nonlinear regression (curve fit)-boltzmann sigmoidal Search Results


non-linear curve fit of boltzmann method  (OriginLab corp)
90
OriginLab corp non-linear curve fit of boltzmann method
Non Linear Curve Fit Of Boltzmann Method, supplied by OriginLab corp, used in various techniques. Bioz Stars score: 90/100, based on 1 PubMed citations. ZERO BIAS - scores, article reviews, protocol conditions and more
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curve fitting analysis using “boltzmann modified” equation  (OriginLab corp)
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OriginLab corp curve fitting analysis using “boltzmann modified” equation
Curve Fitting Analysis Using “Boltzmann Modified” Equation, supplied by OriginLab corp, used in various techniques. Bioz Stars score: 90/100, based on 1 PubMed citations. ZERO BIAS - scores, article reviews, protocol conditions and more
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boltzmann fits  (OriginLab corp)
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OriginLab corp boltzmann fits
Domain-specific charge neutralizations. (A) Sequence alignments of the S4 voltage-sensing segments from each domain in Nav1.4. Mutations are marked in bold. (B) A representative family of ionic current traces for wild-type and mutant channels in response to 30-ms depolarizing pulses from −110 to 65 mV (10-mV steps), preceded by a 20-ms prepulse to −120 mV from a holding potential of −80 mV. (C) Normalized peak G-V relationship for wild-type and mutant channels. Solid lines are single <t>Boltzmann</t> fits to the mean for each construct (wild type: V 1/2 = −23.8 mV and z = 5.8 e − ; DI-CN: V 1/2 = −36.5 mV and z = 3.8 e − ; DII-CN: V 1/2 = −25.1 mV and z = 3.3 e − ; DIII-CN: V 1/2 = −26.4 mV and z = 3.9 e − ; DIV-CN: V 1/2 = −23.1 mV and z = 3.8 e − ).
Boltzmann Fits, supplied by OriginLab corp, used in various techniques. Bioz Stars score: 90/100, based on 1 PubMed citations. ZERO BIAS - scores, article reviews, protocol conditions and more
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boltzmann curve  (OriginLab corp)
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OriginLab corp boltzmann curve
Domain-specific charge neutralizations. (A) Sequence alignments of the S4 voltage-sensing segments from each domain in Nav1.4. Mutations are marked in bold. (B) A representative family of ionic current traces for wild-type and mutant channels in response to 30-ms depolarizing pulses from −110 to 65 mV (10-mV steps), preceded by a 20-ms prepulse to −120 mV from a holding potential of −80 mV. (C) Normalized peak G-V relationship for wild-type and mutant channels. Solid lines are single <t>Boltzmann</t> fits to the mean for each construct (wild type: V 1/2 = −23.8 mV and z = 5.8 e − ; DI-CN: V 1/2 = −36.5 mV and z = 3.8 e − ; DII-CN: V 1/2 = −25.1 mV and z = 3.3 e − ; DIII-CN: V 1/2 = −26.4 mV and z = 3.9 e − ; DIV-CN: V 1/2 = −23.1 mV and z = 3.8 e − ).
Boltzmann Curve, supplied by OriginLab corp, used in various techniques. Bioz Stars score: 90/100, based on 1 PubMed citations. ZERO BIAS - scores, article reviews, protocol conditions and more
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boltzmann curve - by Bioz Stars, 2026-08
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boltzmann function  (OriginLab corp)
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OriginLab corp boltzmann function
Domain-specific charge neutralizations. (A) Sequence alignments of the S4 voltage-sensing segments from each domain in Nav1.4. Mutations are marked in bold. (B) A representative family of ionic current traces for wild-type and mutant channels in response to 30-ms depolarizing pulses from −110 to 65 mV (10-mV steps), preceded by a 20-ms prepulse to −120 mV from a holding potential of −80 mV. (C) Normalized peak G-V relationship for wild-type and mutant channels. Solid lines are single <t>Boltzmann</t> fits to the mean for each construct (wild type: V 1/2 = −23.8 mV and z = 5.8 e − ; DI-CN: V 1/2 = −36.5 mV and z = 3.8 e − ; DII-CN: V 1/2 = −25.1 mV and z = 3.3 e − ; DIII-CN: V 1/2 = −26.4 mV and z = 3.9 e − ; DIV-CN: V 1/2 = −23.1 mV and z = 3.8 e − ).
