Volume 87, Issue 2, Pages (August 2004)

Slides:



Advertisements
Similar presentations
Teresa K. Aman, Indira M. Raman  Biophysical Journal 
Advertisements

Volume 85, Issue 1, Pages (July 2003)
Volume 88, Issue 2, Pages (February 2005)
External Tetraethylammonium As a Molecular Caliper for Sensing the Shape of the Outer Vestibule of Potassium Channels  Frank Bretschneider, Anja Wrisch,
Molecular Determinants of U-Type Inactivation in Kv2.1 Channels
Binding Site in Eag Voltage Sensor Accommodates a Variety of Ions and is Accessible in Closed Channel  William R. Silverman, John P.A. Bannister, Diane.
Interaction between Extracellular Hanatoxin and the Resting Conformation of the Voltage-Sensor Paddle in Kv Channels  Hwa C Lee, Julia M Wang, Kenton.
Functional Modularity of the β-Subunit of Voltage-Gated Ca2+ Channels
Voltage Sensor–Trapping
Chiu Shuen Hui, Henry R. Besch, Keshore R. Bidasee  Biophysical Journal 
Volume 91, Issue 8, Pages (October 2006)
Differential Modulation of Cardiac Ca2+ Channel Gating by β-Subunits
FPL Modification of CaV1
Volume 20, Issue 8, Pages (August 2012)
Volume 113, Issue 12, Pages (December 2017)
Partial Inhibition of Sarcoplasmic Reticulum Ca Release Evokes Long-Lasting Ca Release Events in Ventricular Myocytes: Role of Luminal Ca in Termination.
Preferential Closed-State Inactivation of Neuronal Calcium Channels
Zhuren Wang, J. Christian Hesketh, David Fedida  Biophysical Journal 
Intracellular Ca Alternans: Coordinated Regulation by Sarcoplasmic Reticulum Release, Uptake, and Leak  Lai-Hua Xie, Daisuke Sato, Alan Garfinkel, Zhilin.
Volume 16, Issue 10, Pages (October 2008)
Volume 111, Issue 2, Pages (July 2016)
Volume 85, Issue 1, Pages (July 2003)
Volume 74, Issue 1, Pages (January 1998)
Volume 87, Issue 2, Pages (August 2004)
Volume 75, Issue 5, Pages (September 2012)
Volume 92, Issue 7, Pages (April 2007)
Volume 95, Issue 4, Pages (August 2008)
Francis D. Appling, Aaron L. Lucius, David A. Schneider 
Tzur Paldi, Michael Gurevitz  Biophysical Journal 
Volume 106, Issue 6, Pages (March 2014)
Gilberto J Soler-Llavina, Miguel Holmgren, Kenton J Swartz  Neuron 
Calmodulin Modulates Initiation but Not Termination of Spontaneous Ca2+ Sparks in Frog Skeletal Muscle  George G. Rodney, Martin F. Schneider  Biophysical.
Teresa K. Aman, Indira M. Raman  Biophysical Journal 
Volume 24, Issue 2, Pages (February 2016)
Carlos A. Obejero-Paz, Stephen W. Jones, Antonio Scarpa 
Katie C. Bittner, Dorothy A. Hanck  Biophysical Journal 
Volume 97, Issue 3, Pages (August 2009)
Volume 93, Issue 12, Pages (December 2007)
Volume 100, Issue 1, Pages (January 2011)
Samuel J. Goodchild, Logan C. Macdonald, David Fedida 
Payam Andalib, Joseph F. Consiglio, Josef G. Trapani, Stephen J. Korn 
Volume 88, Issue 3, Pages (March 2005)
Volume 108, Issue 6, Pages (March 2015)
Volume 101, Issue 4, Pages (August 2011)
Daniel Krofchick, Mel Silverman  Biophysical Journal 
Volume 97, Issue 1, Pages (July 2009)
Extrapore Residues of the S5-S6 Loop of Domain 2 of the Voltage-Gated Skeletal Muscle Sodium Channel (rSkM1) Contribute to the μ-Conotoxin GIIIA Binding.
Sara I. Börjesson, Sven Hammarström, Fredrik Elinder 
Effects of Temperature on Heteromeric Kv11.1a/1b and Kv11.3 Channels
Fredrik Elinder, Michael Madeja, Hugo Zeberg, Peter Århem 
Volume 85, Issue 6, Pages (December 2003)
A Specific Tryptophan in the I-II Linker Is a Key Determinant of β-Subunit Binding and Modulation in CaV2.3 Calcium Channels  L. Berrou, H. Klein, G.
Inhibition of αβ Epithelial Sodium Channels by External Protons Indicates That the Second Hydrophobic Domain Contains Structural Elements for Closing.
Vladimir Avdonin, Toshinori Hoshi  Biophysical Journal 
Volume 84, Issue 1, Pages (January 2003)
Elementary Functional Properties of Single HCN2 Channels
A Point Mutation in Domain 4-Segment 6 of the Skeletal Muscle Sodium Channel Produces an Atypical Inactivation State  John P. O’Reilly, Sho-Ya Wang, Ging.
Don E. Burgess, Oscar Crawford, Brian P. Delisle, Jonathan Satin 
Volume 94, Issue 9, Pages (May 2008)
Kinetics of P2X7 Receptor-Operated Single Channels Currents
Christina Karatzaferi, Marc K. Chinn, Roger Cooke  Biophysical Journal 
R.P. Schuhmeier, B. Dietze, D. Ursu, F. Lehmann-Horn, W. Melzer 
Volume 87, Issue 5, Pages (November 2004)
Interaction between Extracellular Hanatoxin and the Resting Conformation of the Voltage-Sensor Paddle in Kv Channels  Hwa C Lee, Julia M Wang, Kenton.
Use Dependence of Heat Sensitivity of Vanilloid Receptor TRPV2
Antonella Gradogna, Michael Pusch  Biophysical Journal 
Volume 84, Issue 1, Pages (January 2003)
Yassine El Hiani, Paul Linsdell  Biophysical Journal 
Volume 101, Issue 11, Pages (December 2011)
Liping He, Jerod Denton, Keith Nehrke, Kevin Strange 
Presentation transcript:

