matlab bvp solver Search Results


bvp4c bvp solver  (MathWorks Inc)
90
MathWorks Inc bvp4c bvp solver
As with the IM, <t>bvp4c</t> was used to numerically solve the BVP of eqn. (34). The figure follows a quite similar format to Fig. 5. can also be assumed higher or lower. All the maximal ionic conductances in the HHM (see also ) are temperature-dependent and are linearly proportional to the coefficient . The 3 solutions shown correspond to the ionic current at (cyan trace), twice higher (thin red dash-dot), or twice lower (thick dashed black) respectively. From eqn. (42) we can see that = 1.6047 (half the nominal) at , and = 6.4188 (twice the nominal) for at . Box: Resting-state and asymptotic-state ionic currents for the 0D HHM; Markers are inserted at the resting and threshold membrane-voltage points, respectively = −77 , = −64.55 and = −52.35 .
Bvp4c Bvp Solver, supplied by MathWorks 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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matlab bvp solvers  (MathWorks Inc)
90
MathWorks Inc matlab bvp solvers
As with the IM, <t>bvp4c</t> was used to numerically solve the BVP of eqn. (34). The figure follows a quite similar format to Fig. 5. can also be assumed higher or lower. All the maximal ionic conductances in the HHM (see also ) are temperature-dependent and are linearly proportional to the coefficient . The 3 solutions shown correspond to the ionic current at (cyan trace), twice higher (thin red dash-dot), or twice lower (thick dashed black) respectively. From eqn. (42) we can see that = 1.6047 (half the nominal) at , and = 6.4188 (twice the nominal) for at . Box: Resting-state and asymptotic-state ionic currents for the 0D HHM; Markers are inserted at the resting and threshold membrane-voltage points, respectively = −77 , = −64.55 and = −52.35 .
Matlab Bvp Solvers, supplied by MathWorks Inc, used in various techniques. Bioz Stars score: 90/100, based on 1 PubMed citations. ZERO BIAS - scores, article reviews, protocol conditions and more
https://www.bioz.com/result/matlab bvp solvers/product/MathWorks Inc
Average 90 stars, based on 1 article reviews
matlab bvp solvers - by Bioz Stars, 2026-04
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matlab software  (MathWorks Inc)
90
MathWorks Inc matlab software
As with the IM, <t>bvp4c</t> was used to numerically solve the BVP of eqn. (34). The figure follows a quite similar format to Fig. 5. can also be assumed higher or lower. All the maximal ionic conductances in the HHM (see also ) are temperature-dependent and are linearly proportional to the coefficient . The 3 solutions shown correspond to the ionic current at (cyan trace), twice higher (thin red dash-dot), or twice lower (thick dashed black) respectively. From eqn. (42) we can see that = 1.6047 (half the nominal) at , and = 6.4188 (twice the nominal) for at . Box: Resting-state and asymptotic-state ionic currents for the 0D HHM; Markers are inserted at the resting and threshold membrane-voltage points, respectively = −77 , = −64.55 and = −52.35 .
Matlab Software, supplied by MathWorks 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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Average 90 stars, based on 1 article reviews
matlab software - by Bioz Stars, 2026-04
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matlab bvp solver  (MathWorks Inc)
90
MathWorks Inc matlab bvp solver
As with the IM, <t>bvp4c</t> was used to numerically solve the BVP of eqn. (34). The figure follows a quite similar format to Fig. 5. can also be assumed higher or lower. All the maximal ionic conductances in the HHM (see also ) are temperature-dependent and are linearly proportional to the coefficient . The 3 solutions shown correspond to the ionic current at (cyan trace), twice higher (thin red dash-dot), or twice lower (thick dashed black) respectively. From eqn. (42) we can see that = 1.6047 (half the nominal) at , and = 6.4188 (twice the nominal) for at . Box: Resting-state and asymptotic-state ionic currents for the 0D HHM; Markers are inserted at the resting and threshold membrane-voltage points, respectively = −77 , = −64.55 and = −52.35 .
