The diameter of the actin filament decreases with an increase of the p
rotein osmotic pressure. This phenomenon is accompanied by a decrease
of the angle (a) formed between the long axis of the actin monomer and
the pointed end of the filament axis. At 1.8 x 10(5) dyn/cm(2) (the p
rotein osmotic pressure in frog muscle) the diameter is 8.34 nm and th
e angle (a) is 61.5 degrees. The interfilament distance of tropomyosin
-decorated actin filaments, at a set of different osmotic pressures, i
s larger than that of F-actin filaments. This suggests that the two tr
opomyosin helices project out of the contour of the actin filament. Th
e tropomyosin-decorated actin filament is more rigid than F-actin. At
1.8 x 10(5) dyn/cm(2), the angle (a) is 76.4 degrees, as compared to t
he value of 61.5 degrees for F-actin. The interfilament distance of tr
oponin-tropomyosin-decorated actin filaments is sensitive to Ca2+: in
the physiological range of protein osmotic pressure it decreases from
13.3 nm, in the presence of 2 mM EGTA, to 12.2 nm in the presence of 0
.2 mM CaCl2. Two alternative models are proposed to explain the decrea
se in interfilament distance. (a) Calcium shifts tropomyosin along the
actin monomer, toward the filament axis (the classical model). (b) Ca
lcium releases the rigidity of the tropomyosin-decorated filament and
restores the original plasticity of F-actin. The consequent decrease o
f the angle (alpha) brings the tropomyosin helices nearer to the filam
ent axis, without any real movement of tropomyosin along the actin mon
omer.