Volume 87, Issue 2, Pages 929-942 (August 2004) Involvement of a Heptad Repeat in the Carboxyl Terminus of the Dihydropyridine Receptor β1a Subunit in the Mechanism of Excitation-Contraction Coupling in Skeletal Muscle  David C. Sheridan, Weijun Cheng, Leah Carbonneau, Chris A. Ahern, Roberto Coronado  Biophysical Journal  Volume 87, Issue 2, Pages 929-942 (August 2004) DOI: 10.1529/biophysj.104.043810 Copyright © 2004 The Biophysical Society Terms and Conditions

Figure 1 Recovery of Ca2+ current and Ca2+ transients by splice variants of the four β-genes expressed in β1 KO myotubes. Columns show representative β1 KO myotubes transfected with skeletal muscle β1a, cardiac/brain β2a, brain β3, and brain β4. GenBank identification numbers are indicated in Materials and Methods. Top trace corresponds to the spatial integral of the confocal Ca2+ transient in ΔF/F units in response to a 200ms depolarization to +30mV from a holding potential of −40mV. The Ca2+ current during the 200-ms depolarization is shown expanded. Note change in amplitude scale for the time course of fluorescence. Bottom shows Ca2+ conductance versus voltage curves for population averages in response to a 500-ms depolarization in 5mV increments from −35 to +60mV. The shaded line in all figures shows the average Ca2+ conductance of nontransfected β1 KO myotubes. Curves were fit with Eq. 1 with the following parameters (Gmax in pS/pF, V1/2 in mV, and k in mV, respectively). For β1a: 194, 14.9, and 7.0; for β2a: 183, 11.6, and 5.2; for β3: 40, 40.2, and 28.1; and for β4: 171, 16.9, and 7.0. Biophysical Journal 2004 87, 929-942DOI: (10.1529/biophysj.104.043810) Copyright © 2004 The Biophysical Society Terms and Conditions

