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Introduction
The two barriers separating the
central nervous system (CNS) from the periphery are the blood-brain
barrier (BBB), located at the endothelial cells of the brain tissue
capillaries, and the blood-cerebrospinal fluid barrier (B-CSF-B), at
the choroids plexus and the circumventricular organs[1].
Formed by complex tight junctions of the brain capillary endothelial
cells, the BBB segregates the circulating blood from interstitial
fluid in the brain[2]. The capillary endothelial cells
regulate the permeability property of the BBB. However, there are at
least four kinds of cells that comprise the brain microvasculature,
and all contribute to the regulation of the cerebral
microvasculature and, indirectly, to the regulation of BBB
permeability. The endothelial cell and the pericyte share a common
capillary basement membrane. There is approximately one pericyte for
every two to four endothelial cells[3]. Also,
immunohistochemistry is a widely used research technique in BBB
research for the cellular localization of proteins of interest in
normal vessels and the documentation of altered expression following
disease states, for the identification of cultured cells and for the
spatial localization of novel gene products[4].
Although the BBB was thought to act
as a static wall protecting the brain, application of recent
advanced methodologies to study the BBB has led to the new concept
that the BBB acts as a dynamic regulatory interface. Using primary
cultured bovine brain capillary endothelial cells, Tsuji et al[5,6]
have found that P-glycoprotein (ABCB1) acts as an efflux pump
for the anti-cancer drugs, vincristine, at the BBB. Schinkel et
al[7-9] have developed the mdr 1a gene
knockout mouse and proved that P-glycoprotein (ie, mdr 1a
gene products) plays a key role in restricting the apparent
cerebral distributed vinblastine (a substrate of P-glycoprotein)
across the BBB. However, several hydrophilic substrates such as
metabolites of cerebral neurotransmitters are present in the brain,
which reduce the cerebral concentration, and as a result, could play
an important role in CNS detoxification.
To be effective, CNS therapeutic
agents must have the ability to cross over the BBB whereas
peripherally acting drugs should hardly be able to pass the BBB. The
uptake of a compound into the brain is a complex process. The
moderately lipophilic drugs can pass the BBB by passive diffusion
and the hydrogen bonding properties of drugs significantly influence
their particular CNS uptake profiles. Polar molecules are generally
poor CNS agents unless they undergo active transport to pass the
CNS. Size, ionization properties, and molecular flexibility are
other factors observed to influence transport of an organic compound
across the BBB[10-13]. Recently, there has been a surge
in computational efforts to evaluate absorption, distribution, meta-bolism,
excretion, and toxicity (ADME/T) properties of drugs. These new
computational approaches remain to focus on modeling structurally
diverse data sets by dealing with the properties of the solutes.
These properties are limited to relative lipophilicity indices,
solvation and hydrogen bond parameters, topological indices, and
limited three-dimensional solute properties[14-19]. Iyer
et al[20] have developed a methodology called
membrane-interaction (MI)-QSAR analysis, where structure-based
design methodology is combined with classic intramolecular QSAR
analysis to model different compounds interacting with cellular
membranes. They have also built a predictive model of BBB
penetration of organic compounds by simulating the interaction of an
organic compound with the phospholipide-rich region of cellular
membranes. As a result, they indicated that BBB penetration of an
organic compound depended upon PSA, ClogP, and the conformational
flexibility of the compounds as well as the strength of their
"binding" to the model biologic membrane. The BBB penetration
process can be reliably described for structurally diverse molecules
whose interactions with the phospholipide-rich regions of cellular
membranes are explicitly considered. There are other important
applications of MI-QSAR analysis. For example, it can be used as a
computational approach to estimate ADME properties such as the
transport of organic solutes through biological membranes; and by
this way, we can forecast intestinal absorption[21] of
drugs and construct MI-QSAR model for skin irritation[22],
and eye irritation[23]. However, as a prediction measure,
the MI-QSAR computational model is itself somewhat inconvenient. It
is quite easily susceptible to manipulation during the prediction
process, and so models with more reliability can still have a
reasonable-looking MI-QSAR model. Moreover, there are several
non-MI-QSAR computational models including other descriptors besides
PSA and ClogP reported to describe and predict BBB penetration.
