Dynamics of signaling between Ca(2+) sparks and Ca(2+)- activated K(+) channels studied with a novel image-based method for direct intracellular measurement of ryanodine receptor Ca(2+) current
dc.contributor.author | ZhuGe, Ronghua | |
dc.contributor.author | Fogarty, Kevin E. | |
dc.contributor.author | Tuft, Richard A. | |
dc.contributor.author | Lifshitz, Lawrence M. | |
dc.contributor.author | Sayar, Kemal | |
dc.contributor.author | Walsh, John V. | |
dc.date | 2022-08-11T08:09:31.000 | |
dc.date.accessioned | 2022-08-23T16:33:47Z | |
dc.date.available | 2022-08-23T16:33:47Z | |
dc.date.issued | 2000-12-01 | |
dc.date.submitted | 2008-10-31 | |
dc.identifier.citation | J Gen Physiol. 2000 Dec;116(6):845-64. | |
dc.identifier.issn | 0022-1295 (Print) | |
dc.identifier.pmid | 11099351 | |
dc.identifier.uri | http://hdl.handle.net/20.500.14038/38184 | |
dc.description.abstract | Ca(2+) sparks are highly localized cytosolic Ca(2+) transients caused by a release of Ca(2+) from the sarcoplasmic reticulum via ryanodine receptors (RyRs); they are the elementary events underlying global changes in Ca(2+) in skeletal and cardiac muscle. In smooth muscle and some neurons, Ca(2+) sparks activate large conductance Ca(2+)-activated K(+) channels (BK channels) in the spark microdomain, causing spontaneous transient outward currents (STOCs) that regulate membrane potential and, hence, voltage-gated channels. Using the fluorescent Ca(2+) indicator fluo-3 and a high speed widefield digital imaging system, it was possible to capture the total increase in fluorescence (i.e., the signal mass) during a spark in smooth muscle cells, which is the first time such a direct approach has been used in any system. The signal mass is proportional to the total quantity of Ca(2+) released into the cytosol, and its rate of rise is proportional to the Ca(2+) current flowing through the RyRs during a spark (I(Ca(spark))). Thus, Ca(2+) currents through RyRs can be monitored inside the cell under physiological conditions. Since the magnitude of I(Ca(spark)) in different sparks varies more than fivefold, Ca(2+) sparks appear to be caused by the concerted opening of a number of RyRs. Sparks with the same underlying Ca(2+) current cause STOCs, whose amplitudes vary more than threefold, a finding that is best explained by variability in coupling ratio (i.e., the ratio of RyRs to BK channels in the spark microdomain). The time course of STOC decay is approximated by a single exponential that is independent of the magnitude of signal mass and has a time constant close to the value of the mean open time of the BK channels, suggesting that STOC decay reflects BK channel kinetics, rather than the time course of [Ca(2+)] decline at the membrane. Computer simulations were carried out to determine the spatiotemporal distribution of the Ca(2+) concentration resulting from the measured range of I(Ca(spark)). At the onset of a spark, the Ca(2+) concentration within 200 nm of the release site reaches a plateau or exceeds the [Ca(2+)](EC50) for the BK channels rapidly in comparison to the rate of rise of STOCs. These findings suggest a model in which the BK channels lie close to the release site and are exposed to a saturating [Ca(2+)] with the rise and fall of the STOCs determined by BK channel kinetics. The mechanism of signaling between RyRs and BK channels may provide a model for Ca(2+) action on a variety of molecular targets within cellular microdomains. | |
dc.language.iso | en_US | |
dc.relation | <a href="http://www.ncbi.nlm.nih.gov/entrez/query.fcgi?db=pubmed&cmd=Retrieve&list_uids=11099351&dopt=Abstract">Link to Article in PubMed</a> | |
dc.subject | Animals | |
dc.subject | Bradykinin | |
dc.subject | Bufo marinus | |
dc.subject | Calcium | |
dc.subject | *Calcium Signaling | |
dc.subject | Cytosol | |
dc.subject | Electric Conductivity | |
