty
amino acids include: (1) the hydrophobicity index measured
by Nozaki and Tanford [ll], (2) the free energy of transfer
calculated by Janin [12], (3) the residue ‘surrounding’ hydrophobicity statistically determined by Manavalan and Ponnuswamy [13], (4) the experimental hydration potential of Wolfenden et al. [14], (5) estimated standard free energies of
transfer for a given residue type in a helix in water to a helix
in a non-polar phase [15], (6) the conformational propensity
parameters for reverse turn configurations as calculated by
Levitt [16], (7) residue bulkiness and (8) polarity listed by
Jones [17], and (9) helical conformational preference values
determined in the present investigation from the putative
buried helical regions in signal sequences. The hydrophobicity
measures 1-5 were all made positive and the characteristics
were normalized to a value of 1.0. All the parameters are
listed in their normalized and scaled form in Table 1 .
The physical characteristics were selected as likely candidates to discern the membrane-buried segments of proteins
except for the turn potential which would point to the exposed
peptide spans connecting the secondary structure in lipid
contact. Sequence spans with high hydrophobicity, bulkiness,
and membrane-buried helical potential as well as low polarity
and turn preference would be expected for regions interacting
with the uniquely apolar membrane. Various hydrophobicity
measures were utilized as there were no a priori means to
judge their sensitivity and ability to select membrane-bound
segments.
Parameters 1 - 5 attempt to quantify the hydrophobic
character of the twenty amino acids through empirical investigations or statistical analyses of the exterior and interior positions of residues as they appear in known protein structures.
Wolfenden et al. [I41 do not list the hydration potentials for
glycine and arginine. These potentials were assigned according
to the method of Moews et al. [18] who proportioned the
residue hydration states to their degree of buriedness in
soluble proteins as determined by Chothia [19].
Characteristic 9 is a buried helical conformational measure
similar to the Chou-Fasman preference parameters for helices
566
Table 1. Scaled and norinaliied physical paramuiers for the twenty amino acids
The parameters are nuinbered according to the scheme given in the text. References for the parameters are also given In thc text
Amino
acid
(1) Hydrophobicity
index
(2) Free
energy
of transfer
(3) Surrounding
Hydrophobicity
(4) Hydration
potential
(5) Burried
transfer
free
energy
(6) Turn
preference
(7) Bulk
(8) Polarity
(9) Slgnal sequence
helical potential
Ah
cys
0.61
1.07
0.46
0.47
2.02
0.07
0.61
2.22
1.15
1.53
1.18
0.06
1.95
0.00
0.60
0.05
0.05
1.32
2.65
1.88
1.24
1.60
0.71
0.65
1.36
1.24
1.01
1.48
0.00
1.36
1.30
0.77
0.89
0.65
0.24
1.01
0.95
1.42
0.24
0.83
1.01
1.14
0.84
0.92
1.09
0.97
0.94
1.22
0.88
1.16
1.12
0.89
0.88
0.91
0.91
0.87
0.91
1.22
1 .ox
1.04
2.00
0.50
0.40
2.28
1.96
0.00
0.72
1.44
0.19
1.60
0.21
0.15
1.33
1.42
1.23
3.10
1.03
0.91
0.29
0.29
0.95
0.82
0.84
1.48
1.05
0.61
1.73
0.73
0.54
1.01
0.62
0.41
1.35
2.01
1.02
0.93
1.40
1.08
0.49
0.79
1.11
0.75
0.88
0.76
0.88
1.29
0.22
0.89
1.39
1.02
1.39
1.06
0.83
1.13
0.94
0.93
0.62
1.03
1.40
1.41
1.17
0.97
0.66
I .56
1.48
0.62
1.08
1.25
0.62
1.36
0.59
0.68
1.39
0.96
1.26
1.26
1.10
1.03
0.71
0.65
0.74
1.81
1.89
0.05
0.11
1.96
0.49
0.3 1
1.45
0.06
3.23
2.67
0.23
0.76
0.72
0.20
0.97
0.84
1.08
0.77
0.39
ASP
Glu
Phe
GlY
His
Ile
Lys
Leu
Met
A sn
Pro
Gln
Arg
Ser
Thr
Val
Trp
TYr
1.51
0.01
0.13
1.58
2.07
0.12
2.03
0.23
2.06
1.47
0.20
0.93
0.25
0.00
0.92
0.94
2.00
0.79
0.75
in soluble proteins [20,21]. It is defined as the ratio of the
fractional occurrence of an amino acid within the putative
helical regions in signal sequences to its fractional occurrence
in known protein structures [16,22]. A 705-residue data base
compiled from signal sequences [I 5,231 was used to determine
the preference parameter.
