The EMBO Journal Vol.19 No.5 pp.800–806, 2000
NEW EMBO MEMBER’S REVIEW
The importance of aquaporin water channel protein
structures
A.Engel1, Y.Fujiyoshi2 and P.Agre3
M.E.Müller-Institute for Microscopy at the Biozentrum, University of
Basel, CH-4056, Switzerland, 2Department of Biophysics, Faculty of
Science, Kyoto University, Kitashirakawa, Sakyo-Ku, Kyoto, 606-01,
Japan and 3Departments of Biological Chemistry and Medicine, Johns
Hopkins University School of Medicine, Baltimore, MD 21205-2185,
USA
1Corresponding
author
e-mail:
[email protected]
The history of the water channel and recent structural
and functional analyses of aquaporins are reviewed.
These ubiquitous channels are important for bacteria,
plants and animals, exhibit a pronounced sequence
homology and share functional as well as structural
similarities. Aquaporins allow water or small specific
solutes to pass unhindered, but block the passage
of ions to prevent dissipation of the transmembrane
potential. Besides advances in structure determination,
recent experiments suggest that many of these channels
are regulated by pH variations, phosphorylation and
binding of auxiliary proteins.
Keywords: aquaporins/atomic force microscopy/electron
crystallography/electron microscopy
Background
Water flows through the membranes of all living cells by
two distinct mechanisms. Diffusion of water through
pure lipid bilayers occurs with high activation energy
(Ea ⬎10 kcal/mol). In contrast, for ⬎40 years it has been
known that the rapid flow of water through human red
cell membranes occurs with Ea ⬍5 kcal/mol, leading to
the hypothesis that water pores must exist (Sidel and
Solomon, 1957). Multiple observations provided clues to
the functioning of water channels in a variety of specialized
membranes, and it has long been recognized that the
permeation of this pore is remarkably specific, since other
small molecules, ions or even protons (H3O⫹) are not
accommodated (reviewed in depth by Finkelstein, 1987).
Nevertheless, the molecular identity of water channels
remained unknown until the 1990s.
Two decades ago, homeostasis of the eye lens was
attributed to special channels in the lens fiber cell membranes, but their nature was subject to controversy. The
protein forming the square arrays observed in freezefracture replicas of lens fiber cells (Figure 1) had been
identified as the major intrinsic protein, MIP (now also
known as AQP0), a hydrophobic protein of Mr 26 kDa
(Kistler and Bullivant, 1980). Based on the amino acid
sequence, AQP0 was predicted to contain six hydrophobic
membrane-spanning regions and five connecting loops of
variable length. The tripeptide motif Asn–Pro–Ala (NPA)
800
in the two longest loops, and the sequence homology
between the N- and C-terminal halves of the molecule
were recognized as particular features of this abundant
membrane protein (Gorin et al., 1984). Despite this
information, the function of AQP0 was not evident.
The sensitivity of red cell water permeation to HgCl2
and certain organomercurials indicated the presence of a
critical sulfhydryl in the water pore (Macey and Farmer,
1970). Radiation target analysis suggested that water flow
by proximal renal membrane vesicles may be mediated
by a protein of ~30 kDa (van Hoek et al., 1991). At the
same time, an abundant 28 kDa protein with homology
to AQP0 was discovered in red cell membranes and was
suspected to be the water channel (Preston and Agre,
1991; Smith and Agre, 1991). This suspicion proved
correct, for when the 28 kDa protein was expressed in
Xenopus laevis oocytes, mercurial-sensitive water permeation appeared (Preston et al., 1992). This protein is now
known as aquaporin-1 (AQP1).
The aquaporin protein family
Many proteins related to AQP1 and AQP0 have been
identified subsequently in diverse life forms (Park and
Saier, 1996; Froger et al., 1998; Heymann and Engel,
1999). The aquaporin family includes strict water channels
as well as channels transporting solutes such as urea and
glycerol. Recent studies have suggested that aquaporins
may also be permeated by gases (Cooper and Boron,
1998). Importantly, a channel allowing the passage of
water but blocking the passage of ions should not dissipate
the transmembrane potential. This contrasts with the ease
with which protons tunnel along a single file of hydrogenbonded water molecules in an unselective channel such
as gramicidin A (Pomès and Roux, 1996). Thus, aquaporins must contain specific sites that prevent ions from
passing through the channel. Such sites must be sought
among conserved residues and in the atomic structures of
these proteins.