Matlab Bvp Solver, supplied by MathWorks Inc, used in various techniques. Bioz Stars score: 90/100, based on 1 PubMed citations. ZERO BIAS - scores, article reviews, protocol conditions and more
https://www.bioz.com/result/matlab bvp solver/product/MathWorks Inc
Average 90 stars, based on 1 article reviews
matlab bvp solver - by Bioz Stars, 2026-04
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matlab pse  (MathWorks Inc)
90
MathWorks Inc matlab pse
As with the IM, <t>bvp4c</t> was used to numerically solve the BVP of eqn. (34). The figure follows a quite similar format to Fig. 5. can also be assumed higher or lower. All the maximal ionic conductances in the HHM (see also ) are temperature-dependent and are linearly proportional to the coefficient . The 3 solutions shown correspond to the ionic current at (cyan trace), twice higher (thin red dash-dot), or twice lower (thick dashed black) respectively. From eqn. (42) we can see that = 1.6047 (half the nominal) at , and = 6.4188 (twice the nominal) for at . Box: Resting-state and asymptotic-state ionic currents for the 0D HHM; Markers are inserted at the resting and threshold membrane-voltage points, respectively = −77 , = −64.55 and = −52.35 .
Matlab Pse, supplied by MathWorks Inc, used in various techniques. Bioz Stars score: 90/100, based on 1 PubMed citations. ZERO BIAS - scores, article reviews, protocol conditions and more
https://www.bioz.com/result/matlab pse/product/MathWorks Inc
Average 90 stars, based on 1 article reviews
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bvp solver bvp4c  (MathWorks Inc)
90
MathWorks Inc bvp solver bvp4c
As with the IM, <t>bvp4c</t> was used to numerically solve the BVP of eqn. (34). The figure follows a quite similar format to Fig. 5. can also be assumed higher or lower. All the maximal ionic conductances in the HHM (see also ) are temperature-dependent and are linearly proportional to the coefficient . The 3 solutions shown correspond to the ionic current at (cyan trace), twice higher (thin red dash-dot), or twice lower (thick dashed black) respectively. From eqn. (42) we can see that = 1.6047 (half the nominal) at , and = 6.4188 (twice the nominal) for at . Box: Resting-state and asymptotic-state ionic currents for the 0D HHM; Markers are inserted at the resting and threshold membrane-voltage points, respectively = −77 , = −64.55 and = −52.35 .
Bvp Solver Bvp4c, supplied by MathWorks Inc, used in various techniques. Bioz Stars score: 90/100, based on 1 PubMed citations. ZERO BIAS - scores, article reviews, protocol conditions and more
https://www.bioz.com/result/bvp solver bvp4c/product/MathWorks Inc
Average 90 stars, based on 1 article reviews
bvp solver bvp4c - by Bioz Stars, 2026-04
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custom bvp solver  (MathWorks Inc)
90
MathWorks Inc custom bvp solver
Novel analytical theory of correlated colored noise-induced synchronization of heterogeneous oscillators matches Monte Carlo simulations for low to moderate levels of <t>noise.</t> <t>Stationary</t> phase difference density is shown as computed from the solution of the <t>BVP</t> and through Monte Carlo simulation from t = 1000 to t = 201000 in steps of 0.05. Monte Carlo data binned into 100 bins between −π and π. There is a frequency difference of ϵ 2 /2 where ϵ is the magnitude of the noise. Here Δ j (θ j ) = sin( a j ) − sin(θ j + a j ) + b j sin(2θ j ), where j = 1, 2 for two oscillators. (A) τ = 1, a 1 = 0.1, a 2 = 0.6, b 1 = 0.32, b 2 = 0.3, and c = 0.8. (B) τ = 0.25, a 1 = a 2 = 0.5, b 1 = b 2 = 0.3, and c = 0.5.
