S-60 Chapter 5 Protein Function
(a) Reversible binding of a ligand to a simple protein, without cooperativity. For Equation 5–8, set up
a plot of vversus [L] (vertical and horizontal axes, respectively). Examine the plots generated
when K
d
is set at 5, 10, 20, and 100 m
M
. Higher affinity of the protein for the ligand means more
binding at lower ligand concentrations. Suppose that four different proteins exhibit these four
different K
d
values for ligand L. Which protein would have the highest affinity for L?
Examine the plot generated when K
d
⫽10 m
M
. How much does vincrease when [L] increases
from 0.2 to 0.4 m
M
? How much does vincrease when [L] increases from 40 to 80 m
M
?
You can do the same exercise for Equation 5–11. Convert [L] to pO
2
and K
d
to P
50
. Examine
the curves generated when P
50
is set at 0.5, 1, 2, and 10 kPa. For the curve generated when
P
50
⫽1 kPa, how much does vchange when the pO
2
increases from 0.02 to 0.04 kPa? From 4 to
8 kPa?
(b) Cooperative binding of a ligand to a multisubunit protein. Using Equation 5–14, generate a bind-
ing curve for a protein and ligand with K
d
⫽10 m
M
and n⫽3. Note the altered definition of K
d
in
Equation 5–16. On the same plot, add a curve for a protein with K
d
⫽20 m
M
and n⫽3. Now see
how both curves change when you change to n⫽4. Generate Hill plots (Eqn 5–16) for each of
these cases. For K
d
⫽10 m
M
and n⫽3, what is vwhen [L] ⫽20 m
M
?
(c) Explore these equations further by varying all the parameters used above.
Answer
Data Analysis Problem
17. Protein Function During the 1980s, the structures of actin and myosin were known only at the resolu-
tion shown in Figure 5–28a, b. Although researchers knew that the S1 portion of myosin binds to actin
and hydrolyzes ATP, there was a substantial debate about where in the myosin molecule the contractile
force was generated. At the time, two competing models were proposed for the mechanism of force gen-
eration in myosin.
In the “hinge” model, S1 bound to actin, but the pulling force was generated by contraction of the
“hinge region” in the myosin tail. The hinge region is in the heavy meromyosin portion of the myosin
molecule, near where trypsin cleaves off light meromyosin (see Fig. 5–27b). This is roughly the point
labeled “Two supercoiled ␣helices” in Figure 5–27a. In the “S1” model, the pulling force was gener-
ated in the S1 “head” itself and the tail was just for structural support.
Many experiments had been performed but provided no conclusive evidence. In 1987, James Spu-
dich and his colleagues at Stanford University published a study that, although not conclusive, went a
long way toward resolving this controversy.
Recombinant DNA techniques were not sufficiently developed to address this issue in vivo, so Spudich
and colleagues used an interesting in vitro motility assay. The alga Nitella has extremely long cells, often sev-
eral centimeters in length and about 1 mm in diameter. These cells have actin fibers that run along their long
axes, and the cells can be cut open along their length to expose the actin fibers. Spudich and his group had
observed that plastic beads coated with myosin would “walk” along these fibers in the presence of ATP, just as
myosin would do in contracting muscle.