Aquaporins are tetrameric proteins
AQP1 is a homotetramer containing four independent
aqueous channels (Smith and Agre, 1991; Verbavatz et al.,
1993; Jung et al., 1994; Shi et al., 1994). When solubilized
in octylglucoside, AQP1 sediments like a 190 kDa tetrameric protein (Smith and Agre, 1991). Mass determination
by scanning transmission electron microscopy (STEM)
yielded a mass of 200 kDa, while negatively stained
solubilized AQP1 revealed square-shaped particles of
~7 nm side length exhibiting four domains (Walz et al.,
1994a; Figure 2A). Similarly, AQP0 solubilized in decylmaltoside has a mass of 160 kDa and exhibits a size of
7 nm (Hasler et al., 1998; Figure 2B). The Escherichia
© European Molecular Biology Organization
Aquaporin water channel protein structures
coli water channel, AqpZ, is a square-shaped particle
after solubilization in octylglucoside and negative staining
(Ringler et al., 1999; Figure 2C) and remains tetrameric
even during SDS–PAGE (Borgnia et al., 1999). As illustrated in Figure 2D, the solubilized bacterial glycerol
facilitator GlpF is a square-shaped particle of 9–10 nm
side length, also suggesting a tetrameric protein (T.Braun,
A.Philippsen and H.Stahlberg, personal communication).
However, the requirement for tetramerization of a protein
that forms four apparently independent channels remains
enigmatic.
Aquaporins form tetragonal arrays
When reconstituted into lipid bilayers, AQP1 forms twodimensional lattices with a unit cell of 9.6 nm side length
containing two tetramers in opposite orientations (Mitra
et al., 1994; Walz et al., 1994b; Jap and Li, 1995). The
same packing arrangement has been observed for AqpZ
(Ringler et al., 1999), while AQP0 assembles into tetragonal arrays with a single tetramer per unit cell of 6.4 nm
side length (Hasler et al., 1998). Projection maps obtained
from these lattices by cryo-electron microscopy revealed
quite similar features. The common motif includes four
monomers comprising a low-density region surrounded
by 7–9 density maxima, depending on the resolution
achieved (Figure 3). The density minimum within monomers is always shifted towards the 4-fold center, where
the lowest density within the tetramer is found. Monomers
are separated by gaps arranged in a cross, which exhibit
pronounced low-density regions in AQP1 and AqpZ.
Three-dimensional structure
Fig. 1. Tetragonal arrays in lens fiber cell membranes are revealed by
freeze–fracture techniques. The arrays are assembled from the major
intrinsic protein, MIP (Kistler et al., 1980), the first member of the
water channel protein family to be sequenced (Gorin et al., 1984) (by
courtesy of J.Kistler, unpublished). Scale bar, 100 nm.
The three-dimensional structure of AQP1 has been determined at 6 Å resolution by cryo-electron microscopy
(Figure 4A). Each AQP1 monomer has six tilted, bilayerspanning α-helices (Li et al., 1997), which form a righthanded bundle surrounding a central density (Cheng et al.,
1997; Walz et al., 1997; Figure 4B), confirming the
membrane topology predicted by sequence analysis and
epitope insertion studies of AQP1 (Preston et al., 1994).
At 4.5 Å resolution, several rod-shaped densities reveal
protrusions that follow a right-handed helical pattern
consistent with the expected density of an α-helix
(Mitsuoka et al., 1999; Figure 4C).
Site-directed mutagenesis on the loops containing the
NPA motifs predicted that these segments line the path of
water permeation (Jung et al., 1994). The similarity to an
ancient time-piece inspired the ‘hourglass’ model in which
an intracellular NPA loop and an extracellular NPA loop
project back into the membrane bilayer where their intersection forms a narrow aperture (Jung et al., 1994). This
prediction was confirmed by the shape of the central
density, which consists of two V-shaped regions touching
one another in the center of the AQP1 monomer to form
the density ‘X’ (Walz et al., 1997). At 4.5 Å resolution,
Fig. 2. All water channel proteins shown are isolated as tetramers (arrows) after solubilization of the respective membranes with octyl glucoside.