Lombardo and colleagues[17] reported about computing BBB
penetration of organic solutes via free energy calculations. Keseru
et al[24] clarified a high-throughput prediction
of BBB penetration of organic molecules using a thermodynamic
approach. Crivori et al[25] elucidated a method to
predict BBB penetration from a three-dimensional molecular
structure. Their research results showed that the BBB penetration
only relies on one or two descriptors, which leads to the
simplification of the prediction model of BBB.
In this article, we focus on
constructing the predictive models of BBB penetration of organic
compounds on the basis of QSAR analysis and MI-QSAR analysis.
Materials and methods
Building solute molecules
A training set of 37 organic compounds[26,27] (Table 1)
and a test set of 8 organic compounds (Table 2) were selected. These
compounds had ranges in molecular weights from 16.03 to 448.58,
whose concentrations in blood and brain (Cblood
and Cbrain) were measured in units of mmol/L, and
there were variations in net charge at pH 7.4[26]. The
dependent variable used in this theoretical model was the logarithm
of the BBB partition coefficient, log BB=log (Cbrain/Cblood)
[27]. Experimental values of log BB published to date covered
the range of about -2.00 to +1.04. Within this range, compounds with
log BB>0.30 cross the BBB readily while compounds with log BB<-1.00 are poorly distributed to the brain[20,27]. All
these compounds were built on a PC computer using the Build module
of the commercial software packages Hyperchem 6[28].
First, the geometry of these compounds were opitimized using the
Amber 94 force field in gas state. Second, they were placed in a
periodic solvent box whose volume was X=16Å, Y=10 Å,
Z=18Å, which included 96 water molecules. Here, temperature was
300 K and pressure was 101.325 kPa. Then the compounds in water were
minimized by the above method. Third, the compounds in water were
simulated by the Monte Carlo method and minimized by the above
method.
Molecular modeling of a DMPC
membrane monolayer complex with a layer of water (DMPC-water model)
A model of dimyristoylphosphatidylcholine (DMPC) membrane
monolayer was constructed using the software Material Studio[29],
and minimized for 200 steps with the smart minimizer. According to
the work done by van der Ploeg and Berendsen[30], the
DMPC monolayer was composed of 25 DMPC molecules (5¡Á5¡Á1).
Here, the unit cell parameters used
for building the DMPC monolayer were a=8Å, b=8Å, and g=96.0º, which
yield an average surface area per phospholipid of 64Å2
that was similar to Stouch's research results[31].
Moreover, we added a layer of water (40¡Á40¡Á10) including 529 water
molecules to the polar side of the DMPC monolayer.
Molecular dynamic simulation
(MDS) of a solute-membrane-water complex In order to prevent
unfavorable van der Waals interactions between a solute molecule and
the membrane DMPC molecules, one of the "center" DMPC molecules was
removed from the DMPC-water model and an organic compound (solute)
was inserted in the space created by the missing DMPC molecule to
form a solute-membrane-water complex. The solute was inserted at
three different positions in the DMPC-water model and three
corresponding MDS models were generated for each compound. MDS of
the complex was performed for 1000 steps using Material Studios[29]
with a Compass force field. Here, the three-dimensional volume
was restricted to a boundary of X=40Å, Y=40Å, Z=91.76Å,
and g=96.0¡ã.
Calculation of descriptors
Most of the intramolecular solute descriptors were calculated by the
commercial software packages CS Chem3D Ultra7.0[32],
which included molecular mechanism (MM) parameters, quantum
chemistry parameters, hydrophobic parameters (such as ClogP), stereo
parameters (such as Es and Balaban Index) and so on. The MM
parameters comprised bending energy, stretch-bend energy, torsion
energy, total energy, van der Waals energy and others. The quantum
chemistry parameters consisted of electronic energy, HOMO energy,
LUMO energy, total energy, and so on. The data of molecular PSA
(polar surface area) came from Iyer and colleagues[20].