Plots of the amino acid sequence number versus a given
parametric value for a particular amino acid in a primary
sequence were calculated. The curves were then ‘smoothed’
through several cycles according to the methodology of Rose
and Siddhartha [24] who determine a least-squares line for all
successive seven-point groups to calculate points for the
smoothened graph. The plots for the nine parameters were
then scaled such that their average value was 0.0 and their
standard deviations from the zero line were the same.
A plot resulting from an additive combination of the
various parameters appropriately weighted was then calculated to give the best prediction of the bacteriorhodopsin
structure as determined by Engelman et al. [8]. Amino acids
with a sequence number corresponding to a combined parametric value greater than zero were considered to be in a helical
conformation while those below zero were assigned as turn
residues. The weighting factors for each of the characteristics
in the combined graph were determined by a linear leastsquares procedure. A hypothetical curve corresponding to
the Engelman bacteriorhodopsin structure was devised such
that trigonometric sine curves were fitted to each of the seven
helical regions and eight turn spans; that is, the hypothetical
value Pi for the ith amino acid in the sequence and the kth
helix or turn region is given by
Pi= Fksin (2jii),
0 <.hi5 112
(1)
is + 1.O for helical spans and - 1.O for turns, fk is
where Fk
the appropriate scale factor for the kth secondary structural
region, and i is the amino acid number of the particular bacteriorhodopsin residue. The weighting factors Wl for each of
the I characteristic values (Cl) were then determined by linear
least squares from the equation
9
C Wi C1.i = Pi, i = 1, N
I= I
(2)
where N is the total number of amino acids in bacteriorhodopsin. The correlation coefficient (CF) used to measure
the agreement between prediction and observation is defined
by Matthews [25] as
where w is the number of residues predicted and observed
helical, x is the number predicted and observed in the turn
configuration, y is the number predicted nonhelical and
observed helical, and z is the number predicted helical and
observed nonhelical.
Concern regarding the fact that the model of Engelman
et al. [8] is not fully established by experiment is allayed by
the reasonableness of the model and its basis in empirical
studies. The structural model does represent the best fit of the
Henderson and Unwin electron density [6] and the Khorana
et al. amino acid sequence [26]. A recent refinement of the
projected bacteriorhodopsin electron density to 3.7 A resolution [27] confirms the Henderson and Unwin results even
to the extent of a density region that can possibly be assigned
to the lysine-retinal attachment site in the C-terminal helix.
Furthermore, the helices were conservatively placed which
would be advantageous for the prediction algorithm.
In the present work the bacteriorhodopsin model served
primarily to select the best paramelers and refine their weighting factors. This was tested by calculating a plot based on all
nine characteristics with unit weights of appropriate sign. The
plot was essentially the same as that resulting from model
refinement with the exceptions of the peak for the fourth helix
which was not as high (vide infiu) and the correlation with the
567
proposed structure which was 0.60 instead of0.69 after refinement. The unit weight approach also gave curves for the other
proteins tested similar to those resulting from the refined
weighting factors. The ability of the prediction method to
detect membrane-buried segments is thus more a consequence of the physical parameters selected rather than the
bacteriorhodopsin model structure.
Cross-correlation coefficients were determined for various
pairs of the physical parameters. If the twenty-component
series for two physical characteristics are respectively designated by [si] and [vi], then their cross correlation (CCF)
becomes
energy) followed by two cycles of smoothing yielded a predicted correlation of 0.50 relative to the modcl structure
derived from electron scattering data [6,7]. The combined
graph correlated better with the observed structure than any
of the individual plots. However, the additive hydrophobic
function was unable to distinguish helices F and G and predicted them as one long helix. Bulk and the buried helical
preference parameter also correlated positively with the model
helical segments while polarity and the turn potential showed
an inverse relationship. A combined graph of the four nonhydrophobic parameters with appropriate sign reversals for
polarity and turn preferences showed a correlation of 0.49
with the model structure: however, the D helix was completcly
20
20
,.i =z1. (Xi- 2 ) ..=
.z,-0 . i - j)
missed in the prediction (Fig. 1). The weak D helix response
C C F = - - __ - - _ _
can
be explained by the large number of glycine residues with(4)
1 2
in the helix. The glycine turn potential is strong [I61 and its
z
(Xi - iy (yi-?;)2]
i*O
=l
bulk is minimal [17].
where .Y and 7 are the respective average values for the two
Weighting factors for all nine parameters were then deterphysical parameters.
mined using the least-squares procedure based on the hypoNormalized Chou-Fasman preference parameters (PM) thetical trigonometric curve derived from the model structure.