(A) AQP1 from erythrocyte ghosts (Walz et al., 1994a). (B) AQP0 from ovine lens fiber cells (Hasler et al., 1998). (C) AqpZ from E.coli cells
overexpressing this water channel (Ringler et al., 1999). (D) GlpF from E.coli cells overexpressing the glycerol facilitator (by courtesy of T.Braun,
A.Philippsen and H.Stahlberg, unpublished). Scale bar, 50 nm.
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A.Engel, Y.Fujiyoshi and P.Agre
the central density is now resolved as two short helices
projecting outwards from the center of the monomer,
connected to adjacent helices by loop regions (Mitsuoka
et al., 1999).
Clues from sequence analysis
Multiple sequence alignment and phylogenetic analysis of
164 different sequences of the aquaporin family revealed
two distinct clusters, the AQP and GLP cluster, altogether
comprised of 46 subtypes (Heymann and Engel, 1999).
The core architecture derived from these aligned sequences
consists of six transmembrane helices, two long functional
loops and three interlinking loops of various lengths,
constituting a minimum of 208 residues. While the NPA
motifs of the functional loops are considered to be the
water channel signature, Figure 5 documents many other
equally conserved residues distributed over the entire core
region (Heymann and Engel, 2000). Helices 1 and 4
possess the remarkable pattern ExxxTxxL/F in their
N-terminal half, while helices 3 and 6 show a distinct
helical periodicity along their entire length. Besides the
NPA motifs, many other residues are conserved in the
functional loops, indicating their structural and functional
significance. The His74 in loop B and the Arg195 in
loop E are the highly conserved positively charged buried
residues that may form ion pairs with the conserved buried
glutamic acid residues in helices 1 and 4. In addition,
conserved Gly/Ala residues indicate possible sites of helix–
helix interaction. Measurement of hydrophobic periodicity
and conservation (entropy) periodicity in the alignment of
46 aquaporin subtypes allowed the assignment of helices 3
and 6 to the peripheral helices that face the lipid, and
helices 1 and 4 to the middle helices whose N-terminal
halves face the lipid. The helices close to the 4-fold axis,
H2 and H5, exhibit the lowest periodicity of all the helices
(Figure 4B; Heymann and Engel, 2000).
Major differences between AQPs and GLPs:
residues involved in specificity
Projection maps of unstained two-dimensional crystals
primarily represent the membrane-spanning regions of the
water channel, because the extracellular and cytosolic
connecting loops comprise only a small fraction of the
total mass. Thus, the similarity of such maps (Figure 3)
suggests that the architecture of these proteins, namely
AQP1, AQP0 and AqpZ, is similar within the membrane
core, which houses the six helices and two functional
loops, in agreement with the conclusions from multiple
sequence alignment (Heymann and Engel, 2000). The
major difference between AQPs and GLPs is that loop E
is longer by ~10–15 residues in the latter, but this
difference still needs to be visualized and its functional
implication to be unraveled. The variability of the other
loops and the N- and C-termini is pronounced throughout
the family. This leads to marked differences in the surface
topography of aquaporins, which are determined to subnanometer resolution by atomic force microscopy, as
demonstrated by topographs of AQP1 (Walz et al., 1996),
AqpZ (Scheuring et al., 1999) and AQP0 (D.Fotiadis,
L.Hasler, D.J.Müller, H.Stahlberg, J.Kistler and A.Engel,
manuscript submitted) (Figure 6).
Froger et al. (1998) have proposed to distinguish the
AQPs and the GLPs based on five particular amino acid
residues, called P1–P5 (Figure 5). The position P1 in
general is non-aromatic in the AQP cluster and aromatic
in the GLP cluster. Positions P2 and P3 just follow the
NPAR motif in loop E and form mostly an S–A pair in
the AQP cluster and a D–R or D–K pair in the GLP
cluster, the aspartic acid at P2 being present in all
aquaglyceroproteins sequenced so far. The positions P4
and P5 in helix 6 are mostly aromatic in the AQP cluster,
with P4 usually a proline in the GLP cluster. Unexpectedly,
AQPcic carrying the S–A pair in positions P2 and P3
could be changed to a functional aquaglyceroporin by a
double mutation in P4 and P5 (Lagrée et al., 1999).
