NATURE CHEMICAL BIOLOGY | VOL 6 | DECEMBER 2010 | www.nature.com/naturechemicalbiology 891
ARTICLE
PUBLISHED ONLINE: 24 OCTOBER 2010 | DOI: 10.1038/NCHEMBIO.457
F
-type ATP synthases are large multisubunit complexes that use
the energy stored in electrochemical gradients of H
+
(ref. 1)
or Na
+
(ref. 2) for the synthesis of ATP, the universal chemi-
cal energy source of living cells. The enzyme is composed of two
structurally and functionally distinct parts; the catalytic F
1
complex
(subunits α
3
β
3
γδε) and the membrane-embedded F
o
complex (for
example, subunits ab
2
c
10–15
in bacteria), which conducts ions across
the membrane. The mechanism of the enzyme entails the rotation of
a subset of subunits against the others
3
; these are collectively known
as the rotor (γεc
10–15
) and stator subcomplexes (α
3
β
3
δab
2
). In ATP
synthesis mode, the downhill movement of ions causes the rotation
of the c-subunit assembly in F
o
, and therefore of subunit γ as well.
This γ-subunit, referred to as the central stalk, protrudes into the
α
3
β
3
assembly in F
1
(ref. 4); its rotation drives a cycle of conforma-
tional changes within the catalytic β-subunits
5
, finally resulting in
ATP synthesis and release. Conversely, F
1
can convert the chemical
energy derived from ATP hydrolysis into a torque that drives the F
o
motor to act as an ion pump, in analogy with the related family of
V
1
V
o
ATPases
6
.
The c-subunit assembly in F
o
, known as the c-ring, is thus the key
element that transduces the electrochemical energy into mechanical
rotation and vice versa. It consists of a species-dependent number
of c-subunits
7,8
and adopts a cylinder-like shape with a central, lipid-
plugged pore. High-resolution crystal structures of the Na
+
-coupled
c
11
ring from Ilyobacter tartaricus
9,10
and the K
10
ring from Enterococcus
hirae
11
, and of the H
+
-coupled c
15
ring from Spirulina platensis
12
and the
c
13
ring from Bacillus pseudofirmus OF4 (ref. 13) have been obtained.
In all structures the ion-binding sites are located near the outer surface
of the ring, facing the hydrophobic acyl-chain layer of the membrane.
The ions bind to grooves formed between adjacent c-subunits and
establish a precise network of interactions; a strictly conserved carbox-
ylate residue is the key ligand for both Na
+
and H
+
. In these structures,
the binding sites are observed in the ion-locked state
9,12,13
.
The microscopic mechanism by which ion translocation across
the F
o
complex is coupled to the rotation of the c-ring is not known.
Nonetheless, it is widely accepted that two independent, discon-
nected access pathways probably exist at the interface of the c-ring
and the a-subunit or within the latter, which allow H
+
or Na
+
ions
to bind to or be released from the c-subunit rotor. The bound ions
would be shuttled from one access channel to the other as the
c-ring rotates around its central axis, effectively completing the ion
pathway across the membrane
14,15
. The underlying principle of this
mechanism is that the occupancy of the binding sites in the c-ring
is dependent on the chemical environment they face at a given time.
As protons (or Na
+
) are shuttled within the membrane core by the
rotating ring, they remain tightly bound to the c-ring. By contrast,
the environment of the a-subunit enables these binding sites to load
and release ions from and to the access channels, through a mecha-
nism that has not been characterized in detail. This is partly because
of the lack of a high-resolution structure of the a-subunit and its
interface with the c-ring. Nevertheless, biochemical data have
established two important facts: first, that the a-subunit harbors a
strictly conserved arginine, whose guanidine group is believed to
have a central role as an electrostatic separator between these access
pathways
14,15
, and second, that the a-c interface is locally hydrated
from the cytoplasmic side to the membrane middle, as evidenced by
solvent-accessibility measurements specific to this region
16
. Lately,
electron microscopy data on a related V-type ATPase
17
has indi-
cated that the contact interface of subunit a and the c-ring (or their
equivalent) is indeed rather minimal and that it appears to include
not only water but lipids as well.
In this work we use experimental and theoretical methods to
show how these essential features give rise to a mechanism of envi-
ronmental control of the ion occupancy of the c-subunit and thus
to the ion-coupled rotary mechanism within the F
o
domain. As sup-
porting evidence, we provide three atomic-resolution structures of
the H
+
-coupled c
15
ring rotor from S. platensis, together with a sys-
tematic, quantitative DCCD–modification assay and detailed free-
energy molecular-dynamics calculations. Our results support the
view that the membrane and a-subunit environments influence the
1
Department of Structural Biology, Max Planck Institute of Biophysics, Frankfurt am Main, Germany.
2
Theoretical Molecular Biophysics Group, Max Planck
Institute of Biophysics, Frankfurt am Main, Germany.
3
Department of Molecular Membrane Biology, Max Planck Institute of Biophysics, Frankfurt am Main,
Germany.
4
Cluster of Excellence Macromolecular Complexes, Frankfurt am Main, Germany.
5
These authors contributed equally to this work.
*e-mail: thomas.meier@biophys.mpg.de or jose.faraldo@biophys.mpg.de
Microscopic rotary mechanism of ion
translocation in the F
o
complex of ATP synthases
Denys Pogoryelov
1
, Alexander Krah
2
, Julian D Langer
3
, Özkan Yildiz
1
, José D Faraldo-Gómez
2,4,5
* &
Thomas Meier
1,4,5
*
The microscopic mechanism of coupled c-ring rotation and ion translocation in F
1
F
o
-ATP synthases is unknown. Here we present
conclusive evidence supporting the notion that the ability of c-rings to rotate within the F
o
complex derives from the interplay
between the ion-binding sites and their nonhomogenous microenvironment. This evidence rests on three atomic structures of
the c
15
rotor from crystals grown at low pH, soaked at high pH and, after N,N′-dicyclohexylcarbodiimide (DCCD) modification,
resolved at 1.8, 3.0 and 2.2 Å, respectively. Alongside a quantitative DCCD-labeling assay and free-energy molecular dynamics
calculations, these data demonstrate how the thermodynamic stability of the so-called proton-locked state is maximized by
the lipid membrane. By contrast, a hydrophilic environment at the a-subunit–c-ring interface appears to unlock the binding-site
conformation and promotes proton exchange with the surrounding solution. Rotation thus occurs as c-subunits stochastically
alternate between these environments, directionally biased by the electrochemical transmembrane gradient.
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