8.5 The Myosin II Motor of Muscle Contraction, a Representative ATPase
439
8.53 and 8.54, the hydrophobic consiUent mech-
anism provides an explanation of the physical
basis for this movement.
Another feature of this perspective involves
the apparent stretching of a chain segment, as
labeled in Figure 8.52. The elastic force result-
ing from such an extension derives from the
elastic consihent mechanism. As will be argued
below, hydrophobic association gives rise to
the development of a functional elastic force.
Such a perspective may become a classic
demonstration in protein-based machines, as it
has been seen in Complex III of the electron
transport chain and in the repulsive aspect of
the comprehensive hydrophobic effect causing
an elastic deformation during functioning of
ATP synthase/Fi-ATPase.
8.5.4.4 Hydrophobic
Association/Dissociation of the Head of
the Lever Arm and the Amino-terminal
Domain
Figure 8.53 shows stereo views of the scallop
muscle cross-bridge, absent the Ught
chains,
that
were oriented to better characterize the nature
of the association (in the near-rigor state) and
the dissociation (in the ATP bound state)
involving the head of the lever arm and the
amino-terminal domain. The stereo views help
to show that the association in Figure 8.53A,C
is hydrophobic, whereas the proximal surfaces
of the head of the lever arm and amino-
terminal domain in Figure 8.53B,D are domi-
nated by charged residues.
Enlarged views of the relationship between
the amino-terminal domain and the head of the
lever arm, shown in stereo in Figure 8.53, are
given in Figure 8.54 for the purpose of better
seeing the interacting residues in the associated
near-rigor state. On the left side of the figure
the association is hydrophobic, with, as seen in
the stereo view of Figures 8.53A, the lower
charged part between the domains having
twisted sUghtly out of
co-planarity.
On the other
hand, the ATP analogue state is dissociated
with a preponderance of charged (white)
residues separating the two surfaces.
The explanation for the structural transition
between the near-rigor and ATP bound states
is given in section
8.5.4.7
(with the assistance
of Figures 8.58 and 8.59). First, however, two
issues require discussion before this pair of
states can be considered models for producing
the motion of muscle contraction. One issue
involves a closer examination of the stretched/
relaxed chain segment of Figure 8.52 in order
to see if this chain segment can provide an
example of elastic force development that
results from hydrophobic association demon-
strated in Figures 8.53 and 8.54. The pair of
structures to be of greater significance should
provide an understanding of force develop-
ment, as required to explain isometric con-
traction and to understand energy-efficient
production of motion. The second issue is how
effectively the two structures demonstrate the
displacement required for the sliding filament
mechanism of muscle contraction.
8.5.4.5 Evidence for Elastic Force
Development Resulting from
Hydrophobic Association
8.5.4.5.1
Stretching the Relay Loop on
Hydrophobic Association of the Head of the
Lever Arm and the Amino-terminal Domain
The suggestion of a stretched chain segment is
shown in Figure
8.52.
An optimized perspective
for considering this potential source of elastic
force development is given in Figure 8.55. The
estimate of length change uses the change of
ratios of the relay loop segment I505-D511 to
the relay helix segment Y500-F472 that accom-
panies the change of states at the nucleotide
binding
site.
There appears to be an extension of
as much as
40%
accompanying the hydrophobic
association resulting from loss of phosphate (or
equivalent) from the nucleotide binding site.
8.5.4.5.2
Presence of a Number of Flexible
Loops for Potential Storage of Elastic Force
By the elastic consihent mechanism the
extension of single flexible loops causes an
increase in the elastic force. It appears that one
such loop has been identified in Figure 8.55.
Rayment et al.^^"^ note a number of flexible
loops in the myosin cross-bridge. Each of
these becomes a candidate for elastic force