Fig. 3. Projection maps of water channel proteins acquired by cryo-electron microscopy and calculated using the MRC software (Crowther et al.,
1996). The maps reveal the structural similarity of the protein core that is embedded in the lipid bilayer and well conserved during sample
preparation in spite of surface tension and interaction with the supporting carbon film. (A) The red cell water channel, AQP1, at 3.5 Å resolution.
AQP1 packs into arrays with P4212 symmetry, housing two tetramers per unit cell of size 96 Å. (B) The lens fiber cell water channel, MIP (AQP0),
at 5.7 Å resolution (D.Fotiadis, L.Hasler, D.J.Müller, H.Stahlberg, J.Kistler and A.Engel, manuscript submitted). AQP0 packs into P4 arrays with a
single tetramer per unit cell of 64 Å side length. The area shown comprises two unit cells. (C) The bacterial water channel, AqpZ, at 8 Å resolution
(Ringler et al., 1999). AqpZ is packed in an up-and-down orientation, as is AQP1, into unit cells of 94 Å width. All projections are viewed from the
cytoplasmic side.
802
Aquaporin water channel protein structures
Fig. 4. The tetrameric arrangement of AQP1 and its molecular architecture is demonstrated three-dimensionally at 6 Å resolution (Walz et al., 1997).
(A) Cytoplasmic view of one unit cell comprising the central tetramer and four monomers in the opposite orientation at the corners. Gaps within the
tetramer indicate the monomer boundary. (B) The helix assignment derived from multiple sequence alignment (Heymann and Engel, 2000) is
different from that proposed in Walz et al. (1997), but compatible with the 4.5 Å map established recently (Mitsuoka et al., 1999). The two NPA
motifs are shown in the middle, and the hydrophobic residues on H1 (F) and H4 (L) are proposed to lie close to the channel (blue circle). (C) At
4.5 Å resolution, the helical nature of a membrane-spanning segment is revealed (Mitsuoka et al., 1999).
Fig. 5. Multiple alignment of 164 AQP/GLP sequences and subsequent phylogenetic analyses yielded 46 subtypes (Heymann and Engel, 1999). To
identify critical residues, the 46 characteristic sequences were aligned and the conservation of each residue calculated (Heymann and Engel, 2000).
Sequence logos, whose heights are a measure of conservation, are drawn with the residue numbers for AQP1. They reveal the conservation patterns
of helices H1–H6 and the highly conserved loops, LB and LE. Helices are grouped in pairs according to the sequence similarity between the first
and second half of the protein. The five positions (P1–P5) that were found by Froger et al. (1998) to be different between the AQP and GLP clusters
are given in italics in circles. Colors: gray, hydrophobic; light blue, polar; green, amide; red, acidic; dark blue, basic.
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A.Engel, Y.Fujiyoshi and P.Agre
are on the same helical face as the conserved glutamic
acid and threonine in helices 1 and 4, and because
positions 24 and 149 are in the middle of these helices,
the leucine and phenylalanine may line the pore. In this
case, these residues could be involved in determining the
size and specificity of the pore.
Structural basis of aquaporin regulation
Fig. 6. Surface topographies of water channel proteins are distinctly
different, reflecting the differences in their sequences that are found
mainly in the helix-connecting loops. Surface reliefs are acquired in
buffer solution by atomic force microscopy. (A) Two-dimensional
crystals assembled from AQP0 tetramers possess a P4 symmetry with
one tetramer per unit cell of 64 Å width (Hasler et al., 1998). Four
bilobed domains protrude by 14 Å from the extracellular surface of
AQP0 (left). They are involved in a ‘tongue and groove’ interaction in
junctions formed by two packed crystal layers (D.Fotiadis, L.Hasler,
D.J.Müller, H.Stahlberg, J.Kistler and A.Engel, manuscript submitted).