Boltzmann Function, supplied by OriginLab corp, used in various techniques. Bioz Stars score: 90/100, based on 1 PubMed citations. ZERO BIAS - scores, article reviews, protocol conditions and more
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boltzmann fits to conductance–voltage relations  (OriginLab corp)
90
OriginLab corp boltzmann fits to conductance–voltage relations
Domain-specific charge neutralizations. (A) Sequence alignments of the S4 voltage-sensing segments from each domain in Nav1.4. Mutations are marked in bold. (B) A representative family of ionic current traces for wild-type and mutant channels in response to 30-ms depolarizing pulses from −110 to 65 mV (10-mV steps), preceded by a 20-ms prepulse to −120 mV from a holding potential of −80 mV. (C) Normalized peak G-V relationship for wild-type and mutant channels. Solid lines are single <t>Boltzmann</t> fits to the mean for each construct (wild type: V 1/2 = −23.8 mV and z = 5.8 e − ; DI-CN: V 1/2 = −36.5 mV and z = 3.8 e − ; DII-CN: V 1/2 = −25.1 mV and z = 3.3 e − ; DIII-CN: V 1/2 = −26.4 mV and z = 3.9 e − ; DIV-CN: V 1/2 = −23.1 mV and z = 3.8 e − ).
Boltzmann Fits To Conductance–Voltage Relations, supplied by OriginLab corp, used in various techniques. Bioz Stars score: 90/100, based on 1 PubMed citations. ZERO BIAS - scores, article reviews, protocol conditions and more
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lattice boltzmann method  (Lallemand inc)
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Lallemand inc lattice boltzmann method
Domain-specific charge neutralizations. (A) Sequence alignments of the S4 voltage-sensing segments from each domain in Nav1.4. Mutations are marked in bold. (B) A representative family of ionic current traces for wild-type and mutant channels in response to 30-ms depolarizing pulses from −110 to 65 mV (10-mV steps), preceded by a 20-ms prepulse to −120 mV from a holding potential of −80 mV. (C) Normalized peak G-V relationship for wild-type and mutant channels. Solid lines are single <t>Boltzmann</t> fits to the mean for each construct (wild type: V 1/2 = −23.8 mV and z = 5.8 e − ; DI-CN: V 1/2 = −36.5 mV and z = 3.8 e − ; DII-CN: V 1/2 = −25.1 mV and z = 3.3 e − ; DIII-CN: V 1/2 = −26.4 mV and z = 3.9 e − ; DIV-CN: V 1/2 = −23.1 mV and z = 3.8 e − ).
Lattice Boltzmann Method, supplied by Lallemand inc, used in various techniques. Bioz Stars score: 90/100, based on 1 PubMed citations. ZERO BIAS - scores, article reviews, protocol conditions and more
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boltzmann  (Loschmidt Laboratories)
86
Loschmidt Laboratories boltzmann
Domain-specific charge neutralizations. (A) Sequence alignments of the S4 voltage-sensing segments from each domain in Nav1.4. Mutations are marked in bold. (B) A representative family of ionic current traces for wild-type and mutant channels in response to 30-ms depolarizing pulses from −110 to 65 mV (10-mV steps), preceded by a 20-ms prepulse to −120 mV from a holding potential of −80 mV. (C) Normalized peak G-V relationship for wild-type and mutant channels. Solid lines are single <t>Boltzmann</t> fits to the mean for each construct (wild type: V 1/2 = −23.8 mV and z = 5.8 e − ; DI-CN: V 1/2 = −36.5 mV and z = 3.8 e − ; DII-CN: V 1/2 = −25.1 mV and z = 3.3 e − ; DIII-CN: V 1/2 = −26.4 mV and z = 3.9 e − ; DIV-CN: V 1/2 = −23.1 mV and z = 3.8 e − ).
Boltzmann, supplied by Loschmidt Laboratories, used in various techniques. Bioz Stars score: 86/100, based on 1 PubMed citations. ZERO BIAS - scores, article reviews, protocol conditions and more
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boltzmann distribution  (Wadiche labs)
90
Wadiche labs boltzmann distribution
