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Molecular Biology of the Cell by Bruce Alberts, Alexander Johnson, Julian Lewis, David Morgan, Martin Raff, Keith Roberts, Peter Walter by by Bruce Alberts, Alexander Johnson, Julian Lewis, David Morg

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918 Chapter 16: The Cytoskeleton

(A)

(B)

displacement

bead

X

50 nm

50 nm

Y

0

position

detector

actin

myosin

1 2 3 4 5 6

time (sec)

optical tweezers

development by the fusion of many separate cells. The large muscle cell retains

the many nuclei of the contributing cells. These nuclei lie just beneath the plasma

membrane (Figure 16–31). The bulk of the cytoplasm inside is made up of myofibrils,

which is the name given to MBoC6 the basic n16.303/16.30 contractile elements of the muscle cell.

A myofibril is a cylindrical structure 1–2 μm in diameter that is often as long as

the muscle cell itself. It consists of a long, repeated chain of tiny contractile units—

called sarcomeres, each about 2.2 μm long—which give the vertebrate myofibril its

striated appearance (Figure 16–32).

Each sarcomere is formed from a miniature, precisely ordered array of parallel

and partly overlapping thin and thick filaments. The thin filaments are composed

of actin and associated proteins, and they are attached at their plus ends to a Z

disc at each end of the sarcomere. The capped minus ends of the actin filaments

extend in toward the middle of the sarcomere, where they overlap with thick filaments,

the bipolar assemblies formed from specific muscle isoforms of myosin

II (see Figure 16–27). When this region of overlap is examined in cross section by

electron microscopy, the myosin filaments are arranged in a regular hexagonal

lattice, with the actin filaments evenly spaced between them (Figure 16–33). Cardiac

muscle and smooth muscle also contain sarcomeres, although the organization

is not as regular as that in skeletal muscle.

Figure 16–30 The force of a single

myosin molecule moving along an

actin filament measured using an

optical trap. (A) Schematic of the

experiment, showing an actin filament

with beads attached at both ends and held

in place by focused beams of light called

optical tweezers (Movie 16.4).

The tweezers trap and move the bead,

and can also be used to measure the

force exerted on the bead through the

filament. In this experiment, the filament

was positioned over another bead to

which myosin II motors were attached,

and the optical tweezers were used to

determine the effects of myosin binding

on movement of the actin filament.

(B) These traces show filament movement

in two separate experiments. Initially, when

the actin filament is unattached to myosin,

thermal motion of the filament produces

noisy fluctuations in filament position. When

a single myosin binds to the actin filament,

thermal motion decreases abruptly and a

roughly 10-nm displacement results from

movement of the filament by the motor. The

motor then releases the filament. Because

the ATP concentration is very low in this

experiment, the myosin remains attached

to the actin filament for much longer than

it would in a muscle cell. (Adapted from

C. Rüegg et al., Physiology 17:213–218,

2002. With permission from the American

Physiological Society.)

Figure 16–31 Skeletal muscle cells (also called muscle fibers). (A) These

huge multinucleated cells form by the fusion of many muscle cell precursors,

called myoblasts. Here, a single muscle cell is depicted. In an adult human,

a muscle cell is typically 50 μm in diameter and can be up to several

centimeters long. (B) Fluorescence micrograph of rat muscle, showing the

peripherally located nuclei (blue) in these giant cells. Myofibrils are stained

red. (B, courtesy of Nancy L. Kedersha.)

(A)

nucleus

myofibril

(B)

50 µm

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