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Compare and contrast the mechanisms of excitation-contraction coupling in skeletal, cardiac, and smooth muscle cells.
For skeletal muscle, describe:
How movement of a voltage sensor couples sarcolemmal depolarization to the opening of SR Ca 2+ release channels.
The source of the Ca 2+ required for the activation of contraction.
What happens to the Ca 2+ to effect relaxation.
Describe how cardiac muscle is activated by Ca 2+ ions in the process known as Ca 2+ -induced Ca 2+ release (CICR) .
Describe the roles of SERCA, the Na + /Ca 2+ exchanger (NCX), and the plasma membrane Ca 2+ pump (PMCA) in the relaxation of cardiac muscle.
Explain how diverse smooth muscles can be activated by depolarization or by agonists through a process known as pharmacomechanical coupling.
Explain the roles of the inositol trisphosphate receptors (IP 3 Rs) and ryanodine receptors (RyRs) in smooth muscle.
Skeletal muscle fibers are innervated by α motor neurons, which are large neurons (cell body diameter up to 70 μm) that originate in the ventral horn of the spinal cord. As discussed in Chapter 12 , a single AP in an α motor neuron causes sufficient ACh release at a single NMJ to trigger an AP that is propagated along an entire muscle fiber.
Skeletal muscle contraction is triggered by depolarization of the muscle fiber membrane beyond a critical level, the mechanical threshold. Under normal physiological conditions an AP causes this depolarization. The relationship between V m and the amount of force, or “tension,” generated by skeletal muscle is presented in Fig. 15.1 . The mechanical responses shown in Fig. 15.1 , which are produced by depolarizations lasting several seconds, are called contractures . As V m becomes more positive than approximately –55 mV (the mechanical threshold), force increases very steeply with further depolarization. The mechanism by which depolarization of the sarcolemma causes contraction of the muscle cell is termed excitation-contraction coupling (E-C coupling) . The fact that force increases with V m indicates that the process of E-C coupling involves a voltage sensor in the sarcolemma that couples depolarization to contraction.
In skeletal muscle, the resting V m (∼–90 mV) is much more negative than in neurons (∼–70 mV) owing to the relatively high permeability of the sarcolemma to both K + and Cl − . Because of the high resting Cl − permeability, a relatively large stimulus is normally necessary to bring the V m to mechanical threshold. In some skeletal muscle diseases, loss-of-function mutations in skeletal muscle Cl − channels drastically reduce the Cl − permeability of the sarcolemma. As a result, the skeletal muscle AP threshold can be reached more easily and the muscle becomes hyperexcitable ( Box 15.1 ).
Two inherited forms of nondystrophic myotonia congenita a involve the Cl − conductance ( g Cl ) of the skeletal muscle sarcolemma: Thomsen’s disease, with autosomal dominant inheritance; and the more severe Becker’s myotonia, with autosomal recessive inheritance. Both forms are characterized by attacks of muscle stiffness caused by a delay in muscle relaxation after stimulation. Under conditions in which normal muscle responds with a single action potential (AP), myotonic muscle cells respond to a single stimulation with repetitive APs. Thus a single α motor neuron AP evokes a twitch in normal skeletal muscle but a tetanus in myotonic muscle. A tetanus is a sustained contraction that is evoked in normal skeletal muscle only when it is stimulated by a train, or burst, of closely spaced APs ( Chapter 16 ). The rigidity and delayed relaxation of myotonic muscle are caused by the tetanic response to a single stimulus.
The hyperexcitability of myotonic muscle is caused by a mutation in the gene encoding the predominant skeletal muscle Cl − channel, CLCN1. This mutation reduces the Cl − conductance ( g Cl ) of the sarcolemma and, thus, increases membrane resistance. A stimulus will produce a larger change in V m in myotonic muscle than in normal muscle (see Ohm’s Law in Chapter 6 ). As a result, the current required to reach AP threshold is less, thereby making the muscle hyperexcitable.
The temporal relationship between the skeletal muscle AP and the force generated by the muscle is illustrated in Fig. 15.2 . The skeletal muscle AP is similar to the nerve axon AP ( Chapter 7 ) in that it is generated by the activity of voltage-gated Na + and K + channels. The development of force by the myocyte begins several milliseconds after the AP. The transient contraction produced by a myocyte in response to a single AP is called a twitch . During the twitch, the contractile force rises to a peak in 30 to 50 milliseconds and then declines over the next 50 to 100 milliseconds. The duration of the twitch is approximately 100-fold longer than the duration of the AP.
In Chapter 14 we learned that an increase in [Ca 2+ ] i activates contraction in all types of muscle cells. Therefore the central question in E-C coupling is, “How does depolarization of the sarcolemma bring about an increase in [Ca 2+ ] i ?” A related, but more subtle, question is, “How does the [Ca 2+ ] i increase fast enough throughout the muscle fiber so that myofibrils deep inside the fiber can contract synchronously with those close to the surface?”
Is diffusion of a soluble factor from the surface membrane (e.g., Ca 2+ ions entering the cell through voltage-gated Ca 2+ channels) to the interior of the cell sufficiently fast to explain the rapid activation of skeletal muscle? A molecule would take about a second to diffuse to the center of a 100-μm diameter skeletal muscle cell ( Chapter 2 ). This is much too slow to account for the development of force during a twitch contraction, which begins just a few milliseconds after the AP ( Fig. 15.2 ).
How, then, does the AP in the sarcolemma rapidly activate the myofibrils in the center of the cell? The critical clue was the discovery that “hot spots” distributed over the sarcolemma (later shown to be T-tubule openings) provide a pathway for depolarization to spread from the surface into the interior of the fiber. T-tubules form an intricate network that extends throughout the skeletal muscle cell ( Fig. 15.3 ). Thus the T-tubule lumen is a narrow extension of the extracellular space into the interior of the muscle cell. The T-tubule membrane contains voltage-gated Na + and K + channels, and APs from the surface are propagated along the T-tubule membrane into the interior of the cell.
The T-tubule membrane of skeletal muscle contains receptors for the dihydropyridine derivatives that block L-type voltage-gated Ca 2+ channels ( Chapter 8 ). Voltage clamp studies in skeletal muscle demonstrate that inward Ca 2+ currents are generated by depolarization ( Fig. 15.4 ) and that these currents are blocked by dihydropyridines. Thus the dihydropyridine receptors (DHPRs) in the T-tubule membrane are L-type Ca 2+ channels. Therefore we might reasonably expect that the Ca 2+ entry through these channels raises [Ca 2+ ] i and activates contraction, but this is not the case. Skeletal muscle continues to contract normally when bathed in a solution containing no Ca 2+ ions. This finding indicates that Ca 2+ entry is not essential for skeletal muscle contraction and that all the Ca 2+ required for activating the contractile machinery is derived from intracellular sources. This is in marked contrast to the mechanism of E-C coupling in cardiac muscle, where Ca 2+ entry through voltage-gated Ca 2+ channels is required (see later). Even though Ca 2+ entry through DHPRs is not required for E-C coupling in skeletal muscle, the DHPRs do play a crucial role in this mechanism.
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