Pawel Swietach, Kenneth W. Spitzer, Richard D. Vaughan-Jones 

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Ca2+-Mobility in the Sarcoplasmic Reticulum of Ventricular Myocytes Is Low  Pawel Swietach, Kenneth W. Spitzer, Richard D. Vaughan-Jones  Biophysical Journal  Volume 95, Issue 3, Pages 1412-1427 (August 2008) DOI: 10.1529/biophysj.108.130385 Copyright © 2008 The Biophysical Society Terms and Conditions

FIGURE 1 Protocol for stabilizing SR Ca2+ load. Rat myocytes. (A) Fluo-3 fluorescence (F/F0) was measured in cells paced at 2Hz in NT, and then superfused with 0Na0Ca medium (fluorescence normalized to diastolic levels in NT). Ca2+-waves were observed in the first 2 min in 0Na0Ca. After waves ceased, diastolic F/F0 was ∼1. (B) In 0Na0Ca solution with SERCA inhibited by 10μM CPA (stabilizing solution, SS), RyRs were dose-dependently inhibited by 0.3 or 2mM Tet. Inclusion of Tet in SS-superfusate blocked Ca2+-waves. At both doses of Tet, resting F/F0 stabilized (at a 25% lower level) with a half-time of ∼36s. Cells stabilized in SS + Tet were then used for the main experiments. (C) The reduction of resting F/F0 observed in the presence of SS + Tet was absent in rat cells preloaded with 100μM BAPTA-AM. (A–C) Mean of 7–10 cells. Biophysical Journal 2008 95, 1412-1427DOI: (10.1529/biophysj.108.130385) Copyright © 2008 The Biophysical Society Terms and Conditions

FIGURE 2 Mobilizing SR Ca2+ with caffeine. (A) Rat myocyte, AM-loaded with Fluo-3 and initially paced at 2Hz in NT was then superfused with 0Na0Ca medium containing 10μM CPA (stabilizing solution, SS), interspersed with three 30-s episodes of SS + 10mM caffeine. (Upper panel) time course for F/F0 averaged along a longitudinal line scan (inset indicates position of line scan axis); (middle panel) F/F0 line scan; (lower panel) cell shortening. The first caffeine exposure mobilizes all SR Ca2+. (B) Different rat myocyte exposed to SS containing 10mM caffeine and 10mM [Ca2+]o; note lack of Cai2+ -recovery, suggesting block of sarcolemmal PMCA. Final recovery in 0Na0Ca (with zero CPA) is attributable to SERCA and PMCA activity. Biophysical Journal 2008 95, 1412-1427DOI: (10.1529/biophysj.108.130385) Copyright © 2008 The Biophysical Society Terms and Conditions

FIGURE 3 Assessing SR Ca2+-leak. Myocytes paced at 2Hz in NT were then superfused with SS containing 0.3 or 2.0mM Tet. (A) After 1min in SS+0.3mM Tet, rat myocyte was exposed to Tet-free SS+10mM caffeine for 30s. (Upper panel) longitudinal line scan average for F/F0; (middle panel) F/F0 line scan (y axis normalized to cell length); (lower panel) cell shortening. (B) Different rat myocyte, exposed to caffeine after 4min in SS+0.3mM Tet. Smaller Ca2+-release is due to longer preceding period of SR-membrane Ca2+-leakage. (C) (i) Peak F/F0 during caffeine-exposure, measured after 1–6min delay (normalized to F/F0 at switch into SS) in rat myocytes in 0.3mM (green) or 2mM (black) Tet, and in guinea pig myocytes in 2mM Tet (gray) (n=5–10 cells/data-point). (ii) Cell shortening responses to caffeine in rat myocytes. Rundown of both F/F0 and cell shortening gives time course of SR depletion caused by Ca2+-leak. Biophysical Journal 2008 95, 1412-1427DOI: (10.1529/biophysj.108.130385) Copyright © 2008 The Biophysical Society Terms and Conditions