are calculated for the twenty amino acids to indicate their The value of Fk was chosen as 1 .O (Eqn 1). The resulting curve
likelihood to be within a membrane. They are defined as
predicted well all the helical and turn segments except the
D helix and adjacent turn spans and the turn segment between
helices F and G. In the hypothetical curve these latter regions
were given F k values of 2.0 to 8.0 in integral steps with weighting factors and prediction correlation coefficients (Eqn 3)
calculated at each step. It was clear from the correlations
where NMqiis the number of times the ith amino acid type with the model bacteriorhodopsin structure as well as from
appears within primary sequences predicted to be membrane visual inspection that Fk = 4.0 provided the best curve. Four
buried and Ns. i is the number of times the ith amino acid type of the nine weighting factors had values near zero or a sign
appears within sequences of soluble proteins. The denomina- opposite from that expected. The hydration potential, turn
tor which is the fractional occurrence of a residue within the propensity, polarity, buried transfer free energy, and bulk
soluble protein data base normalizes the P M values [20,21].
had respective weights of 2.42, - 1.68, - 0.76, - 0.73 and
0.52. The ratio of contributions (hydrophobic to non-hydrophobic) to the final plot showed a ratio of 1.08. The weighted
physical parameters are listed in Table 2.
RESULTS AND DISCUSSION
The selection of the hydration potential and the buried
Bacturiorliodopsin
transfer free energy as the best hydrophobicity measures for
membrane-buried amino acids would be expected. Nozaki
The 248-residue primary structure of bacteriorhodopsin
determined by Khorana et al. [26] was used in the present and Tanford [ l l ] compared empirically the hydration states
investigation. The seven helices of the model structure are of isolated residues in an aqueous environment or in solutions
sequentially labelled A-G from the N to the C termini, containing ethanol or dioxane which are questionable in
following the pattern designated by Engelman et al. [8]. Appli- their ability to mimic the lipid bilayer environment. The surcation of the refined prediction method to the sequence is rounding hydrophobicities of Manavalan and Ponnuswamy
shown in Fig.1 and was developed as described below. The [13] were calculated by averaging the Nozdki-Tanford values
algorithm essentially consists of the addition of several physi- for residues surrounding a given amino acid type within
cal characteristics (e.g. hydrophobicity) for each amino acid known soluble protein structures which again are unlikely
within the sequence. A plot of the additive function versus to reproduce the membrane environment given their interior
sequence number results in maxima and minima indicating hydrogen bonds. Similarly the Janin transfer free energies [12]
respectively helical and turn regions in the bacteriorhodopsin were determined through the buried/accessible surface area
ratios of amino acids in known soluble tertiary structures. The
structure.
Plots of the bacteriorhodopsin sequence number versus Wolfenden values [14] result from measured vapor-water
the residue characteristic value were determined for each of partition coefficients for model compounds identical to each
the nine physical parameters (Fig. 1); three cycles of smooth- of the amino acids. The buried free energies [15] are estimates
ing were performed. Each of the graphs was then standardized for transfer of residues originally in a helix in water to a helix
to a zero parametric value. It was observed that positive peaks in a non-polar phase lacking hydrogen-bonding capacity.
Fig. 2 displays the weighted five-parameter plot for bacin the graphs for the all hydrophobic parameters except for the
buried transfer free energy correlated with the helical regions teriorhodopsin; two cycles of smoothing were used after the
in the Engelman model of bacteriorhodopsin while the nega- weighted combination of the already smoothed graphs for
tive troughs corresponded to the turn regions between the the five parameters. The additive function clearly resulted in a
buried helical segments (Fig. 1). The phase was opposite for superior correlation (0.69) with the model structure than
the buried transfer free energy. These results would be expected did any of the individual parameters. Helices F and G were
given the membrane environment of the helices. A graph distinguishable and the D helix region was delineated by a
resulting from the addition of the five hydrophobic curves positive peak value (Fig. 2). If the combined parametric value
(with appropriate sign change for the buried transfer free for a particular amino acid was greater than or equal to zero,
I
568
-1.m
j
0.0
w.0
Im.ogRtTRIdO.O
1
m.0
m.0
-1
.om
0.0
im.agRCTRiw.o
QO.O
m.0
.sm
.sm
2
w.0
g
.m
+
.om
-.cm
- .sm
.m
z>
LL
w
.om
E
+
m
e
- .sm
-1
.om
-.m
.om
0.0
w.0
m . 0BRCTR 160.0
mO.0
W.0
Fig. 1. Plot o / ’ / h p amino arid sequrnw numher.for bacteriorhodopsin (BACTR) versus various umino acid physical parurne/ers discussed in /At /c.y/. The
solid lines have undcrgone three cycles of smoothing. The dashed line rfers lo the helical (positive peaks) and turn (negative troughs) regions of the
bacteriorhodopsin model structure. Abbreviations as well as the text numbering scheme used for the physical characteristics are (1) HFBNT,
hydrophobicity index [ l l ] ; (2) HFBJN, free energy of transfer [12]; (3) HFBMP, surrounding hydrophobicity [13]; (4) HDPTL. hydration potential
[14]; ( 5 ) BTRFE, buried transfer free energy [IS]; (6) TURN, Chou-Fasman turn conformational prcference parameter [ l h ] ; (7) BULK, bulk
parameter [17]; (8) PLRTY, polarity [17]; (9) HELBR, membrane-buried helical potential dctermined from signal sequences (Table 1): and HELCF.