The cytoplasmic surface exhibits four domains of 8 Å in height
surrounding a depression about the 4-fold axis (center). Carboxypeptidase Y treatment on mica removes these domains and identifies
them as carboxylic (D.Fotiadis, L.Hasler, D.J.Müller, H.Stahlberg,
J.Kistler and A.Engel, manuscript submitted) (right). (B) AQP1
crystals have a P4212 symmetry and a corrugated extracellular surface
with four protrusions of 12 Å in height (left). The cytosolic surface
with four elongated peripheral and four small central domains produce
a windmill-shaped structure with a height of 6 Å (center). Preliminary
data from carboxypeptidase Y treatment on mica indicate that the
C-terminus is located at a similar position as in AQP0 (D.J.Müller and
A.Engel, unpublished data; right). (C) AqpZ has an extracellular
surface with four elongated peripheral protrusions and four central
protrusions of 7 Å in height (left). The poly-His tag used for
purification produces a massive protrusion on the cytosolic surface
(center). After trypsin cleavage, the cytosolic surface exhibits four
small protrusions (right). The elongated extracellular protrusion in
AqpZ has been identified as loop C based on its volume and flexibility
(Scheuring et al., 1999). Correlation averages displayed comprise two
tetramers and have a side length of ~95 Å. Horizontal and vertical
scaling are identical, but the gray level range is adapted to go from
black to full white within each topograph.
Further clues are found in the more recent sequence
analysis by Heymann and Engel (2000), who identified
two critical conserved hydrophobic residues in the middle
of helices 1 and 4. As shown in Figure 5, these are either
a phenylalanine or a leucine in position 24, or mostly a
leucine in position 149. In 17 out of 21 GLP subfamilies,
these positions harbor the L–L pair; in two subfamilies it
is an M–L pair. In contrast, 16 out of 28 AQP subfamilies
exhibit an F–L, F–M or L–F pair, while AQP0, AQP6
and BIB_DROME have a tyrosine in position 24. However,
seven AQPs possess the L–L pair characteristic for GLPs.
Among them are three plant water channels (NIPs), two
archaeal AQPs and two fly AQPs, the latter including
AQPcic. Because the two conserved hydrophobic residues
804
The significance of structural studies is greatly amplified
by evidence emerging from multiple laboratories that
aquaporins are directly regulated. While aquaporins are
found in virtually all life forms, the mammalian homologs
have received greatest attention due to their relevance
to disease.
At least three mammalian aquaporins appear to be
regulated directly by pH. Thus, structural pH sensors must
reside in these proteins. Naturally occurring mutations in
the gene encoding mouse AQP0 result in congenital
cataracts (Shiels and Bassnett, 1996), and preliminary
evidence indicates that the low baseline water permeability
of AQP0 becomes activated at pH 6.5 (Cahalan and Hall,
1999). AQP3 is expressed in basolateral membranes of
water-reabsorbing principal cells in the renal collecting
duct, airway epithelia and secretory glands. AQP3 is
permeated by water and glycerol at neutral pH, but the
channel appears gated shut at pH ⬍6 (Zeuthen and Klaerke,
1999). AQP6 resides in acid-secreting intercalated cells
of the renal collecting duct (Yasui et al., 1999a) and
undergoes a conformational change at pH ⬍5.5 during
which the channel opens for selective permeation by water
and chloride ions (Yasui et al., 1999b). AQP0 and AQP6
are AQPs, both possessing a tyrosine at position 24 instead
of a leucine, implying a role for Tyr24 in the regulation
of the channel. However, AQP3 is a typical GLP exhibiting
the characteristic L–L pair, suggesting that different mechanisms of pH-driven regulation must exist. Interestingly,
pH-induced conformational changes related to channel
closure at pH 3 have also been observed with the bacterial
porin OmpF (Müller and Engel, 1999).
Phosphorylation of specific residues in certain aquaporins may induce protein trafficking or channel gating.
