Use of a new index to study relaxation in a vascular model of anaphylactic shock

Isotonic relaxation of control and sensitized airway smooth muscle

Smooth muscle relaxation has most often been studied in isometric mode. However, this only tells us about the stiffness properties of the bronchial wall and thus only about wall capacitative properties. It tells us little about airflow. To study the latter, which of course is the meaningful parameter in regulation of ventilation and in asthma, we studied isotonic shortening of bronchial smooth muscle (BSM) strips. Failure of BSM to relax could be another important factor in maintaining high airway resistance. To analyze relaxation curves, we developed an index of isotonic relaxation, t1/2(P, lCE), which is the half-time for relaxation that is independent of muscle load (P) and of initial contractile element length (lCE). This index was measured in curves of relaxation initiated at 2 s (normally cycling crossbridges) and at 10 s (latch-bridges). At 10 s no difference was seen for adjusted t1/2(P, lCE) between curves obtained from control and sensitized BSM, (8.38 +/- 0.92 s vs. 7.78 +/- 0.93 s, respectively). At 2 s the half-time was almost doubled in the sensitized BSM (6.98 +/- 0.01 s (control) vs. 12.74 +/- 2.5 s (sensitized)). Thus, changes in isotonic relaxation are only seen during early contraction. Using zero load clamps, we monitored the time course of velocity during relaxation and noted that it varied according to 3 phases. The first phase (phase i) immediately followed cessation of electrical field stimulation (EFS) at 10 s and showed almost the same velocity as during the latter 1/3 of shortening; the second phase (phase ii) was linear in shape and is associated with zero load velocity, we speculate it could stem from elastic recoil of the cells' internal resistor; and the third phase (phase iii) was convex downwards. The zero load velocities in phase iii showed a surprising spontaneous increase suggesting reactivation of the muscle. Measurements of intracellular calcium (Fura-2 study) and of phosphorylation of the 20 kDa myosin light chain showed simultaneous increments, indicating phase iii represented an active process. Studies are under way to determine what changes occur in these 3 phases in a sensitized muscle. And of course, in the context of this conference, just what role the plastic properties of the muscle play in relaxation requires serious consideration.

Regulation of myosin light chain phosphatase and pulmonary arterial relaxation

Neonatal circulatory transition is dependent upon tightly regulated pulmonary circuit relaxation. Persistent pulmonary hypertension (PPHN), a rapidly progressive disease of pulmonary arterial vasospasm and remodelling, may be characterized by pulmonary arterial myocyte relaxation failure. A key regulator of vascular tone is myocyte calcium sensitivity, determined by the relative stoichiometry of myosin light chain phosphorylation and dephosphorylation. We have recently reported downregulation of myosin light chain phosphatase activity in a hypoxic model of neonatal pulmonary hypertension. This review examines the recognized pathways of regulation governing myosin light chain phosphatase activity, including targeting subunit isoform switching, targeting unit phosphorylation and catalytic site inhibition. In light of the reviewed literature, further speculation is proposed on the potential contributions of these mechanisms to the pathophysiology of the perinatal pulmonary arterial relaxation defect in PPHN.Key words: smooth muscle, pulmonary hypertension, myosin light chain phosphatase, CPI-17, MYPT, review.

Role of speed vs. grade in relation to muscle pump function at locomotion onset

We sought to clarify the roles of contraction frequency (speed) and contraction force (grade) in the rise in muscle blood flow at the onset of locomotion. Shoemaker et al. (Can J Physiol Pharmacol 76: 418-427, 1998) explored this relationship in human handgrip exercise and found that the time course of the rise in muscle vascular conductance was similar when a light weight was lifted in a fast cadence and a heavy weight was lifted in a slow cadence (total work constant). This indicates that muscle pumping (contraction frequency) was of limited importance in governing the time course. Rather, vasodilator substances released in proportion to the total work performed appeared to determine the pattern and extent of the rise in conductance. We hypothesized that conductance would rise faster during locomotion at a high speed (frequency) and low grade (force) than at a low speed and high grade, despite similar total increases in conductance, owing to more effective muscle pumping at faster contraction rates. Seven male rats performed nine 1-min bouts of treadmill locomotion across a combination of three speeds (5, 10, and 20 m/min) and three grades (-10, 0, and +15 degrees ) in random order. Locomotion at 10 m/min and 0 degrees grade and 20 m/min and -10 degrees grade led to an equal rise in terminal aortic vascular conductance. However, the equal rise was achieved more quickly at the higher running speed, suggestive of more effective muscle pumping. Across the nine combinations of exercise, speed began to exert a statistically significant influence on conductance by the 3rd s of locomotion. Grade did not begin to exert an influence until the 12th s of locomotion (similar to the delays reported for arteriolar dilation to muscle contraction). Additional experiments in dogs provided similar results. Thus the muscle pump appears to initiate the increase in blood flow in proportion to contraction frequency at locomotion onset.