Chou-Fasman helical conformational preference parameter [16]
569
Table 2. Tlwfiiv ireiglitcd ptiysical parumeters that provided thc htTsI pretlii'tion (!/ tht) Iielical .socoriclarv sirucrurnl regions in hactcriorl~oclopsin
The parameters are numbered according to the scheme given in the text
Amino
acid
Ala
cys
ASP
Glu
Phe
GlY
His
Ile
Lys
Leu
Met
Asn
Pro
GI I1
Arg
Ser
Thr
Val
TrP
Tyr
(4)
Hydration
potential
(5)
Buried
transfer
free
energy
(6)
Turn
preference
(7)
Bulk
4.84
3.65
0.02
0.31
3.82
5.01
0.29
4.91
0.56
4.w
3.56
0.48
2.25
0.61
0.00
2.23
2.27
3.84
-0.36
- 0.29
- 1.66
- 1.43
-0.00
-0.53
- 1.05
-0.14
-1.17
-0.15
- 0.11
-0.97
- 1.04
- 0.90
- 2.26
-0.75
-0.66
-0.21
-0.21
-0.69
- 1.38
- 1.41
- 2.49
- 1.76
- 1.03
0.39
0.46
0.40
0.46
0.67
0.11
0.46
0.71
0.53
0.71
0.55
0.43
0.59
0.49
0.48
0.32
0.54
0.73
0.73
0.51
1.91
I .82
-2.91
- 1.23
-0.91
- 1.70
-1.04
-0.69
- 2.27
- 3.38
- 1.71
- 1.56
-2.35
- 1.81
-0.82
- 1.33
- 1.86
(8)
Polarity
Helical
designation
- 0.74
- 0.50
- 1.19
- 1.12
- 0.47
- 0.82
- 0.95
- 0.47
- 1.03
- 0.45
0.52
- 1.06
- 0.73
- 0.96
- 0.96
- 0.84
- 0.78
0.54
- 0.49
- 0.56
~
~
2.0
1.o
Table 3. Trunsmemhrane helicc~s41' haetc~ric~rliodupsiti
The primary structure used is that of Khorana et al. (261. The predicted
helices arc those determined from the prediction method discussed in
the present work while the model hclices are those proposed by Engelinan et al. [8]
n
x
VJ
3
0.0
+
x
@=
W
a
x
e-1.o
I-x
Predicted
helices
Model
helices
11- 29
45- 66
88- 99
105- 127
134- 156
174-192
200 - 225
8 - 31
41- 64
78- 101
107-130
133- I57
167-191
1 YX - 224
Some researchers (cf. [23,28,29]) have utilized the ChouFasman conformational propensity parameters calculated
from soluble protein structures to predict the sccondary structure of proteins that are at least partially membrane-bound.
It is noteworthy that the Chou-Fasman helical parameter [16]
resulted in a correlation of 0.01 between the predicted and
model bacteriorhodopsin structures while the helical propensities determined from signal sequences were able to locate
five of the seven helices in bacteriorhodopsin, yielding a
correlation accuracy of 0.35 (Fig. 1). Use of thc Chou-Fasman S-strand preferences [I61 showed a correlation of 0.48.
This would be expected as the hydration potential plays a
significant role in predicting the bacteriorhodopsin helices
and the ,4-strand parameters and hydration potential show a
CCF value of 0.46 (Eqn 4). The helical preference display a
near random cross correlation of - 0.10 with the hydration
potential. The conformational preference parameter calculated from the putative helices in signal sequences cross correlates with the P-preference values and the hydration potentials as 0.32 and 0.76 respectively. These results would suggest
that erroneous secondary structure predictions based on the
soluble protein preferences would be expected for primary
structural regions that exist within membranes.