AQP2 is expressed in collecting duct principal cells and
contains a protein kinase A phosphorylation consensus at
the C-terminus (Fushimi et al., 1993). In response to
vasopressin, AQP2 migrates from intracellular membrane
vesicles to the apical membrane, thereby raising the
surface water permeability (Nielsen et al., 1995). The
gene encoding AQP2 contains mutations in some forms
of nephrogenic diabetes insipidus (Deen et al., 1994), and
AQP2 expression is perturbed in several other disorders
of either water loss or water retention (reviewed by
Marples et al., 1999). Although previously thought to be
constitutively active, AQP1 may traffic from intracellular
sites to the plasma membrane in cultured cholangiocytes
stimulated with secretin (Marinelli et al., 1999). Square
arrays of AQP4 proteins reside in astroglial end-feet where
water crosses the blood–brain barrier (Rash et al., 1998).
Interestingly, protein kinase C agonists (phorbol esters)
were found to inactivate the water permeability of AQP4
expressed in oocytes (Han et al., 1998). In plants, the
regulation of water flow is a crucial task. The water activity
of the vacuolar membrane aquaporin α-TIP (Maurel, 1995)
Aquaporin water channel protein structures
as well as that of the plant plasma membrane aquaporin
PM28A is regulated by phosphorylation (Johansson
et al., 1998).
Recently, the possibility of direct binding of aquaporins
to other proteins has been proposed. Recognition of the
PDZ consensus at the C-terminus of AQP4 suggests that
a cytoskeletal linkage may determine the highly polarized
distribution within astroglia (Nagelhus et al., 1999). The
exciting finding of specific inactivation of the lacrymal
gland AQP5 by protein agonists suggests a new molecular
approach to regulating tear formation (N.Ishida and
M.Mita, personal communication).
Conclusions and perspectives
These studies underscore the need to determine the
structure of aquaporins and aquaglyceroporins at high
resolution. It is essential that structural landmarks be
established in aquaporin proteins, since these ultimately
may be used to develop therapeutic agents for important
clinical disorders. Three-dimensional maps from electron
crystallographic analyses now approach a sufficient resolution to build an atomic model, and highly ordered
two-dimensional crystals of AQP0, AQP1, AqpZ, α-TIP
(Daniels et al., 1999) and GlpF (T.Braun, A.Philippsen and
H.Stahlberg, personal communication) are now available.
This and the three-dimensional crystals of AQP1 (Wiener,
1999) promise that this goal should be reached soon.
Meanwhile, we may speculate as to how the channel
might work based on the 4.5 Å density map of AQP1
(Mitsuoka et al., 1999), data derived from sequence
analyses (Heymann and Engel, 2000) and measurements
of water mobility by NMR spectroscopy. Size exclusion
is likely to be an important aspect of specificity, which
could be provided by the hydrophobic F–L pairs in AQPs
and the L–L pairs in GLPs. The question arises of whether
the pore exhibits altogether a hydrophobic surface. From
NMR measurements taken at different temperatures, the
activation energy for water displacement in non-polar
surface pockets of RNase A (Denisov and Halle, 1998)
and in the minor groove of a B-DNA duplex (Denisov
et al., 1997) has been estimated as 10 and 13 kcal/mol,
respectively. This is compatible with the activation energy
Ea ⬎10 kcal/mol for the diffusion of water through pure
lipid bilayers, but incompatible with the osmotically driven
water flux that can amount to two water molecules
per channel and nanosecond. The activation energy for
movement of water molecules in bulk water, 5 kcal/mol,
is close to the activation energy measured for passage of
water in aquaporins. This suggests that some polar residues
or main chain carbonyls in the vicinity of the pore facilitate
a water hydrogen-bonding network. Such polar sites are
also required to interrupt hydrogen bonds in a single file
of water molecules to prevent the creation of a ‘proton
wire’ (Pomès and Roux, 1996). Water molecules may thus
tumble from one set of tetrahedral hydrogen bonds to the
next and pass through the channel without noticing it.
Acknowledgements
The authors gratefully acknowledge the expert help of Drs L.Hasler,
J.B.Heymann, K.Mitsuoka, S.A.Müller and H.Stahlberg, and of T.Braun,
D.Fotiadis and S.Scheuring. Unpublished micrographs have been kindly
provided by J.Kistler (Figure 1) and T.Braun (Figure 2D). The work
was supported by the Swiss National Foundation for Scientific Research,
the National Heart, Lung, and Blood Institute of the NIH, and the
Maurice E.Müller Foundation of Switzerland.
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Received June 9, 1999; revised and accepted January 12, 2000