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Results: 5

1.
Figure 2

Figure 2. From: A fully implicit finite element method for bidomain models of cardiac electromechanics.

Illustration of the cardiac and extracardiac domains and and the endocardium , the epicardium , and outer boundary .

Hüsnü Dal, et al. Comput Methods Appl Mech Eng. ;253:323-336.
2.
Figure 3

Figure 3. From: A fully implicit finite element method for bidomain models of cardiac electromechanics.

Initiation and rotation of a spiral re-entry in excitable and deformable cardiac tissue. The first, second and third row denote the transmembrane potential Φ, extracellular potential Φe and active fiber tension σ, respectively.

Hüsnü Dal, et al. Comput Methods Appl Mech Eng. ;253:323-336.
3.
Figure 4

Figure 4. From: A fully implicit finite element method for bidomain models of cardiac electromechanics.

Coupled excitation induced contraction of generic heart model at various stages of depolarization. The first, second and third row denote the transmembrane potential Φ, extracellular potential Φe and active fiber tension σ, respectively.

Hüsnü Dal, et al. Comput Methods Appl Mech Eng. ;253:323-336.
4.
Figure 5

Figure 5. From: A fully implicit finite element method for bidomain models of cardiac electromechanics.

Coupled excitation induced contraction of generic heart model at various stages of repolarization. The first, second and third row denote the transmembrane potential Φ, extracellular potential Φe and active fiber tension σ, respectively.

Hüsnü Dal, et al. Comput Methods Appl Mech Eng. ;253:323-336.
5.
Figure 1

Figure 1. From: A fully implicit finite element method for bidomain models of cardiac electromechanics.

One-dimensional representaion of myocardium and approximation of the cell membrane by resistor-capacitor circuit. The circuit consists of a nonlinear resistor dependent on the ionic concentrations (sodium [Na]+, potassium [K]+ and leakage currents) of intra- and extracellular domains and a capacitor .

Hüsnü Dal, et al. Comput Methods Appl Mech Eng. ;253:323-336.

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