dc.subject | Fluorescence | |
dc.subject | Image Processing, Computer-Assisted | |
dc.subject | Intracellular Membranes | |
dc.subject | Ion Channels | |
dc.subject | Kinetics | |
dc.subject | Microscopy | |
dc.subject | Models, Biological | |
dc.subject | Patch-Clamp Techniques | |
dc.subject | Potassium Channels | |
dc.subject | Ryanodine Receptor Calcium Release Channel | |
dc.subject | Engineering Physics | |
dc.subject | Physical Sciences and Mathematics | |
dc.title | Dynamics of signaling between Ca(2+) sparks and Ca(2+)- activated K(+) channels studied with a novel image-based method for direct intracellular measurement of ryanodine receptor Ca(2+) current | |
dc.type | Journal Article | |
dc.source.journaltitle | The Journal of general physiology | |
dc.source.volume | 116 | |
dc.source.issue | 6 | |
dc.identifier.legacyfulltext | https://escholarship.umassmed.edu/cgi/viewcontent.cgi?article=2064&context=oapubs&unstamped=1 | |
dc.identifier.legacycoverpage | https://escholarship.umassmed.edu/oapubs/1065 | |
dc.identifier.contextkey | 659254 | |
refterms.dateFOA | 2022-08-23T16:33:48Z | |
html.description.abstract | <p>Ca(2+) sparks are highly localized cytosolic Ca(2+) transients caused by a release of Ca(2+) from the sarcoplasmic reticulum via ryanodine receptors (RyRs); they are the elementary events underlying global changes in Ca(2+) in skeletal and cardiac muscle. In smooth muscle and some neurons, Ca(2+) sparks activate large conductance Ca(2+)-activated K(+) channels (BK channels) in the spark microdomain, causing spontaneous transient outward currents (STOCs) that regulate membrane potential and, hence, voltage-gated channels. Using the fluorescent Ca(2+) indicator fluo-3 and a high speed widefield digital imaging system, it was possible to capture the total increase in fluorescence (i.e., the signal mass) during a spark in smooth muscle cells, which is the first time such a direct approach has been used in any system. The signal mass is proportional to the total quantity of Ca(2+) released into the cytosol, and its rate of rise is proportional to the Ca(2+) current flowing through the RyRs during a spark (I(Ca(spark))). Thus, Ca(2+) currents through RyRs can be monitored inside the cell under physiological conditions. Since the magnitude of I(Ca(spark)) in different sparks varies more than fivefold, Ca(2+) sparks appear to be caused by the concerted opening of a number of RyRs. Sparks with the same underlying Ca(2+) current cause STOCs, whose amplitudes vary more than threefold, a finding that is best explained by variability in coupling ratio (i.e., the ratio of RyRs to BK channels in the spark microdomain). The time course of STOC decay is approximated by a single exponential that is independent of the magnitude of signal mass and has a time constant close to the value of the mean open time of the BK channels, suggesting that STOC decay reflects BK channel kinetics, rather than the time course of [Ca(2+)] decline at the membrane. Computer simulations were carried out to determine the spatiotemporal distribution of the Ca(2+) concentration resulting from the measured range of I(Ca(spark)). At the onset of a spark, the Ca(2+) concentration within 200 nm of the release site reaches a plateau or exceeds the [Ca(2+)](EC50) for the BK channels rapidly in comparison to the rate of rise of STOCs. These findings suggest a model in which the BK channels lie close to the release site and are exposed to a saturating [Ca(2+)] with the rise and fall of the STOCs determined by BK channel kinetics. The mechanism of signaling between RyRs and BK channels may provide a model for Ca(2+) action on a variety of molecular targets within cellular microdomains.</p> | |
dc.identifier.submissionpath | oapubs/1065 | |
dc.contributor.department | Biomedical Imaging Group | |
dc.source.pages | 845-64 |