-2.0
Bovine Rliodopsin
-3.0
Fig. 2. P h of' Ihc amino acid sequence numher j u r hrirteriorl~odupsin[26]
wrsus a wc~ightrrljive-purumeter characteristic value jor a given amino
(rcid. Thc termini of predicted helices were dcterrnined by the intersec-
tion points of the positive peaks with the zero line. Turn regions were
similarly dclineated at the trough intersection points. Helical segments
determincd from the electron scattering data 16-81 are shown as black
bars and labelled A - G according to Engelman et al. [8]. The parametric
value is shown as zero at each of the seven terminal residues due to thc
end-effects of the least-squares 'smoothing' procedures [24]
the residue was assigned as helical; the turn regions were
indicated by parametric values less than zero. Table 3 lists
the predicted and observed helical regions. The combined
approach predicted correctly 82 "/, of the helical residues and
89"; of the turn regions. The missed predictions at the N-termini of helices C and F are primarily caused by the appearance
of charged amino acids.
The weighted .five-parameter algorithm was applied to
the 108 residues in the bovine rhodopsin C-terminal sequence
[30-321 where the amino acid at the C-terminus is designated
1'. Two helices separated by a turn region and a long C-terminal turn span were clearly delineated (Fig. 3). Helix 1 at the
C-terminus is comprised of residues 43' to 66' while helix 2
rangcs from 73' to 97'. Since the rise per residue in an ?-helix
is near 1.5 A, a 25-residue stretch can traverse about 35 A, a
typical membrane width. It is also striking that the C-terminal
helices in both the bacterial and bovine rhodopsins are
characterized by a two-prong peak with their minima corresponding to lysine residues known to be retinal attachment
sites for both proteins [33,34]. Replacement of the lysine by
a leucine did not alter the shape of the peak for bovine rhodopsin while the bacteriorhodopsin peak tended toward some
smoothing. This result may indicate a special environment
for retinal binding in the two rhodopsins and yet some
differences relating to the unique functions of the chromophore in the two rhodopsins. Though the prediction algorithm has been calculated for only the C-terminal residues
of bovine rhodopsin, it is suggested that its fold is similar
570
Table 4. Amino acid scyrrenc.e spans ‘predicied‘ to he nwmhrane buried by the algorithm discu.wvl in the present work us u~ellas those regions ‘suggested‘
by chemical or theorcticul investigutions
Spans are only given if their weighted five-parameter peak heights were greater than or equal to 1.0. An ‘X’in the ‘suggested’ column indicates that
a span with specific amino acid boundaries was not given by the authors listed in the references
Molecule
Predicted
region
Glycophorin A
61- 98
Peak
height
3.8
Suggested
region
65- 98
Cytochrome bs
103-128
3.5
103-125
Cytochrome
204 - 229
3.0
X
9 - 20
52- 74
9- 20
45- 62
4- 18
1- 22
80- 93
125-156
180- 193
252-213
280- 31 3
329 - 340
25- 42
56- 80
1.1
2.1
1 .o
1.8
1 .I
1 .o
1 .o
1.2
1.3
1.8
1.3
1.3
X
1.2
1.3
X
c.1
ATP synthase
MI3 coal protein
Pre x-casein
Porin
Proteolipid
(N.crassa)
3*0
2 .o
X
4-
21
X
1
Comments
References
Hydrophobic domain determined by tryptic cleayage
sites
Two C-terminal helical segments suggested to be
buried completely in mcinbrane
Strongly hydrophobic span noted near predicted
region
Residues 51 -81 and 1-36 observed as largely
hydrophobic
Two spans suggested on either side or alanyl
residue 24, an exposed protcase cleavage site
Signal proteasc clcaves at Ala-21
Residua 83- 194 noted as nonpolar
140,671
Chemical evidence suggests Glu-65 to be membraneburied; circular dichroic studies indicate a helical
hairpin structure
[50,63]
[681
(411
1421
[44,53]
[23,51J
[391
structure will allow a more significant test of the hypothesis.
The details of the structure-function relationship of the helical
structure are discussed elsewhere 1321.
Membrane-bound Proteins
-1 .o
-2.0
Fig.3. Plot of the amino acid sequence number for the 108 C-terminal
residues in bovine rhodopsin 132J versus u weightedfive-parameter characteristic value for u given amino acid. The residues are numbered from
the C-terminus as 1 ’ to 108’. The two predicted helical spans designated
helix 1 and helix 2 are shown as black bars on the zero line. The residue
at 85’ was not determined but was taken as cysteine which is the comparable amino acid in the homologous ovine rhodopsin sequence [66]
to bacteriorhodopsin. Further support is provided by circular dichroic studies which indicate the secondary structure of the bovine rhodopsin to be 58% helical [35], linear
dichroism which suggests aligned transmembrane helices
[36,37] and neutron diffraction investigations that indicate
about half of the bovine rhodopsin molecular mass to be
buried in lipid [38]. A knowledge of the complete primary
The weighted five-parameter algorithm was applied to
the primary structure of other proteins known to be at least
partially bound to a lipid bilayer in an attempt to delineate
the buried regions. The proteins included the pore-forming
outer membrane protein I (porin) from Escherichia coli B/r
[39], human erythrocyte glycophorin A [40], bovine heart
cytochrome (‘1 [41], the proteolipid subunit of the ATP synthase from spinach chloroplasts [42], coliphage MI 3 coat
protein [43-461, bovine microsomal cytochrome hs [47-491,
the proteolipid subunit of the mitochondria1 adenosinetriphosphatase from Neurospora crussu [50], and various
amino-terminal extension sequences of secreted proteins
(signal sequences) as listed by Austen [23] and von Heijne [15].