FIGURE 4 Measuring SR Ca2+-mobility. Caffeine is used to estimate the decline of distal [Ca2+]SRT, while Ca2+ is being drained from the proximal end of SR. (A) Dual-microperfusion apparatus is used to deliver two solutions: SS (without Tet or with 0.3 or 2mM Tet) and SS + caffeine (10mM with no Tet). Myocyte is first bathed in SS + Tet (configuration 0). Throughout the experiment, intracellular Fluo-3 fluorescence (F/F0) is averaged in two ROIs, each 20% of cell length, one positioned proximally (ROI-P) and one distally (ROI-D), at the ends of a line scan (see schematic diagram shown to the right of configuration 0). SS + caffeine is then applied to proximal end of myocyte to start SR-drainage (configuration 1); after a 30–240s delay, SS + caffeine is applied to whole cell (configuration 2) to assess remaining SR Ca2+-content. At the end of the experiment, cells are returned to 0Na0Ca, free of CPA, Tet, and caffeine (not illustrated, denoted by arrow 3 in B and C). (B) SS microstream (but not SS + caffeine microstream) contained 0.3mM Tet. (i) Rat myocyte; delay of 30s between configurations 1 and 2. (Upper panel) F/F0-time course for [Ca2+]i averaged in ROI-P (black trace) and ROI-D (gray trace). Dashed line shows predicted decline of caffeine-mobilizable Ca2+-release because of SR Ca2+-leak (from Fig. 3). (Middle panel) Longitudinal F/F0 line scan (y axis normalized to cell length). (Lower panel) cell shortening. (ii) Rat myocyte; delay of 240s between configurations 1 and 2. (C) SS microstream (but not SS + caffeine microstream) contained 2.0mM Tet. (i) Rat myocyte; delay of 120s between configurations 1 and 2. (ii) Guinea pig myocyte; delay of 180s between configurations 1 and 2. (D) Ratio of distal fluorescence rise (configuration 2) to initial proximal rise (configuration 1), ΔF2/ΔF1, for different delay times. Rat myocytes with 2mM Tet (black), 0.3mM Tet (green), and zero Tet (blue). Guinea pig myocytes with 2mM Tet (gray) (4–12 cells/data point). Time constants (τ) obtained from monoexponential fits. Biophysical Journal 2008 95, 1412-1427DOI: (10.1529/biophysj.108.130385) Copyright © 2008 The Biophysical Society Terms and Conditions

FIGURE 5 Distal SR depletion with proximal caffeine is unaffected by Fluo-3. (A) Myocyte AM-loaded with carboxy-SNARF-1, a non-Ca2+ binding fluorophore. Upper panel: fluorescence line scan (y axis shows cell length) used to monitor cell shortening (carboxy-SNARF-1 excitation at 514nm, emission at 580nm). (Lower panel) time course of cell shortening (derived from upper panel) in response to caffeine. Protocol of Fig. 4 was applied. Cell initially exposed to SS+0.3mM Tet. At circle 1, the proximal end of the cell exposed to SS+10mM caffeine; at circle 2 the whole cell exposed to SS+10mM caffeine. (B) Ratio of second/first shortening-event is plotted versus time delay between circles 1 and 2 in the presence of intracellular carboxy-SNARF-1 (black; n=8, 7) or Fluo-3 (gray; n=6–13). Time constants (τ) obtained from monoexponential fits. The presence of the Ca2+-binding fluorophore, Fluo-3, does not affect the rate of decline of distal contraction (and hence distal SR-depletion) during proximal caffeine exposure. Biophysical Journal 2008 95, 1412-1427DOI: (10.1529/biophysj.108.130385) Copyright © 2008 The Biophysical Society Terms and Conditions