Figure 2 Charge movements and Ca2+ conductance expressed by β1a-β2a chimeras in β1 KO myotubes. Chimeras were identified according to the source, β1a or β2a, of the five domains (D1, D2, D3, D4, and D5). Boundaries for each domain were obtained from a sequence lineup described in Materials and Methods. In the block diagram representation of the chimeras, shaded is β2a and black is β1a. The shaded line in all graphs shows the average charge movement or Ca2+ conductance of nontransfected β1 KO myotubes. Charge movement curves were fit with Eq. 1 with the following parameters (Qmax in fC/pF, V1/2 in mV, and k in mV, respectively). For β2a(D1–D3)/β1a(D4, D5): 4.0, 32.5, and 19.7; for β1a(D1–D3)/β2a(D4, D5): 4.7, 33.3, and 20.9; for β2a(D1–D4)/β1aD5: 3.5, −6.8, and 11.5; for β1a(D1–D4)/β2aD5: 3.9, 9.3, and 18.2; and for nontransfected β1 KO myotubes: 1.8, 5.2, and 17. Ca2+ conductance curves were fit with Eq. 1 with the following parameters (Gmax in pS/pF, V1/2 in mV, and k in mV, respectively). For β2a(D1–D3)/β1a(D4, D5): 204, 9.9, and 6.0; for β1a(D1–D3)/β2a(D4, D5): 63, 15.2, and 5.3; for β2a(D1–D4)/β1aD5: 181, 5.5, and 5.0; for β1a(D1–D4)/β2aD5: 42, 14.6, and 6.2; and for nontransfected β1 KO myotubes: 20, 20, and 14. Biophysical Journal 2004 87, 929-942DOI: (10.1529/biophysj.104.043810) Copyright © 2004 The Biophysical Society Terms and Conditions

Figure 3 Ca2+ transients expressed by β1a-β2a chimeras in β1 KO myotubes. Open symbols correspond to peak ΔF/F obtained with a 200-ms depolarization and solid symbols were obtained with a 50-ms depolarization. Except for β1a(D1–D4)/β2aD5, the lines correspond to a Boltzmann fit of the mean (peak ΔF/F) for the population of cells. For β1a(D1–D4)/β2aD5, the lines are an interpolation of the mean at each potential. All fluorescence versus voltage curves were fit with Eq. 1, except those obtained with the 200ms depolarization in the bottom row, which were fit with Eq. 2. Curves were fit with the following parameters (ΔF/Fmax in ΔF/F units, V1/2 in mV, and k in mV, respectively). For β2a(D1–D3)/β1a(D4, D5): 2.5, −5.5, 8.4 (50ms), and 2.9, −7.1, 8.0 (200ms); for β2a(D1–D4)/β1aD5: 2.3, 2.8, 5.8 (50ms) and 2.5, −1.5, 5.5 (200ms); and for β1a(D1–D3)/β2a(D4, D5): 0.2, −16.3, 13.4 (50ms) and 0.9, 11.1, 1.9 (200ms). Biophysical Journal 2004 87, 929-942DOI: (10.1529/biophysj.104.043810) Copyright © 2004 The Biophysical Society Terms and Conditions

Figure 4 Nifedipine-insensitive Ca2+ transients expressed by β1a-β2a chimeras in β1 KO myotubes. Columns show representative β1 KO myotubes expressing full-length WT β1a, β2a(D1–D3)/β1a(D4, D5), and β2a(D1–D4)/β1aD5. Myotubes were depolarized for 200ms from a holding potential of −40mV to +30mV in standard external solution containing 10mM Ca2+. Ca2+ transients and Ca2+ currents were measured in the same myotube before and after (shaded traces) inhibition of the Ca2+ current by 2.5μM nifedipine added to the external solution. Ca2+ currents during the 200ms depolarization are shown expanded. Graphs show peak ΔF/F versus voltage relationships before and after (shaded symbols) nifedipine inhibition. Biophysical Journal 2004 87, 929-942DOI: (10.1529/biophysj.104.043810) Copyright © 2004 The Biophysical Society Terms and Conditions

Figure 5 Ca2+ conductance and Ca2+ transients expressed by β1a-β2a chimeras with domain D5 in different positions. Columns show the functional behavior chimeras with a C-terminus corresponding to a tandem of β1aD5 and β2aD5 domains expressed in β1 KO myotube. Ca2+ conductance curves were fit with Eq. 1 with the following parameters (Gmax in pS/pF, V1/2 in mV, and k in mV, respectively). For β2a(D1–D4)/β2aD5/β1aD5: 192, 16.7, and 5.5; for β2a(D1–D4)/β1aD5/β2aD5: 175, 11.9, and 4.4; for β1a(D1–D4)/β2aD5/β1aD5: 71, 19.4, and 5.3; and for β1a(D1–D4)/β1D5/β2aD5: 177, 18.5, and 6.8. For fluorescence curves, open symbols correspond to peak ΔF/F obtained with a 200-ms depolarization, and solid symbols were obtained with a 50-ms depolarization. The lines correspond to fit of the mean peak ΔF/F. All fluorescence versus voltage curves were fit with Eq. 1 except those obtained with the 200ms depolarization in myotubes expressing β1a(D1–D4)/β2aD5/β1aD5 and β2a(D1–D4)/β2aD5/β1aD5, which were fit with Eq. 2. Curves were fit with the following parameters (ΔF/Fmax in ΔF/F units, V1/2 in mV, and k in mV, respectively). For β1a(D1–D4)/β1aD5/β2aD5:1.9, 7.0, and 9.4 (50ms), and 2.0, 8.9, and 10.5 (200ms). For β1a(D1–D4)/β2aD5/β1aD5: 0.4, 20.3, and 21.4 (50ms), and 0.5, 11.1, and 7.8 (200ms). For β2a(D1–D4)/β2aD5/β1aD5: 0.3, 4.9, and 12.5 (50ms), and 0.9, 16.9, and 9.5 (200ms). For β2a(D1–D4)/β1aD5/β2aD5: 2.2, 16.3, and 9.9 (50ms), and 2.3, 5.8, and 6.3 (200ms). Biophysical Journal 2004 87, 929-942DOI: (10.1529/biophysj.104.043810) Copyright © 2004 The Biophysical Society Terms and Conditions

Figure 6 Ca2+ conductance and Ca2+ transients expressed by heptad repeat mutants in β1 KO myotubes. β1a positions L478, V485, and V492 were mutated to alanine (β1a L478A/V485A/V492A). This triple mutation is labeled D5ALA. β1a positions S481, L488, and S495 were mutated to alanine (β1a S481A/L488A/S495A). This triple control mutation is labeled D5ALAc. Ca2+ conductance curves expressed by WT β1a, D5ALA, and D5ALAc were fit with Eq. 1 with the following parameters (Gmax in pS/pF, V1/2 in mV, and k in mV, respectively). For WT β1a (see Fig. 1); for D5ALA: 123, 24.9, and 5.3; for D5ALAc: 106, 23.0, and 10.7. The shaded line in the top right curve corresponds to WT β1a. In fluorescence curves, open symbols correspond to peak ΔF/F obtained with a 200-ms depolarization and solid symbols were obtained with a 50-ms depolarization. All fluorescence versus voltage curves were fit with Eq. 1 with the following parameters (ΔF/Fmax in ΔF/F units, V1/2 in mV, and k in mV, respectively). For WT β1a: 2.8, −6.1, and 7.8 (50ms), and 3.2, −10.2, and 5.7 (200ms). For D5ALA: 0.4, 14.6, and 14.4 (50ms), and 0.7, 18.1, and 12.1 (200ms). For D5ALAc: 2.1, 13.7, and 7.9 (50ms), and 2.4, 9.1, and 4.3 (200ms). The shaded lines in bottom right curve correspond to WT β1a used as a reference. Conductance versus voltage curve for WT β1a shown in this figure is the same as in the left panel of Fig. 1. Ca2+ transient versus voltage curves from WT β1a are from Sheridan et al. (2003b). Biophysical Journal 2004 87, 929-942DOI: (10.1529/biophysj.104.043810) Copyright © 2004 The Biophysical Society Terms and Conditions

Figure 7 Proposed model of the domain organization of β1a. An EC coupling “permissive” domain organization of β1a (diagrams A and B) requires domain β1aD5 (red) to be present immediately downstream from conserved D4 (yellow). Nonpermissive domain organizations (diagrams C and D) come about when the bulkier β2aD5 domain (blue) hinders interaction of the subunit and critical binding partners such as RyR1 (gray). A core of tightly bound D2 (green) and D4 (yellow) is conserved among all tested chimeras, consistent with the homology of β-subunits to MAGUK proteins and the structure of the MAGUK protein PSD-95 (McGee et al., 2001; Tavares et al., 2001). For the sake of clarity, β1aD5 has been drawn next to D4. However, according to the PSD-95 structure, β1aD5 may be located closer to the cleft between D2 and D4 domains. EC coupling permissive states with β1aD5 next to D4 (A and B) could bind preferentially to RyR1 (gray), or could facilitate binding of other domains of the DHPR to RyR1. Biophysical Journal 2004 87, 929-942DOI: (10.1529/biophysj.104.043810) Copyright © 2004 The Biophysical Society Terms and Conditions