The intermolecular solute-membrane
interaction descriptors were extracted directly from the MDS
trajectories in which the solute-membrane-water complex had the
lowest energy geometry. These descriptors were mainly energy
parameters. The total energy of a system could be expressed as
follows[20]:
Etotal=Evalence+Ecrossterm+Enonbond
Here, the valence interactions
include bond stretching (bond), valence angle bending (angle),
dihedral angle torsion (torsion), and inversion, also called
out-of-plane interactions (oop) terms, which are part of nearly all
forcefields for covalent systems. In addition, a Urey-Bradley term (UB)
may be used to account for interactions between atom pairs involved
in 1, 3 configurations (ie, atoms bound to a common atom). Evalence=Ebond+E
angle+Etorsion+E oop+Eup.
Modern (second-generation) forcefields generally achieve higher
accuracy by including crossterms to account for such factors as bond
or angle distortions caused by nearby atoms. Crossterms can include
the following terms: stretch-stretch, stretch-bend-stretch,
bend-bend, torsion-stretch, torsion-bend-bend, bend-torsion-bend and
stretch-torsion-stretch. The interaction energy between non-bonded
atoms is accounted by van der Waals, electrostatic (Coulomb), and
hydrogen bond terms in some older forcefields. Enon-bond=
Evan-der-Waals+ECoulomb +Ehydrogen-bond.
Restraints that can be added to an energy expression include
distance, angle, torsion, and inversion restraints. Restraints are
useful if you, for example, are interested in only part of a
structure for information on restraints and their implementation,
use, and also the documentation for the particular simulation
engine.
Construction and testing of MI-QSAR
models MI-QSAR models of some organic compounds through BBB were
constructed by partial sum of squares for regression using software
SPSS. A training set of 37 structurally diverse compounds whose BBB
partition coefficients had been measured was used to construct MI-QSAR
models. MDSs were used to determine the explicit interaction of each
test compound with the DMPC-water model. An additional set of
intramolecular solute descriptors were computed and considered in
the trial pool of descriptors for building MI-QSAR models. The QSAR
models were optimized using multidimensional linear regression
fitting and stepwise method. A test set of 8 compounds was evaluated
using the MI-QSAR models as part of a validation process.
Results
Building solute molecules
A training set of 37 organic compounds and a test set of 8 organic
compounds were built and minimized, dissolved in liquid, and
optimized by Monte Carlo method and MM. Finally, the dominant
conformations of these compounds were obtained (Figure 1).
MDS of a solute-membrane-water
complex The result revealed that the energy of a solute inserted
at the middle position of the DMPC-water model was lower than that
of the other two positions. Figure 2 shows the dominant conformation
of a solute-membrane-water complex in the MDS.
Construction and testing of
MI-QSAR models MI-QSAR analysis was used to develop predictive
models of some organic compounds through BBB and to simulate the
interaction of a solute with the phospholipide-rich regions of
cellular membranes surrounded by a layer of water. Molecular
descriptors of 37 compounds in the training set were listed in Table
3. Six MI-QSAR equations were constructed based on Table 3 and were
listed as follows:
log BB=0.552-1.73¡Á10-2
PSA
n=37 R=0.835 S=0.398
(1)
log BB=0.229-1.70¡Á10-2
PSA+0.131 Clog P
n=37 R=0.878 S=0.352
(2)
log BB=4.965¡Á10-2-1.28¡Á10-2
PSA+0.211 Clog P -6.40¡Á10-7 BIndx
n=37 R=0.924 S=0.285
(3)
log BB=6.262¡Á10-2-1.36¡Á10-2
PSA+0.205 Clog P -7.11¡Á10-7 BIndx -0.185Esb
n=37 R=0.938 S=0.264
(4)
log BB=6.580¡Á10-2-1.21¡Á10-2
PSA+0.206 Clog P -7.77¡Á10-7 BIndx-0.197Esb+1.330¡Á10
-3DEtotal
n=37 R=0.947 S=0.248
(5)
log BB=8.730¡Á10-2-1.04¡Á10-2
PSA+0.222 Clog P -9.60¡Á10-7 BIndx-0.183Esb+1.364¡Á10
-3 DEtotal-2.68¡Á10-3DEtorsion
n=37 R=0.955 S=0.232
(6)
where PSA is the polar surface area,
ClogP is the calculated logP (the logarithm of the partition
coefficient for octanol/water), BIndx is the Balaban Index, namely
connective index of molecular average total distance (relative
covalent radius), and Esb is the stretch-bend
energy of a molecule. These intramolecular solute descriptors came
from CS calculation. In addition, calculated from the MDS,
intermolecular descriptors DEtotal and DEtorsion
are related to interactions between a solute and the DMPC-water
model. They display the change in the total potential energy and the
dihedral torsion energy of the solute-membrane-water complex
comparing with that of the DMPC-water model, respectively. Here,
n is the number of organic compounds, R is the
correlation coefficient, and S is the standard deviation.