FIGURE 6 Quantifying DCaSR. (A) (i) Schematic diagram of the simple Ca2+-diffusion model, incorporating SR-membrane leak and proximal SR-exposure to caffeine (see Appendix 1). (ii) Best-fitting of diffusion model (SERCA activity=0, simulating CPA-addition) to data in Fig. 4 D gives displayed values for DCaSR (0.3mM Tet, green; 2mM Tet, black: rat myocytes; 2mM Tet, gray: guinea pig myocytes). Note unique value for DCaSR (8–9μm2/s). (iii) Best-fitting when SR Ca2+-leak is ignored; note lack of unique value for DCaSR (42, 23, and 10μm2/s for rat myocyte data (Fig. 4 D) with 0, 0.3, and 2mM Tet, respectively). (B) (i) Schematic diagram of diffusion-reaction model showing principal reaction elements (see Appendix 1). (ii) Displayed DCaSR: best-fit values averaged between 0 and 240s. (Green) rat, 0.3mM Tet; (black) rat, 2mM Tet; (gray) guinea pig, 2mM Tet. Note similarity with DCaSR values from Aii. (C) Output of cellular diffusion-reaction model simulating experimental protocol (Fig. 4). (i) Time course of F/F0 from simulated line scan in proximal (black) and distal (gray) ROIs. (ii) Simulated line scans for F/F0, [Ca2+]i and [Ca2+]SR. Biophysical Journal 2008 95, 1412-1427DOI: (10.1529/biophysj.108.130385) Copyright © 2008 The Biophysical Society Terms and Conditions

FIGURE 7 Effect of DCaSR on longitudinal [Ca2+]SR profile during simulated local Ca2+-release. Diffusion-reaction model was run to simulate local SR Ca2+-release (see Appendix 1). [Ca2+]SR was calculated 250ms after increasing SR-membrane permeability to 1.35μM/s in a central 2μm length of SR. This estimate of DCaSR (9μm2/s) supports large and localized SR-depletion, with only small effects on adjacent luminal regions. Higher DCaSR significantly depletes SR Ca2+ from regions beyond the release site. (Dashed line) 5% depletion threshold. Biophysical Journal 2008 95, 1412-1427DOI: (10.1529/biophysj.108.130385) Copyright © 2008 The Biophysical Society Terms and Conditions

FIGURE 8 Modeling Ca2+-diffusion in SR nanoarchitecture. (A) (i) 2-D geometry for a unit of sarcomeric SR (jSR-cisterna connected to four nSR-tubes) triangulated for diffusion modeling. (ii) To simulate jSR Ca2+-recovery after local Ca2+-release, [Ca2+]jSR was set instantaneously to 0.25 (50% depletion), whereas [Ca2+]nSR was set initially to 0.5mM and the distal ends of the nSR elements were coupled to an infinite 0.5mM Ca2+ source. The time constant (τ) of recovery of [Ca2+]jSR was then derived for a range of jSR Ca2+-mobility values (DCajSR), with Ca2+-mobility in nSR assumed to be 1000μm2/s. The predicted time courses of change for [Ca2+]jSR and [Ca2+]nSR are shown in the inset. Filled circle denotes τ=29ms, which has been determined experimentally for rabbit SR Ca2+-blinks. (iii) Spatial [Ca2+]SR map after 29ms of jSR-refilling for a DCajSR of 1.8μm2/s. (B) (i) 63×10 SR units based on Ai, coupled into a 2-D network for simulating whole-SR during proximal caffeine exposure (see Appendix 2). (ii) Predicted relationship between global DCaSR and DCajSR. DCajSR of 1.8μm2/s (derived from normal Ca2+-blink recovery rate) predicts a global DCaSR of 8μm2/s, similar to the value measured experimentally. In contrast, a high global DCaSR (60μm2/s) predicts a relatively high DCajSR (41μm2/s), which would then predict an ultrafast Ca2+-blink recovery τ of <1ms (see Aii). (Inset) Close-up of DCaSR range between 0 and 10μm2/s. (iii) Model of nSR/jSR unit featuring a minimal length nSR (0.65μm), divided into snSR and inSR. Diffusion in the inSR is slower than in the snSR (see Appendix 2 for details). Biophysical Journal 2008 95, 1412-1427DOI: (10.1529/biophysj.108.130385) Copyright © 2008 The Biophysical Society Terms and Conditions