The plots for these proteins and an exemplary signal sequence
(ovine pre x-casein [51]) are shown in Fig.4. Table 4 lists the
amino acid sequence spans that are associated with peak
heights greater than 1.O. Due to the end effects of the sevenpoint smoothing process, the seven residues at the two termini
of the primary structures are assigned a zero parametric value
in Fig.4. If a peak height occurred near these regions, the
terminal amino acid number was calculated as K f N where
K is the nearest residue number whose parametric value ( P K )
was unaffected by smoothing and N is the rounded integral
value of (PK/0.2). Table 4 also shows the amino acid spans
suggested to be within the membrane by chemical or theoretical investigations.
The predicted membrane-buried regions for glycophorin
A and cytochrome hs agree well with the segments determined
571
Y.0
3.0
n
3 .o
2.0
E: 2.0
2
r
3
y
1.0
c
K
Y
LL
E 0.0
c
-1
.o
-2.0
3.0
9.G
7
_I
Y.D
3.0
2.0
P.0
5
3 1.0
1.o
r
In
c
-2.0
u
Fig. 4. Plot of the amino acid st'quence number ( A A NO) for residues in various membrane-bound proteins versus a weiglited ,fi:ve-parametercharorferistic.vulue,fi)ra given amino acid. The residues are numbered from the N-terminus for all proteins. The termini of membrane-buried regions were
determined by the intersection points of the positive peaks with the zero line. The parametric value is shown as zero at each of the seven terminal
amino acids due to the end-effects of the least-squares 'smoothing' procedures [24]. The sources of the amino acid sequences are referenced in the text
chemically. Cytochrome c1 also displays a tail that is likely
to be encompassed by the lipid bilayer. The parametric peaks
for these three proteins are the largest in the sample, ranging
from 3.0-3.8. Since the prediction algorithm was refined by
identification of the helices in bacteriorhodopsin, it is suggested that the buried spans in the three proteins will adopt a
similar secondary structural configuration. The lengths of the
predicted helices are cornpatable with typical membrane
widths to be spanned. It is also noteworthy that the buried
tails are in the C-terminal regions of the molecules.
Membrane-buried helices have been proposed for signal
sequences (cf. [15,23,52]). Though the x-casein example
shows a peak height of only 1.7, the delineated membrane
segment is in good agreement with protease cleavage experiments [51]. Similar investigations suggest two buried helical
regions for M13 coat protein [53] and yet the parametric
Amino
acid
Normalized
preference value
Met
2.96
2.93
2.03
I .67
1.56
1.23
Leu
Phe
Ile
Ala
cys
Val
TrP
Thr
Ser
Pro
TYr
GlY
Gln
A%
His
Asn
Glu
LYS
ASP
1.14
1.08
0.91
0.81
0.76
0.68
0.62
0.51
0.45
0.29
0.27
0.23
0.15
0.14
maximums for the two regions are only 1.8 and 1.O. Though
the membrane inserted spans of ATP synthase are not well
known chemically, the algorithm indicates two such regions.
Thc character of the porin plot is certainly an exception.
There are seven peaks greater than 1 .O with an average length
of 21 residues; no buried tail is indicated. Porin is considered
to be an integral membrane protein which forms hydrophilic
channels allowing the diffusion of various low molecular
weight solutes (see Lodish and Rothman [54] for a recent
review). Circular dichroism and infrared spectroscopy indicate that a large fraction of the polypeptide exists in p-conformation [55]. Kennedy [56] has proposed various types of
regular structures which can favorably interact with the bilayer
interior: a-helices, P-barrels, and a Family of &helices. Engelman and Steitz [52] suggest from energetic consideration of
polypeptide structures in a lipid environment that only a
and 3,o helices will be observed in the membrane hydrophobic
interior. Porin has been recently crystallized [57] ;a knowledge
of its tertiary structure must await the X-ray dilTraction
results.
A few peak values in the remaining soluble regions of
cytochrome 65 approach 1.0 (Fig.4). In order to distinguish
between membrane-buried segments and hydrophobic regions
in soluble proteins, the algorithm was applied to the primary
sequence of eight soluble proteins with two taken from each
of the four basic structural classes [58]: all-a (sperm-whale
myoglobin and Themiste pyroides hemerythrin) ;all$ (bovine
Cu,Zn-superoxide dismutase and jack-bean concanavalin A) ;
a + /I (hen egg-white lysozyme and bovine pancreatic ribonuclease A) ; and u / j (bacteriophage T4 thioredoxin and
porcine muscle adenyl kinase). The primary structures are
listed by Levitt and Greer [22]. The plots for the soluble proteins resulted in 43 peaks with parametric values greater than
0.0; their average height was 1 . I with a standard deviation of
0.5 while the largest peak was 1.8 noted in myoglobin. It is
suggested that primary structural spans with parametric
maximums greater than 2.0 are likely to be within the lipid
environment. For peak heights between 0.0 and 2.0 it would
be difficult without experimental facts to distinguish between
hydrophobic areas in the soluble portion of the protein or
protein fragments in contact with or buried within the lipid
surface. However, the prediction results coupled with chemical evidence should be useful in discriminating among various
structural models for protein-lipid interactions.
Chou-Fasman preference parameters were claculated for
the twenty amino acids using a membrane-bound protein
data base (Eqn 5). It consisted of 1125 residues taken from
the seven helical spans of bacteriorhodopsin, the signal
sequence segments delineated by von Heijne [I 51 and Austen
[23] and residues associated with a peak value greater than
2.0 for the protein structures predicted in Table 4. Also
included were segments from several homologous ATP synthase proteolipids listed by Sebald and Wachter [42]. The
resulting membrane-buried preference values are given in
Table 5 ; they were normalized according to the distribution
of the amino acids in known soluble protein structures listed
by Levitt and Greer [22]. The correlations of the membranebound preferences with the Chou-Fasman helical and sheet
conformational preferences [ 161are 0.32 and 0.36 respectively,
indicating that the helical and sheet parameters would yield
erroneous predictions for lipid-buried protein segments. Of
the five hydrophobic parameters, correlation with the NozakiTanford values was the smallest at 0.44.
Buried Helicul Sidednrss
Engelman and Zaccai [59] have suggested through neutron-scattering experiments that bacteriorhodopsin is an
'inside-out' protein contrasting with the structural organization of soluble proteins. By comparing their electron density map of deuterated valines and phenylalanines with the
bacteriorhodopsin model structure, they indicated which
helical Faces were in contact with the exterior lipid bilayer.
The charged and polar residues were distributed on the interior
faces exposed to the protein while the strongly nonpolar
groups were on the exterior faces associated with the membrane side. With the use of the amino acid preferences for
lipid contact (Table 5), it was possible to detect the exterior
and interior faces for other membrane-bound proteins.
The successive C.-atoms in a helical peptide backbone
would, in projeclion down the helical axis, lie on a circle with
successive positions rotated by 100". Lines emanating from
the circle center and passing through the C , positions would
show thc projected direction of the associated amino iicid
side groups, giving the appearance of a helical 'wheel' [60].
Only 18 unique C, points separated by 20" would exist on the
wheel regardless of the helical length as there are on the
average only 3.6 residues per turn of an a-helix. This would
result in nine possible pairs of faces for any helix. If amino
acids with membrane-buried preferences less than 1.O (Table 5 )
tend to cluster on one side of a helical wheel; then the lipidfacing and protein-facing helical sides can be inferred. The
helical faces were chosen such that the arithmetic difference
between the number of residues N with a preference less than
1 .O on the two helical sides ( N I - N ~was
) a maximum.
Wheels for the two predicted helices in the C-terminal
region of the bovine rhodopsin sequence are shown in Fig. 5a.
The ( N l - N z ) values are respectively (9-2) and (6-0). It is
clear that amino acids not favoring lipid contact can be
generally relegated to one side of the helices. These results
suggest that the retinal-binding lysine sits within the protein
interior. A wheel analysis for the seven model helices
(A through G ) in bacteriorhodopsin resulted in respective
573
LEU
ALP 80' VAL 91'
I
M E 73'
PHE 76,*
ALA 77'
VAL 95'
LEU 83'
BOVINE
RHODOPSIN
I L E 74.