Custom Bvp Solver, supplied by MathWorks Inc, used in various techniques. Bioz Stars score: 90/100, based on 1 PubMed citations. ZERO BIAS - scores, article reviews, protocol conditions and more
https://www.bioz.com/result/custom bvp solver/product/MathWorks Inc
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boundary value problem (bvp) solver  (MathWorks Inc)
90
MathWorks Inc boundary value problem (bvp) solver
Novel analytical theory of correlated colored noise-induced synchronization of heterogeneous oscillators matches Monte Carlo simulations for low to moderate levels of <t>noise.</t> <t>Stationary</t> phase difference density is shown as computed from the solution of the <t>BVP</t> and through Monte Carlo simulation from t = 1000 to t = 201000 in steps of 0.05. Monte Carlo data binned into 100 bins between −π and π. There is a frequency difference of ϵ 2 /2 where ϵ is the magnitude of the noise. Here Δ j (θ j ) = sin( a j ) − sin(θ j + a j ) + b j sin(2θ j ), where j = 1, 2 for two oscillators. (A) τ = 1, a 1 = 0.1, a 2 = 0.6, b 1 = 0.32, b 2 = 0.3, and c = 0.8. (B) τ = 0.25, a 1 = a 2 = 0.5, b 1 = b 2 = 0.3, and c = 0.5.
Boundary Value Problem (Bvp) Solver, supplied by MathWorks 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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Average 90 stars, based on 1 article reviews
boundary value problem (bvp) solver - by Bioz Stars, 2026-04
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bvp solver  (MathWorks Inc)
90
MathWorks Inc bvp solver
Novel analytical theory of correlated colored noise-induced synchronization of heterogeneous oscillators matches Monte Carlo simulations for low to moderate levels of <t>noise.</t> <t>Stationary</t> phase difference density is shown as computed from the solution of the <t>BVP</t> and through Monte Carlo simulation from t = 1000 to t = 201000 in steps of 0.05. Monte Carlo data binned into 100 bins between −π and π. There is a frequency difference of ϵ 2 /2 where ϵ is the magnitude of the noise. Here Δ j (θ j ) = sin( a j ) − sin(θ j + a j ) + b j sin(2θ j ), where j = 1, 2 for two oscillators. (A) τ = 1, a 1 = 0.1, a 2 = 0.6, b 1 = 0.32, b 2 = 0.3, and c = 0.8. (B) τ = 0.25, a 1 = a 2 = 0.5, b 1 = b 2 = 0.3, and c = 0.5.
Bvp Solver, supplied by MathWorks Inc, used in various techniques. Bioz Stars score: 90/100, based on 1 PubMed citations. ZERO BIAS - scores, article reviews, protocol conditions and more
https://www.bioz.com/result/bvp solver/product/MathWorks Inc
Average 90 stars, based on 1 article reviews
bvp solver - by Bioz Stars, 2026-04
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two-point bvp (boundary value problem) solver  (MathWorks Inc)
90
MathWorks Inc two-point bvp (boundary value problem) solver
Novel analytical theory of correlated colored noise-induced synchronization of heterogeneous oscillators matches Monte Carlo simulations for low to moderate levels of <t>noise.</t> <t>Stationary</t> phase difference density is shown as computed from the solution of the <t>BVP</t> and through Monte Carlo simulation from t = 1000 to t = 201000 in steps of 0.05. Monte Carlo data binned into 100 bins between −π and π. There is a frequency difference of ϵ 2 /2 where ϵ is the magnitude of the noise. Here Δ j (θ j ) = sin( a j ) − sin(θ j + a j ) + b j sin(2θ j ), where j = 1, 2 for two oscillators. (A) τ = 1, a 1 = 0.1, a 2 = 0.6, b 1 = 0.32, b 2 = 0.3, and c = 0.8. (B) τ = 0.25, a 1 = a 2 = 0.5, b 1 = b 2 = 0.3, and c = 0.5.
Two Point Bvp (Boundary Value Problem) Solver, supplied by MathWorks 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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Image Search Results