With the increase of the variable
from one to six, the relativity of MI-QSAR equations was also
improved, and the predictive ability of the models was enhanced.
Figure 3 displaye a diagnostic plot of the MI-QSAR models. Here,
equation 6 was the most significant, which means that the capability
of an organic compound through BBB depends upon PSA, ClogP, BIndx,
Esb, DEtotal, and DEtorsion.
Moreover, the potential of an organic compound through BBB is
directly proportional to ClogP and DEtotal, but
inversely proportional to PSA, BIndx, Esb, and
DEtorsion. The observed and predicted log BB values
of the training set are listed in Table 5 and plotted in Figure 4.
The predicted log BB value of compound 18 in the training set was
much higher than observed, and this molecule has also been
identified as an outlier in other studies[20].
Protonation of the molecule could account for its low log BB value.
A test set of 8 organic compounds
was constructed as a way to attempt to validate the MI-QSAR models
given by the six equations mentioned. The compounds of the test set
were selected so as to span almost the entire range in BBB
penetration. The observed and predicted log BB values for this test
set are given in Table 6 and plotted in Figure 5. It seems that the
5-6 terms MI-QSAR models could predict log BB for other compounds in
drug design.
Discussion
We have built up a theoretical model
of BBB penetration of organic compounds by simulating the
interaction of an organic compound with the phospholipid-rich
regions of cellular membranes. The family of these MI-QSAR models
reveal that the capability of an organic compound through BBB focus
on six significant features, which are PSA, ClogP, BIndx, Esb,
DEtotal, and DEtorsion. The
descriptor PSA is found as a dominant descriptor in these MI-QSAR
models, which is related to the aqueous solubility of the solute and
can be used as a direct lipophilicity descriptor[19].
When the value of PSA lessens within the range from 0 to 108.80 Å2,
the value of log BB will increase. This is consistent with the
experimental result that the higher polarity it possesses, the more
difficultly a molecule enters the hydrophobic environment of BBB[31].
Along with PSA, many descriptors can display various other kinds of
the hydrophobic parameters of compounds, such as ClogP. In some
cases it may be appropriate to display the parameter in the form of
meshes, such as PSA. The higher the hydrophobic property, the
greater the value of ClogP is. And the value of log BB of a molecule
increases with the increase of ClogP. It means that the hydrophobic
molecule can pass through BBB more easily than the hydrophilic
molecule does, which is supported by the experimental results[33].
As stated, BIndx is the connective index of molecular average total
distance, which pertains to the volume parameter. Our research
result reveals that with the accretion of its bulk, a molecule
becomes more and more difficult to cross over BBB by diffusion. The
presence of the descriptor Esb suggests that with
the decrease of the stretch-bend energy the value of log BB
increases.
Interestingly, the other two
descriptors, ¦¤Etotal, and
¦¤Etorsion,
reflect the interaction of the solute with the membrane and the
behavior of the entire membrane-solute complex. Here, the more the
value of ¦¤Etotal changes, the more the value of
log BB increases. This is because that small molecule acrossing the
BBB membrane leads to the change in the structure of the
complex, which therefore, results in a greater change of total
potential energy, and the accretion of the energy change is the most
important cause for the increase of BBB penetration of small
molecules. In contrast, the less the difference in the torsion
energy is, the larger the value of log BB is. It displays that a
small molecule tightly combined with the membrane-water complex has
a higher value of log BB. The relationship suggests that as the
solute becomes more flexible within the membrane-water complex, its
log BB value would increase, which is in agreement with the research
results by Iyer et al[20].
As an extra bonus of our work, we
have developed an extension of traditional computational approaches
that combines QSAR with solute-membrane-water complex. There is an
obvious difference between our method and Iyer's method, which is
the addition of a layer of water on the hydrophilic side of the DMPC
membrane monolayer. So it is more analogous to the true BBB
environment. Our results revealed that the distribution of organic
molecules through BBB was not only influenced by the properties of
organic solutes, but also related to the property of the
solute-membrane-water complex. The former involves the polarity,
hydrophobicity, size, and conformational freedom degree of organic
molecules. The latter deals with the strength of an organic molecule
to combine with the BBB membrane and the structural changeability of
a solute-membrane-water complex. Moreover, the capability of a small
molecule across BBB is mainly related to four physicochemical
factors, which are the relative polarity of a small molecule, the
molecular volume, the strength of a small molecule to combine with
DMPC-water model, and the changeability of the structure of a
solute-membrane-water complex. The MI-QSAR model shows that,
relatively, less polar and more hydrophobic small molecules, which
tightly combine with the membrane-water complex and are more
flexible within the complex, can easily pass through BBB and enter
the brain to be effective. In drawing conclusions from our model, it
seldom matters if one or two parameters are slightly off (eg,
BIndx), but it is often critical if some parameters are actually
in the wrong value (eg, ClogP, PSA, or Esb):
that will change which molecules are in a position to penetrate
through BBB.
Incidentally, since the molecular
structures in the training set are not very comparable, our MI-QSAR
equations possess universal significance. Nevertheless, the
precision of the MI-QSAR equation is so low that there is still some
time before it can be applied. If a series of organic compounds with
similar structures were chosen to construct a training set, the
precision of MI-QSAR simulation may be largely increased, while the
prediction of the analogues through BBB will be greatly improved.
In conclusion, we have developed an
extension of traditional computational approaches that combines QSAR
with solute-membrane-water complex to simulate the BBB environment,
which resembles Iyer's method, but differs from it by adding a layer
of water on the hydrophilic side of the DMPC membrane monolayer. Our
modified MI-QSAR method is more approximate to the body condition
than Iyer's MI-QSAR analysis and possesses higher ability to predict
organic compounds across BBB. Moreover, while still applying the
structural information in a two-dimensional, "structure-function
relationship" fashion, this method also takes into account the
powerful three-dimensional information displayed by membrane
structures, and thus improves existing MI-QSAR method. The MI-QSAR
models indicate that the distribution of organic molecules through
BBB was not only influenced by organic solutes themselves, but also
related to the properties of the solute-membrane-water complex, that
is, interactions of the molecule with the phospholipid-rich regions
of cellular membranes.
References
- 1 Bickel U, Yoshikawa T,
Pardridge WM. Delivery of peptides and proteins through the
blood-brain barrier. Adv Drug Deliv Rev 2001; 46: 247-79.
- 2 Hosoyo K, Ohtsuki S, Terasaki
T. Recent advances in the brain-to-blood efflux transport across
the blood/brain barrier. Int J Pharm 2002; 248: 15-29.
- 3 Pardridge WM. Molecular
biology of the blood-brain barrier. Methods Mol Med 2003; 89:
385-99.
- 4 Nag S. Immunohistochemical
detection of endothelial proteins. Methods Mol Med 2003; 89:
489-502.
- 5 Tsuji A, Tamai I.
Carrier-mediated or specialized transport of drugs across the
blood-brain barrier. Adv Drug Deliv Rev 1999; 36: 277-90.
- 6 Tamai I, Tsuji A. Drug
delivery through the blood-brain barrier. Adv Drug Deliv Rev
1996; 19: 401-2.
- 7 Jette L, Murphy GF, Leclerc
JM, Beliveau R. Interaction of drugs with P-glycoprotein in
brain capillaries. Biochem Pharmacol 1995; 50: 1701-9.
- 8 Chen W, Mehta SC, Lu DR.
Selective boron drug delivery to brain tumors for boron neutron
capture therapy. Adv Drug Deliv Rev 1997; 26: 231-47.
- 9 Friden PM. Utilization of an
endogenous cellular transport system for the delivery of
therapeutics across the blood-brain barrier. J Control Release
1997; 46: 117-28.
- 10 Begley DJ. The blood-brain
barrier: Principles for targeting peptides and drugs to the
central nervous system. J Pharm Pharmacol 1996; 48: 136-46.
- 11 Anderson BD. Prodrugs for
improved CNS delivery. Adv Drug Deliv Rev 1996; 19: 171-202.
- 12 Pardridge WM. CNS drug
design based on principles of blood-brain barrier transport. J
Neurochem 1998; 70: 1781-92.
- 13 Cornford EM, Hyman S.
Blood-brain barrier permeability to small and large molecules.
Adv Drug Deliv Rev 1999; 36: 145-63.
- 14 Liu R, Sun H, So SS.
Development of quantitative structure-property relationship
models for early ADME evaluation in drug discovery. 2.
Blood-brain barrier penetration. J Chem Inf Comput Sci 2001; 41:
1623-32.
- 15 Rogers D, Hopfinger AJ.
Applications of genetic function approximation to quantitative
structure-activity relationships and quantitative
structure-property relationships. J Chem Inf Comput Sci 1994;
34: 854-66.
- 16 Abraham MH, Chadha HS,
Mitchell RC. Hydrogen bonding factors that influence the
distribution of solutes between blood and brain. J Pharm Sci
1994; 83: 1257-68.
- 17 Lombardo F, Blake JF,
Curatolo WJ. Computation of brain-blood partitioning of organic
solutes via free energy calculations. J Med Chem 1996; 39:
4750-5.
- 18 Luco JM. Prediction of
brain-blood distribution of a large set of drugs from
structurally derived descriptors using partial least squares
(PLS) modeling. J Chem Inf Comput Sci 1999; 39: 396-404.
- 19 Clark DE. Rapid calculation
of polar molecular surface area and its application to the
prediction of transport phenomena. 2. Prediction of blood-brain
barrier penetration. J Pharm Sci 1999; 88: 815-21.
- 20 Iyer M, Mishra R, Han Y,
Hopfinger AJ. Predicting blood-brain barrier partitioning of
organic molecules using membrane-interaction QSAR analysis.
Pharm Res 2002; 19: 1611-21.
- 21 Kulkarni A, Han Y, Hopfinger
AJ. Predicting Caco-2 cell permeation coefficients of organic
molecules using membrane-interaction QSAR analysis. J Chem Inf
Comput Sci 2002; 42: 331-42.
- 22 Kodithala K, Hopfinger AJ,
Thompson ED, Robinson MK. Prediction of skin irritation from
organic chemicals using membrane-interaction QSAR analysis.
Toxicol Sci 2002; 66: 336-46.
- 23 Kulkarni A, Hopfinger AJ,
Osborne R, Bruner LH, Thompson ED. Prediction of eye irritation
from organic chemicals using membrane-interaction QSAR analysis.
Toxicol Sci 2001; 59: 335-45.
- 24 Keseru GM, Molnar L.
High-throughput prediction of blood-brain partitioning: A
thermodynamic approach. J Chem Inf Comput Sci 2001; 41: 120-8.
- 25 Crivori P, Cruciani G,
Carrupt PA, Testa B. Predicting blood-brain barrier permeation
using three-dimensional molecular structure. J Med Chem 2000;
43: 2204-16.
- 26 Abraham MH, Chadha HS,
Mitchell RC. Hydrogen bonding. Part 36. Determination of
blood-brain barrier distribution using octanol-water partition
coefficients. Drug Des Discov 1995; 13: 123-31.
- 27 Abraham MH, Takacs-Novak K,
Mitchell RC. On the partition of ampholytes: Application to
blood-brain distribution. J Pharm Sci 1997; 86: 310-5.
- 28 Hyperchem HyperChem. Release
6.0 for MS Windows. Waterloo, Ontario, Hypercube Inc, 2001.
- 29 Materials Studios. San
Diego, USA, Accelrys Inc, 2001
- 30 van der Ploeg P, Berendsen
HJC. Molecular dynamics simulation of a bilayer membrane. J Chem
Phys 1982; 76: 3271-6.
- 31 Stouch TR. Lipid membrane
structure and dynamics studied by all atom molecular dynamics
simulations of hydrated phosphatidylcholine vesicles. Mol
Simulation 1993; 1: 335-62.
- 32 Chemoffice 2002 CS Chem3D
Ultra7.0. Cambridge, USA, Cambri-dgesoft Inc, 2002
- 33 Kaliszan R, Markuszewski M.
Brain-blood distribution described by a combination of partition
coefficients and molecular mass. Int J Pharm 1996; 45: 9-16.
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