Domain-specific charge neutralizations. (A) Sequence alignments of the S4 voltage-sensing segments from each domain in Nav1.4. Mutations are marked in bold. (B) A representative family of ionic current traces for wild-type and mutant channels in response to 30-ms depolarizing pulses from −110 to 65 mV (10-mV steps), preceded by a 20-ms prepulse to −120 mV from a holding potential of −80 mV. (C) Normalized peak G-V relationship for wild-type and mutant channels. Solid lines are single <t>Boltzmann</t> fits to the mean for each construct (wild type: V 1/2 = −23.8 mV and z = 5.8 e − ; DI-CN: V 1/2 = −36.5 mV and z = 3.8 e − ; DII-CN: V 1/2 = −25.1 mV and z = 3.3 e − ; DIII-CN: V 1/2 = −26.4 mV and z = 3.9 e − ; DIV-CN: V 1/2 = −23.1 mV and z = 3.8 e − ).
Boltzmann Distribution, supplied by Wadiche labs, used in various techniques. Bioz Stars score: 90/100, based on 1 PubMed citations. ZERO BIAS - scores, article reviews, protocol conditions and more
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boltzmann modified equation  (OriginLab corp)
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OriginLab corp boltzmann modified equation
Domain-specific charge neutralizations. (A) Sequence alignments of the S4 voltage-sensing segments from each domain in Nav1.4. Mutations are marked in bold. (B) A representative family of ionic current traces for wild-type and mutant channels in response to 30-ms depolarizing pulses from −110 to 65 mV (10-mV steps), preceded by a 20-ms prepulse to −120 mV from a holding potential of −80 mV. (C) Normalized peak G-V relationship for wild-type and mutant channels. Solid lines are single <t>Boltzmann</t> fits to the mean for each construct (wild type: V 1/2 = −23.8 mV and z = 5.8 e − ; DI-CN: V 1/2 = −36.5 mV and z = 3.8 e − ; DII-CN: V 1/2 = −25.1 mV and z = 3.3 e − ; DIII-CN: V 1/2 = −26.4 mV and z = 3.9 e − ; DIV-CN: V 1/2 = −23.1 mV and z = 3.8 e − ).
Boltzmann Modified Equation, supplied by OriginLab corp, used in various techniques. Bioz Stars score: 90/100, based on 1 PubMed citations. ZERO BIAS - scores, article reviews, protocol conditions and more
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finite-element numerical calculations of a poisson-boltzmann formulation  (Verlag GmbH)
90
Verlag GmbH finite-element numerical calculations of a poisson-boltzmann formulation
Domain-specific charge neutralizations. (A) Sequence alignments of the S4 voltage-sensing segments from each domain in Nav1.4. Mutations are marked in bold. (B) A representative family of ionic current traces for wild-type and mutant channels in response to 30-ms depolarizing pulses from −110 to 65 mV (10-mV steps), preceded by a 20-ms prepulse to −120 mV from a holding potential of −80 mV. (C) Normalized peak G-V relationship for wild-type and mutant channels. Solid lines are single <t>Boltzmann</t> fits to the mean for each construct (wild type: V 1/2 = −23.8 mV and z = 5.8 e − ; DI-CN: V 1/2 = −36.5 mV and z = 3.8 e − ; DII-CN: V 1/2 = −25.1 mV and z = 3.3 e − ; DIII-CN: V 1/2 = −26.4 mV and z = 3.9 e − ; DIV-CN: V 1/2 = −23.1 mV and z = 3.8 e − ).
Finite Element Numerical Calculations Of A Poisson Boltzmann Formulation, supplied by Verlag GmbH, used in various techniques. Bioz Stars score: 90/100, based on 1 PubMed citations. ZERO BIAS - scores, article reviews, protocol conditions and more
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lattice boltzmann  (Unifi Inc)
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Unifi Inc lattice boltzmann
Figure 5. Crystal structures developed at different Da numbers and at solute saturation (1.2): (a) Da = 600; (b) Da = 150; (c) Da = 48; (d) Da = 2. m represents the number of solid particles (crystal mass). [Used by permission of John Wiley and Sons, from Kang Q, Zhang D, Lichtner PC, Tsimpanogiannis IN (2004) Lattice <t>Boltzmann</t> model for crystal growth from supersaturated solution. Geophysical Research Letters, Vol. 31, Fig. 2, p. L21604-3]
Lattice Boltzmann, supplied by Unifi Inc, used in various techniques. Bioz Stars score: 86/100, based on 1 PubMed citations. ZERO BIAS - scores, article reviews, protocol conditions and more
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Image Search Results


