4 research outputs found

    Modeling CICR in rat ventricular myocytes: voltage clamp studies

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    <p>Abstract</p> <p>Background</p> <p>The past thirty-five years have seen an intense search for the molecular mechanisms underlying calcium-induced calcium-release (CICR) in cardiac myocytes, with voltage clamp (VC) studies being the leading tool employed. Several VC protocols including lowering of extracellular calcium to affect <it>Ca</it><sup>2+ </sup>loading of the sarcoplasmic reticulum (SR), and administration of blockers caffeine and thapsigargin have been utilized to probe the phenomena surrounding SR <it>Ca</it><sup>2+ </sup>release. Here, we develop a deterministic mathematical model of a rat ventricular myocyte under VC conditions, to better understand mechanisms underlying the response of an isolated cell to calcium perturbation. Motivation for the study was to pinpoint key control variables influencing CICR and examine the role of CICR in the context of a physiological control system regulating cytosolic <it>Ca</it><sup>2+ </sup>concentration ([<it>Ca</it><sup>2+</sup>]<it><sub>myo</sub></it>).</p> <p>Methods</p> <p>The cell model consists of an electrical-equivalent model for the cell membrane and a fluid-compartment model describing the flux of ionic species between the extracellular and several intracellular compartments (cell cytosol, SR and the dyadic coupling unit (DCU), in which resides the mechanistic basis of CICR). The DCU is described as a controller-actuator mechanism, internally stabilized by negative feedback control of the unit's two diametrically-opposed <it>Ca</it><sup>2+ </sup>channels (trigger-channel and release-channel). It releases <it>Ca</it><sup>2+ </sup>flux into the cyto-plasm and is in turn enclosed within a negative feedback loop involving the SERCA pump, regulating[<it>Ca</it><sup>2+</sup>]<it><sub>myo</sub></it>.</p> <p>Results</p> <p>Our model reproduces measured VC data published by several laboratories, and generates graded <it>Ca</it><sup>2+ </sup>release at high <it>Ca</it><sup>2+ </sup>gain in a homeostatically-controlled environment where [<it>Ca</it><sup>2+</sup>]<it><sub>myo </sub></it>is precisely regulated. We elucidate the importance of the DCU elements in this process, particularly the role of the ryanodine receptor in controlling SR <it>Ca</it><sup>2+ </sup>release, its activation by trigger <it>Ca</it><sup>2+</sup>, and its refractory characteristics mediated by the luminal SR <it>Ca</it><sup>2+ </sup>sensor. Proper functioning of the DCU, sodium-calcium exchangers and SERCA pump are important in achieving negative feedback control and hence <it>Ca</it><sup>2+ </sup>homeostasis.</p> <p>Conclusions</p> <p>We examine the role of the above <it>Ca</it><sup>2+ </sup>regulating mechanisms in handling various types of induced disturbances in <it>Ca</it><sup>2+ </sup>levels by quantifying cellular <it>Ca</it><sup>2+ </sup>balance. Our model provides biophysically-based explanations of phenomena associated with CICR generating useful and testable hypotheses.</p

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    This chapter describes lasers and other sources of coherent light that operate in a wide wavelength range. First, the general principles for the generation of coherent continuous-wave and pulsed radiation are treated including the interaction of radiation with matter, the properties of optical resonators and their modes as well as such processes as Q-switching and mode-locking. The general introduction is followed by sections on numerous types of lasers, the emphasis being on todayʼs most important sources of coherent light, in particular on solid-state lasers and several types of gas lasers. An important part of the chapter is devoted to the generation of coherent radiation by nonlinear processes with optical parametric oscillators, difference- and sum-frequency generation, and high-order harmonics. Radiation in the extended ultraviolet (EUV) and x-ray ranges can be generated by free electron lasers (FEL) and advanced x-ray sources. Ultrahigh light intensities up to 1021 W/cm2 open the door to studies of relativistic laser–matter interaction and laser particle acceleration. The chapter closes with a section on laser stabilization
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