articlesThe building block of synaptic transmission is the quantum, the minimal increment of postsynaptic signals 1 . At vertebrate neuromuscular junctions, the quantum may be equated with spontaneous signals obtained in the absence of presynaptic action potentials, called miniature currents (or potentials) and believed to be due to release of one neurotransmitter vesicle. For central synapses, this issue remains an open question, as large miniature currents are suggested to arise from the concerted release of several presynaptic vesicles and to be the sum of several quanta 2-5 . Such multivesicular miniature events could reflect tetrodotoxinresistant action potentials in presynaptic terminals 6 . Another explanation comes from evidence for functional intracellular Ca 2+ stores in presynaptic terminals. First, inositoltrisphosphate (InsP 3 ) receptors are immunolocalized in presynaptic terminals of the deep cerebellar nuclei and retina 7,8 . Second, at the frog neuromuscular junction, agents that affect ryanodine-sensitive Ca 2+ stores also regulate presynaptic intracellular Ca 2+ (Ca 2+ i ) rises and acetylcholine release during high-frequency stimulation 9,10 . Third, action-potential-evoked release of acetylcholine at synapses in Aplysia buccal ganglia is inhibited by ryanodine and augmented by presynaptic injection of cyclic ADP ribose 11 . Fourth, caffeine and/or ryanodine modify presynaptic Ca 2+ i signals in autonomic ganglia 12,13 and in photoreceptors 14 . Finally, in hippocampal pyramidal cells, caffeine or thapsigargin can increase the frequency of miniature IPSCs 15 . Hence, spontaneous Ca 2+ release from presynaptic Ca 2+ stores may provide the synchronization mechanism that leads to multivesicular miniatures. However, except for one study that gave negative results in cultured retinal amacrine cells 16 , this possibility has not been tested systematically.To assess the contribution of intracellular Ca 2+ stores to neurotransmitter release, we monitored the amplitude distribution of miniature synaptic currents while manipulating potential presynaptic Ca 2+ stores. Using cerebellar interneuron-Purkinje cell synapses, in which large miniature synaptic currents are prominent, we found that the largest mIPSCs result from multivesicular release and depend on Ca 2+ mobilization from ryanodine-sensitive presynaptic stores. Further, two-photon confocal microscopy showed ryanodine-sensitive intracellular Ca 2+ i transients highly localized to presumed release sites, which may underlie large miniature currents. RESULTSMiniature IPSCs recorded in cerebellar Purkinje cells, at -60 mV under symmetrical Cl -concentrations and in the presence of tetrodotoxin (TTX) and ionotropic glutamate receptor blockers, showed mean amplitudes of 125 ± 9 pA (n = 28 cells), larger than for most neurons (Fig. 1a). Amplitude histograms had a distinct peak for values less than 200 pA, followed by a long tail with amplitudes up to 1500 pA (Fig. 1b). Spurious summation of independent events did not contribute to the generation of lar...

1. The fluorescent dye fluo-3, in its permeant acetoxymethyl form, was used to monitor calcium transients during twitch and tetanus of single fibres isolated from the anterior tibialis muscle of Rana temporaria (2-5°C 6. The results strongly suggest that the non-uniform length changes that are known to occur along a muscle fibre during relaxation enhance the release of calcium from the contractile system. The calcium mobilized in this way probably accounts for the transitory increase of [Ca2+], that is observed during the latter part of force relaxation.

First coined by Alexander Sandow in 1952, the term excitation-contraction coupling (ECC) describes the rapid communication between electrical events occurring in the plasma membrane of skeletal muscle fibres and Ca 2+ release from the SR, which leads to contraction. The sequence of events in twitch skeletal muscle involves: (1) initiation and propagation of an action potential along the plasma membrane, (2) spread of the potential throughout the transverse tubule system (T-tubule system), (3) dihydropyridine receptors (DHPR)-mediated detection of changes in membrane potential, (4) allosteric interaction between DHPR and sarcoplasmic reticulum (SR) ryanodine receptors (RyR), (5) release of Ca 2+ from the SR and transient increase of Ca 2+ concentration in the myoplasm, (6) activation of the myoplasmic Ca 2+ buffering system and the contractile apparatus, followed by (7) Ca 2+ disappearance from the myoplasm mediated mainly by its reuptake by the SR through the SR Ca 2+ adenosine triphosphatase (SERCA), and under several conditions movement to the mitochondria and extrusion by the Na + /Ca 2+ exchanger (NCX). In this text, we review the basics of ECC in skeletal muscle and the techniques used to study it. Moreover, we highlight some recent advances and point out gaps in knowledge on particular issues related to ECC such as (1) DHPR-RyR molecular interaction, (2) differences regarding fibre types, (3) its alteration during muscle fatigue, (4) the role of mitochondria and store-operated Ca 2+ entry in the general ECC sequence, (5) contractile potentiators, and (6) Ca 2+ sparks.

SUMMARY1. The time course of potassium contractures can be significantly prolonged by low concentrations of caffeine.2. This effect of caffeine is not due to impairment of the fibre relaxing system.3. Under conditions where contractile repriming is delayed (low temperature) an extra amount of activator can be released by caffeine, in addition to that released by potassium.4. The source of this extra amount of activator is intracellular since its release can be shown in a 0 calcium EGTA medium.5. Local anaesthetics, tetracaine, and to a lesser extent procaine, affect the release of contractile activator, without impairing the contractile machinery itself.6. The results of the present paper support the view that the time course of potassium contracture is controlled by a membrane mechanism which is activated upon depolarization and later inactivates with time.7. The effect of caffeine and local anaesthetics can be explained by assuming that the former prolongs the inactivation time course while the latter shortens it.

The relationship between force and velocity of shortening was studied during fused tetani of single fibres isolated from the anterior tibialis muscle of Rana temporaria (1.5–3.3°C; sarcomere length, 2.20 mm). Stiffness was measured as the change in force that occurred in response to a 4 kHz length oscillation of the fibre. The results confirmed the existence of two distinct curvatures of the force–velocity relationship located on either side of a breakpoint in the high‐force, low‐velocity range. Reduction of the isometric force (P0) to 83.4 ± 1.7% (mean ±s.e.m., n= 5) of the control value by dantrolene did not affect the relative shape of the force–velocity relationship. The breakpoint between the two curvatures was located at 75.9 ± 0.9% of P0 and 11.4 ± 0.6% of maximum velocity of shortening (Vmax) in control Ringer solution and at 75.6 ± 0.7% of P0 and 12.2 ± 0.7% of Vmax in the presence of dantrolene. These results provide evidence that the transition between the two curvatures of the forcevelcity relationship is primarily related to the speed of shortening, not to the actual force within the fibre. The instantaneous stiffness varied with the speed of shortening forming a biphasic relationship with a breakpoint near 0.15 Vmax and 0.8 P0, respectively. The force/stiffness ratio (probably reflecting the average force per cross‐bridge), increased with force during shortening. The increase of the force/stiffness ratio with force was less steep at forces exceeding 0.8 P0 than below this point. A four‐state cross‐bridge model (described in the Appendix) was used to evaluate the experimental results. The model reproduces with great precision the characteristic features of the force–stiffness–velocity relationships recorded in intact muscle fibres.