Domain-specific charge neutralizations. (A) Sequence alignments of the S4 voltage-sensing segments from each domain in Nav1.4. Mutations are marked in bold. (B) A representative family of ionic current traces for wild-type and mutant channels in response to 30-ms depolarizing pulses from −110 to 65 mV (10-mV steps), preceded by a 20-ms prepulse to −120 mV from a holding potential of −80 mV. (C) Normalized peak G-V relationship for wild-type and mutant channels. Solid lines are single Boltzmann fits to the mean for each construct (wild type: V 1/2 = −23.8 mV and z = 5.8 e − ; DI-CN: V 1/2 = −36.5 mV and z = 3.8 e − ; DII-CN: V 1/2 = −25.1 mV and z = 3.3 e − ; DIII-CN: V 1/2 = −26.4 mV and z = 3.9 e − ; DIV-CN: V 1/2 = −23.1 mV and z = 3.8 e − ).

Journal: The Journal of General Physiology

Article Title: Domain IV voltage-sensor movement is both sufficient and rate limiting for fast inactivation in sodium channels

doi: 10.1085/jgp.201310998

Figure Lengend Snippet: Domain-specific charge neutralizations. (A) Sequence alignments of the S4 voltage-sensing segments from each domain in Nav1.4. Mutations are marked in bold. (B) A representative family of ionic current traces for wild-type and mutant channels in response to 30-ms depolarizing pulses from −110 to 65 mV (10-mV steps), preceded by a 20-ms prepulse to −120 mV from a holding potential of −80 mV. (C) Normalized peak G-V relationship for wild-type and mutant channels. Solid lines are single Boltzmann fits to the mean for each construct (wild type: V 1/2 = −23.8 mV and z = 5.8 e − ; DI-CN: V 1/2 = −36.5 mV and z = 3.8 e − ; DII-CN: V 1/2 = −25.1 mV and z = 3.3 e − ; DIII-CN: V 1/2 = −26.4 mV and z = 3.9 e − ; DIV-CN: V 1/2 = −23.1 mV and z = 3.8 e − ).

Article Snippet: Boltzmann fits to conductance–voltage relations were performed in Origin (OriginLab).

Techniques: Sequencing, Mutagenesis, Construct

DIV voltage-sensor movement is sufficient for fast inactivation. (A) A representative family of current traces in response to a 30-ms test pulse to −30 mV to assay the fraction of non–steady-state inactivated channels after a 100-ms conditioning prepulse between −170 and 50 mV. See Results for a detailed description of the voltage-pulse protocol. (B) Normalized steady-state inactivation versus conditioning prepulse voltage for wild-type and mutant channels. Solid lines are single Boltzmann fits to the mean for each construct (wild type: V 1/2 = −62.3 mV and z = 4.7 e − ; DI-CN: V 1/2 = −69.2 mV and z = 4.2 e − ; DII-CN: V 1/2 = −65.8 mV and z = 3.7 e − ; DIII-CN: V 1/2 = −68.7 mV and z = 2.7 e − ; DIV-CN: V 1/2 = −137.3 mV and z = 1.1 e − ). Note that the relation does not saturate above −200 mV for DIV-CN, so the observed left-shift in the steady-state inactivation versus voltage relation reflects the minimum shift conferred by this mutant.

Journal: The Journal of General Physiology

Article Title: Domain IV voltage-sensor movement is both sufficient and rate limiting for fast inactivation in sodium channels

doi: 10.1085/jgp.201310998

Figure Lengend Snippet: DIV voltage-sensor movement is sufficient for fast inactivation. (A) A representative family of current traces in response to a 30-ms test pulse to −30 mV to assay the fraction of non–steady-state inactivated channels after a 100-ms conditioning prepulse between −170 and 50 mV. See Results for a detailed description of the voltage-pulse protocol. (B) Normalized steady-state inactivation versus conditioning prepulse voltage for wild-type and mutant channels. Solid lines are single Boltzmann fits to the mean for each construct (wild type: V 1/2 = −62.3 mV and z = 4.7 e − ; DI-CN: V 1/2 = −69.2 mV and z = 4.2 e − ; DII-CN: V 1/2 = −65.8 mV and z = 3.7 e − ; DIII-CN: V 1/2 = −68.7 mV and z = 2.7 e − ; DIV-CN: V 1/2 = −137.3 mV and z = 1.1 e − ). Note that the relation does not saturate above −200 mV for DIV-CN, so the observed left-shift in the steady-state inactivation versus voltage relation reflects the minimum shift conferred by this mutant.

Article Snippet: Boltzmann fits to conductance–voltage relations were performed in Origin (OriginLab).

Techniques: Mutagenesis, Construct

Figure 5. Crystal structures developed at different Da numbers and at solute saturation (1.2): (a) Da = 600; (b) Da = 150; (c) Da = 48; (d) Da = 2. m represents the number of solid particles (crystal mass). [Used by permission of John Wiley and Sons, from Kang Q, Zhang D, Lichtner PC, Tsimpanogiannis IN (2004) Lattice Boltzmann model for crystal growth from supersaturated solution. Geophysical Research Letters, Vol. 31, Fig. 2, p. L21604-3]

Journal: Reviews in Mineralogy and Geochemistry

Article Title: Lattice Boltzmann-Based Approaches for Pore-Scale Reactive Transport

doi: 10.2138/rmg.2015.80.12

Figure Lengend Snippet: Figure 5. Crystal structures developed at different Da numbers and at solute saturation (1.2): (a) Da = 600; (b) Da = 150; (c) Da = 48; (d) Da = 2. m represents the number of solid particles (crystal mass). [Used by permission of John Wiley and Sons, from Kang Q, Zhang D, Lichtner PC, Tsimpanogiannis IN (2004) Lattice Boltzmann model for crystal growth from supersaturated solution. Geophysical Research Letters, Vol. 31, Fig. 2, p. L21604-3]

Article Snippet: J Comput Phys 250: 293–307 Tong ZX, He YL (2015) A unifi ed coupling scheme between lattice Boltzmann method and fi nite volume method for unsteady fl uid fl ow and heat transfer.

Techniques:

Figure 6. Crystal structures and solute concentration obtained using single-mineral VOP approach (ran- dom growth) (left) and multiple-mineral VOP approach (right). [Used by permission of Hindawi, from Kang QJ, Lichtner PC (2013) A lattice Boltzmann method for coupled fl uid fl ow, solute transport, and chemical reaction. In: Progress in Computational Physics. Ehrhardt M (ed) Bentham Science Publishers, Vol. 3, Fig. 8, p. 196]

Journal: Reviews in Mineralogy and Geochemistry

Article Title: Lattice Boltzmann-Based Approaches for Pore-Scale Reactive Transport

doi: 10.2138/rmg.2015.80.12

Figure Lengend Snippet: Figure 6. Crystal structures and solute concentration obtained using single-mineral VOP approach (ran- dom growth) (left) and multiple-mineral VOP approach (right). [Used by permission of Hindawi, from Kang QJ, Lichtner PC (2013) A lattice Boltzmann method for coupled fl uid fl ow, solute transport, and chemical reaction. In: Progress in Computational Physics. Ehrhardt M (ed) Bentham Science Publishers, Vol. 3, Fig. 8, p. 196]

Article Snippet: J Comput Phys 250: 293–307 Tong ZX, He YL (2015) A unifi ed coupling scheme between lattice Boltzmann method and fi nite volume method for unsteady fl uid fl ow and heat transfer.

Techniques: Concentration Assay