M T 92'
I L E ffi
LEU 2 5
TRP8O
DLD 98
PHE 88
LEU 9 4
ALD 81
BACTERIORHODOPSIN
(HELIX Cl
VAL 101
LEU 9 2
LEU97
I L E 78
LEU loo
DLD9
ILE6 2
MET 19
VDL 13
MI3 COAT
PROTEIN
VDL 17
\
/
VALIt
I L E 45
MET51
DLD14
(d)
DLD62
PHE 80
DLD 28
MET73
DLD 66
LEU 6 9
ILE 58
LEU 76
VDL 35
PROTEOLIPID
LEU 5 9
MET 77
PHE 70
PROTEOLIPID
DLD38
LEU 34 & I L E
ILE77
30
I L E 88
VAL 84
I L E 73
I L E 91
I L E 85
GLYCOPHORIN
I L E 76
F-
LEU 75
LEU^
,+0
GLY 7 9
GLy86
Fig. 5. Helical wlteels for the diferenr membrane-hound proteins. (a) Helical
wheels [60] for the two predicted membrane-buried helices in the C-terminal
segment of bovine rhodopsin. The views are projections down the helical axis
with successive C, positions rotated to 100"along the projected peptide backbones. The direction of the projected side chains are indicated by spokes
emanating from the wheel center. Amino acids with membrane-buried propensities (Table 5 ) less than 1.0 are boxed. The side of the helices suggested to
face the protein interior is indicated by thick lines. (b) Helical wheels for bacteriorhodopsin model helices A and C as proposed by Engelman et al. IS].
(c) Helical wheels for the two predicted membrane-bound regions in coliphage MI3 coat protein. (d) Helical wheels for the two predicted mernbranebound segments in the proteolipid subunit of the mitochondria1 adenosinetriphosphatase from Nuurosporu crassa. (e) Helical wheel for the predicted
membrane-buried region in human erythrocyte glycophorin A
514
( N 1 - ~ 2values
)
of (9-1). (7-3), (7-l), (7-3), (5-2), ( 7 4 , and
(6-3). Wheels for helices A and C are given as examples in
Fig. 5 b. The amphipathic nature of putative membraneburied helices has also been noted for other proteins; for
example, diphtheria toxin fragment B [28,61] and E. coli
murein-lipoprotein [62].
A model consisting of two membrane-buried helices has
been proposed for the coliphage M13 coat protein [53].The
prediction algorithm indicates two possible segments of the
M13 protein in contact with lipid (Table 3 and Fig. 4). A helical
wheel analysis of these regions (Fig. 5c) suggests a sidedness
for the putative helices, thus supporting the model of two
helices in contact with each other and the membrane. A similar structure can be inferred for the proteolipid subunit of the
mitochondrial adenosinetriphosphatases from N. cmssu. The
prediction routines applied to the subunit primary sequence
[50] suggest two membrane-buried segments (Fig.4) whose
wheels show sidedness (Fig. 5d). Recent circular dichroic
studies also suggest a helical hairpin structure for the proteolipid monomer [63]. Since the major subunit of the ATP
phosphohydrolase complex of the N . crassa mitochondrial
inner membrane is likely to be a hexamer of the proteolipid
subunits. a twelve-helical bundle can be envisaged for the
proteon-translocating structure 1421.
The prediction method indicated glycophorin A residues
67 - 98 as membrane-buried candidates. Recent cross-linking
studies (A. H. Ross, R. Radhakrishnan, R. J. Robson and
H. G . Khorana, unpublishcd rcsults) suggest that Glu-70 is
within the bilayer and that residues 62 - 96 probably define the
boundaries of the membrane-embedded segment in glycophorin A. A helical wheel for amino acids 73 - 94 displays a
distinct sidedness (Fig. 5e). Terminal spans were not included
in the wheel as they contained charged amino acids which are
likely to interact with the polar lipid headpieces and therefore
may not participate in the transmembrane helical structure.
The distinct facedness of the putative glycophorin helix would
suggest that glycophorin A acts as a dimer within the membrane, which is also supported by cross-linking investigations
(see Marchesi et al. [65] for a review).
Conclusions
A prediction algorithm based on the physical characteristics of the twenty amino acids can be used to indicate which
regions in the primary sequence of a membrane-bound protein
arc likely to be in contact with the lipid bilayer. A helical
wheel analysis of these primary structural spans coupled with
chemical evidence allows discrimination among hypothetical
models of secondary structural association within the membrane.
The authors wish to express thanks to Drs William Cramer, Schlomo
Pundak, and Nancy Scavarda for many useful discussion and to Marilyn
Anthony for help in the preparation of the manuscript. P.A. acknowledges support from the National Institutes of Health (grant no. GM27682)
and the American Cancer Society (Faculty Research Award no. FRAl73).
P.A.H. acknowledges support from the National Institutes of Health
(grant nos. EY1275 and ER2875) and from the National Science Foundation (grant no. PCM77-17808).
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