As with the IM, bvp4c was used to numerically solve the BVP of eqn. (34). The figure follows a quite similar format to Fig. 5. can also be assumed higher or lower. All the maximal ionic conductances in the HHM (see also ) are temperature-dependent and are linearly proportional to the coefficient . The 3 solutions shown correspond to the ionic current at (cyan trace), twice higher (thin red dash-dot), or twice lower (thick dashed black) respectively. From eqn. (42) we can see that = 1.6047 (half the nominal) at , and = 6.4188 (twice the nominal) for at . Box: Resting-state and asymptotic-state ionic currents for the 0D HHM; Markers are inserted at the resting and threshold membrane-voltage points, respectively = −77 , = −64.55 and = −52.35 .

Journal: PLoS ONE

Article Title: Energy-Optimal Electrical-Stimulation Pulses Shaped by the Least-Action Principle

doi: 10.1371/journal.pone.0090480

Figure Lengend Snippet: As with the IM, bvp4c was used to numerically solve the BVP of eqn. (34). The figure follows a quite similar format to Fig. 5. can also be assumed higher or lower. All the maximal ionic conductances in the HHM (see also ) are temperature-dependent and are linearly proportional to the coefficient . The 3 solutions shown correspond to the ionic current at (cyan trace), twice higher (thin red dash-dot), or twice lower (thick dashed black) respectively. From eqn. (42) we can see that = 1.6047 (half the nominal) at , and = 6.4188 (twice the nominal) for at . Box: Resting-state and asymptotic-state ionic currents for the 0D HHM; Markers are inserted at the resting and threshold membrane-voltage points, respectively = −77 , = −64.55 and = −52.35 .

Article Snippet: Hence, we used the Matlab bvp4c BVP solver with boundary conditions and . illustrates the energy-optimal LAP solution and the corresponding membrane voltage profile .

Techniques: Membrane

Novel analytical theory of correlated colored noise-induced synchronization of heterogeneous oscillators matches Monte Carlo simulations for low to moderate levels of noise. Stationary phase difference density is shown as computed from the solution of the BVP and through Monte Carlo simulation from t = 1000 to t = 201000 in steps of 0.05. Monte Carlo data binned into 100 bins between −π and π. There is a frequency difference of ϵ 2 /2 where ϵ is the magnitude of the noise. Here Δ j (θ j ) = sin( a j ) − sin(θ j + a j ) + b j sin(2θ j ), where j = 1, 2 for two oscillators. (A) τ = 1, a 1 = 0.1, a 2 = 0.6, b 1 = 0.32, b 2 = 0.3, and c = 0.8. (B) τ = 0.25, a 1 = a 2 = 0.5, b 1 = b 2 = 0.3, and c = 0.5.

Journal: Frontiers in Computational Neuroscience

Article Title: Impact of neuronal heterogeneity on correlated colored noise-induced synchronization

doi: 10.3389/fncom.2013.00113

Figure Lengend Snippet: Novel analytical theory of correlated colored noise-induced synchronization of heterogeneous oscillators matches Monte Carlo simulations for low to moderate levels of noise. Stationary phase difference density is shown as computed from the solution of the BVP and through Monte Carlo simulation from t = 1000 to t = 201000 in steps of 0.05. Monte Carlo data binned into 100 bins between −π and π. There is a frequency difference of ϵ 2 /2 where ϵ is the magnitude of the noise. Here Δ j (θ j ) = sin( a j ) − sin(θ j + a j ) + b j sin(2θ j ), where j = 1, 2 for two oscillators. (A) τ = 1, a 1 = 0.1, a 2 = 0.6, b 1 = 0.32, b 2 = 0.3, and c = 0.8. (B) τ = 0.25, a 1 = a 2 = 0.5, b 1 = b 2 = 0.3, and c = 0.5.

Article Snippet: We solve the BVP for the stationary phase difference density using a custom BVP solver written in MATLAB.

Techniques: