$\frac{-\mathrm{Total\_current}}{\mathrm{Cm}}$ $\mathrm{i\_Na}+\mathrm{i\_K1}+\mathrm{i\_to}+\mathrm{i\_Kur}+\mathrm{i\_Kr}+\mathrm{i\_Ks}+\mathrm{i\_B\_Na}+\mathrm{i\_B\_Ca}+\mathrm{i\_NaK}+\mathrm{i\_CaP}+\mathrm{i\_NaCa}+\mathrm{i\_Ca\_L}+\mathrm{i\_Ca\_T}+\mathrm{i\_f}+\mathrm{i\_KACh}$ $\begin{cases}-0.5 & \text{if $\mathrm{Total\_current}< -20$}\\ 0 & \text{otherwise}\end{cases}$ $\begin{cases}-0.5 & \text{if $(\mathrm{Total\_current}< -2)\land (\mathrm{Total\_current}> -3)\land (V< 0)$}\\ 0 & \text{otherwise}\end{cases}$ $\frac{\mathrm{m\_inf}-m}{\mathrm{tau\_m}}$ $\begin{cases}3.2 & \text{if $V=-47.13$}\\ \frac{0.32(V+47.13)}{1-e^{-0.1(V+47.13)}} & \text{otherwise}\end{cases}$ $0.08e^{\frac{-V}{11}}$ $\frac{\mathrm{alpha\_m}}{\mathrm{alpha\_m}+\mathrm{beta\_m}}$ $\frac{1}{\mathrm{alpha\_m}+\mathrm{beta\_m}}$ $\frac{\mathrm{h\_inf}-h}{\mathrm{tau\_h}}$ $\begin{cases}0.135e^{\frac{V+80}{-6.8}} & \text{if $V< -40$}\\ 0 & \text{otherwise}\end{cases}$ $\begin{cases}3.56e^{0.079V}+3.1E5e^{0.35V} & \text{if $V< -40$}\\ \frac{1}{0.13(1+e^{\frac{V+10.66}{-11.1}})} & \text{otherwise}\end{cases}$ $\frac{\mathrm{alpha\_h}}{\mathrm{alpha\_h}+\mathrm{beta\_h}}$ $\frac{1}{\mathrm{alpha\_h}+\mathrm{beta\_h}}$ $\frac{\mathrm{j\_inf}-j}{\mathrm{tau\_j}}$ $\begin{cases}\frac{(-1.2714E5e^{0.2444V}-3.474E-5e^{-0.04391V})(V+37.78)}{1+e^{0.311(V+79.23)}} & \text{if $V< -40$}\\ 0 & \text{otherwise}\end{cases}$ $\begin{cases}\frac{0.1212e^{-0.01052V}}{1+e^{-0.1378(V+40.14)}} & \text{if $V< -40$}\\ \frac{0.3e^{-2.535E-7V}}{1+e^{-0.1(V+32)}} & \text{otherwise}\end{cases}$ $\frac{\mathrm{alpha\_j}}{\mathrm{alpha\_j}+\mathrm{beta\_j}}$ $\frac{1}{\mathrm{alpha\_j}+\mathrm{beta\_j}}$ $\mathrm{Cm}\mathrm{g\_Na}m^{3}hj(V-\mathrm{E\_Na})$ $\frac{RT}{F}\ln \left(\frac{\mathrm{Na\_o}}{\mathrm{Na\_i}}\right)$ $\frac{\mathrm{Cm}\mathrm{g\_K1}(V-\mathrm{E\_K})}{1+e^{0.07(V+80)}}$ $\frac{RT}{F}\ln \left(\frac{\mathrm{K\_o}}{\mathrm{K\_i}}\right)$ $\frac{\mathrm{oa\_infinity}-\mathrm{oa}}{\mathrm{tau\_oa}}$ $0.65(e^{\frac{V--10}{-8.5}}+e^{\frac{V--10-40}{-59}})^{-1}$ $0.65(2.5+e^{\frac{V--10+72}{17}})^{-1}$ $\frac{(\mathrm{alpha\_oa}+\mathrm{beta\_oa})^{-1}}{\mathrm{K\_Q10}}$ $(1+e^{\frac{V--10+10.47}{-17.54}})^{-1}$ $\frac{\mathrm{oi\_infinity}-\mathrm{oi}}{\mathrm{tau\_oi}}$ $(18.53+1e^{\frac{V--10+103.7}{10.95}})^{-1}$ $(35.56+1e^{\frac{V--10-8.74}{-7.44}})^{-1}$ $\frac{(\mathrm{alpha\_oi}+\mathrm{beta\_oi})^{-1}}{\mathrm{K\_Q10}}$ $(1+e^{\frac{V--10+33.1}{5.3}})^{-1}$ $\mathrm{Cm}\mathrm{g\_to}\mathrm{oa}^3\mathrm{oi}(V-\mathrm{E\_K})$ $\frac{\mathrm{ua\_infinity}-\mathrm{ua}}{\mathrm{tau\_ua}}$ $0.65(e^{\frac{V--10}{-8.5}}+e^{\frac{V--10-40}{-59}})^{-1}$ $0.65(2.5+e^{\frac{V--10+72}{17}})^{-1}$ $\frac{(\mathrm{alpha\_ua}+\mathrm{beta\_ua})^{-1}}{\mathrm{K\_Q10}}$ $(1+e^{\frac{V--10+20.3}{-9.6}})^{-1}$ $\frac{\mathrm{ui\_infinity}-\mathrm{ui}}{\mathrm{tau\_ui}}$ $(21+1e^{\frac{V--10-195}{-28}})^{-1}$ $\frac{1}{e^{\frac{V--10-168}{-16}}}$ $\frac{(\mathrm{alpha\_ui}+\mathrm{beta\_ui})^{-1}}{\mathrm{K\_Q10}}$ $(1+e^{\frac{V--10-109.45}{27.48}})^{-1}$ $\mathrm{Cm}\mathrm{g\_Kur}\mathrm{ua}^3\mathrm{ui}(V-\mathrm{E\_K})$ $(0.005+\frac{0.05}{1+e^{\frac{V-15}{-13}}})\times 0.13$ $\frac{\mathrm{xr\_infinity}-\mathrm{xr}}{\mathrm{tau\_xr}}$ $\begin{cases}0.0015 & \text{if $\left|V+14.1\right|< 1E-10$}\\ \frac{0.0003(V+14.1)}{1-e^{\frac{V+14.1}{-5}}} & \text{otherwise}\end{cases}$ $\begin{cases}3.7836118E-4 & \text{if $\left|V-3.3328\right|< 1E-10$}\\ \frac{7.3898E-5(V-3.3328)}{e^{\frac{V-3.3328}{5.1237}}-1} & \text{otherwise}\end{cases}$ $(\mathrm{alpha\_xr}+\mathrm{beta\_xr})^{-1}$ $(1+e^{\frac{V+14.1}{-6.5}})^{-1}$ $\frac{\mathrm{Cm}\mathrm{g\_Kr}\mathrm{xr}(V-\mathrm{E\_K})}{1+e^{\frac{V+15}{22.4}}}$ $\frac{\mathrm{xs\_infinity}-\mathrm{xs}}{\mathrm{tau\_xs}}$ $\begin{cases}0.00068 & \text{if $\left|V-19.9\right|< 1E-10$}\\ \frac{4E-5(V-19.9)}{1-e^{\frac{V-19.9}{-17}}} & \text{otherwise}\end{cases}$ $\begin{cases}0.000315 & \text{if $\left|V-19.9\right|< 1E-10$}\\ \frac{3.5E-5(V-19.9)}{e^{\frac{V-19.9}{9}}-1} & \text{otherwise}\end{cases}$ $0.5(\mathrm{alpha\_xs}+\mathrm{beta\_xs})^{-1}$ $(1+e^{\frac{V-19.9}{-12.7}})^{-0.5}$ $\mathrm{Cm}\mathrm{g\_Ks}\mathrm{xs}^2(V-\mathrm{E\_K})$ $\frac{\mathrm{d\_infinity}-d}{\mathrm{tau\_d}}$ $(1+e^{\frac{V+10}{-8}})^{-1}$ $\begin{cases}\frac{4.579}{1+e^{\frac{V+10}{-6.24}}} & \text{if $\left|V+10\right|< 1E-10$}\\ \frac{1-e^{\frac{V+10}{-6.24}}}{0.035(V+10)(1+e^{\frac{V+10}{-6.24}})} & \text{otherwise}\end{cases}$ $\frac{\mathrm{f\_infinity}-f}{\mathrm{tau\_f}}$ $\frac{e^{\frac{-(V+28)}{6.9}}}{1+e^{\frac{-(V+28)}{6.9}}}$ $9(0.0197e^{-0.0337^2(V+10)^2}+0.02)^{-1}$ $\frac{\mathrm{f\_Ca\_infinity}-\mathrm{f\_Ca}}{\mathrm{tau\_f\_Ca}}$ $(1+\frac{\mathrm{Ca\_i}}{0.00035})^{-1}$ $2$ $\mathrm{Cm}\mathrm{g\_Ca\_L}df\mathrm{f\_Ca}(V-65)$ $\frac{\frac{\mathrm{Cm}\mathrm{i\_NaK\_max}\mathrm{f\_NaK}\times 1}{1+\left(\frac{\mathrm{Km\_Na\_i}}{\mathrm{Na\_i}}\right)^{1.5}}\mathrm{K\_o}}{\mathrm{K\_o}+\mathrm{Km\_K\_o}}$ $(1+0.1245e^{\frac{-0.1FV}{RT}}+0.0365\mathrm{sigma}e^{\frac{-FV}{RT}})^{-1}$ $\frac{1}{7}(e^{\frac{\mathrm{Na\_o}}{67.3}}-1)$ $\mathrm{Cm}\mathrm{g\_B\_Na}(V-\mathrm{E\_Na})$ $\mathrm{Cm}\mathrm{g\_B\_Ca}(V-\mathrm{E\_Ca})$ $\mathrm{Cm}\mathrm{g\_B\_K}(V-\mathrm{E\_K})$ $\frac{RT}{2F}\ln \left(\frac{\mathrm{Ca\_o}}{\mathrm{Ca\_i}}\right)$ $\frac{\mathrm{Cm}\mathrm{I\_NaCa\_max}(e^{\frac{\mathrm{gamma}FV}{RT}}\mathrm{Na\_i}^3\mathrm{Ca\_o}-e^{\frac{(\mathrm{gamma}-1)FV}{RT}}\mathrm{Na\_o}^3\mathrm{Ca\_i})}{(\mathrm{K\_mNa}^3+\mathrm{Na\_o}^3)(\mathrm{K\_mCa}+\mathrm{Ca\_o})(1+\mathrm{K\_sat}e^{\frac{(\mathrm{gamma}-1)VF}{RT}})}$ $\frac{\mathrm{Cm}\mathrm{i\_CaP\_max}\mathrm{Ca\_i}}{0.0005+\mathrm{Ca\_i}}$ $\frac{\mathrm{u\_infinity}-u}{\mathrm{tau\_u}}$ $8$ $(1+e^{\frac{-(\mathrm{Fn}-3.4175E-13)}{13.67E-16}})^{-1}$ $\frac{\mathrm{v\_infinity}-v}{\mathrm{tau\_v}}$ $1.91+2.09(1+e^{\frac{-(\mathrm{Fn}-3.4175E-13)}{13.67E-16}})^{-1}$ $1-(1+e^{\frac{-(\mathrm{Fn}-6.835E-14)}{13.67E-16}})^{-1}$ $\frac{\mathrm{w\_infinity}-w}{\mathrm{tau\_w}}$ $\begin{cases}\frac{6\times 0.2}{1.3} & \text{if $\left|V-7.9\right|< 1E-10$}\\ \frac{6(1-e^{\frac{-(V-7.9)}{5}})}{(1+0.3e^{\frac{-(V-7.9)}{5}})\times 1(V-7.9)} & \text{otherwise}\end{cases}$ $1-(1+e^{\frac{-(V-40)}{17}})^{-1}$ $\mathrm{K\_rel}u^{2}vw(\mathrm{Ca\_rel}-\mathrm{Ca\_i})$ $1E3(1E-15\mathrm{V\_rel}\mathrm{i\_rel}-\frac{1E-15}{2F}(0.5\mathrm{i\_Ca\_L}-0.2\mathrm{i\_NaCa}))$ $\frac{\mathrm{Ca\_up}-\mathrm{Ca\_rel}}{\mathrm{tau\_tr}}$ $\frac{\mathrm{I\_up\_max}}{1+\frac{\mathrm{K\_up}}{\mathrm{Ca\_i}}}$ $\frac{\mathrm{I\_up\_max}\mathrm{Ca\_up}}{\mathrm{Ca\_up\_max}}$ $\frac{\mathrm{CMDN\_max}\mathrm{Ca\_i}}{\mathrm{Ca\_i}+\mathrm{Km\_CMDN}}$ $\frac{\mathrm{TRPN\_max}\mathrm{Ca\_i}}{\mathrm{Ca\_i}+\mathrm{Km\_TRPN}}$ $\frac{\mathrm{CSQN\_max}\mathrm{Ca\_rel}}{\mathrm{Ca\_rel}+\mathrm{Km\_CSQN}}$ $\frac{-3\mathrm{i\_NaK}-3\mathrm{i\_NaCa}+\mathrm{i\_B\_Na}+\mathrm{i\_Na}}{\mathrm{V\_i}F}$ $\frac{\mathrm{B1}}{\mathrm{B2}}$ $\frac{2\mathrm{i\_NaK}-\mathrm{i\_K1}+\mathrm{i\_to}+\mathrm{i\_Kur}+\mathrm{i\_Kr}+\mathrm{i\_Ks}+\mathrm{i\_B\_K}}{\mathrm{V\_i}F}$ $(\mathrm{i\_tr}-\mathrm{i\_rel})(1+\frac{\mathrm{CSQN\_max}\mathrm{Km\_CSQN}}{(\mathrm{Ca\_rel}+\mathrm{Km\_CSQN})^2})^{-1}$ $\mathrm{i\_up}-\mathrm{i\_up\_leak}+\frac{\mathrm{i\_tr}\mathrm{V\_rel}}{\mathrm{V\_up}}$ $\mathrm{V\_cell}\times 0.68$ $0.0048\mathrm{V\_cell}$ $0.0552\mathrm{V\_cell}$ $\frac{2\mathrm{i\_NaCa}-\mathrm{i\_CaP}+\mathrm{i\_Ca\_L}+\mathrm{i\_B\_Ca}}{2\mathrm{V\_i}F}+\frac{\mathrm{V\_up}(\mathrm{i\_up\_leak}-\mathrm{i\_up})+\mathrm{i\_rel}\mathrm{V\_rel}}{\mathrm{V\_i}}$ $1+\frac{\mathrm{TRPN\_max}\mathrm{Km\_TRPN}}{(\mathrm{Ca\_i}+\mathrm{Km\_TRPN})^2}+\frac{\mathrm{CMDN\_max}\mathrm{Km\_CMDN}}{(\mathrm{Ca\_i}+\mathrm{Km\_CMDN})^2}$ $\frac{\mathrm{d\_f\_infinity}-\mathrm{d\_f}}{\mathrm{tau\_d\_f}}$ $\frac{0.36(V+148.8)}{e^{0.066(V+148.8)}-1}$ $\frac{0.1(V+87.3)}{1-e^{-0.21(V+87.3)}}$ $\frac{1}{\mathrm{alpha\_d\_f}+\mathrm{beta\_d\_f}}$ $\frac{1}{\mathrm{alpha\_d\_f}+\mathrm{beta\_d\_f}}-0.054$ $\mathrm{g\_f}\mathrm{d\_f}(V-\mathrm{E\_f})$ $\frac{\mathrm{d\_T\_infinity}-\mathrm{d\_T}}{\mathrm{tau\_d\_T}}$ $1068e^{\frac{V+26.3}{30}}$ $1068e^{\frac{V+26.3}{-30}}$ $\frac{1}{1+e^{\frac{V+26.3}{-6}}}$ $\frac{1}{\mathrm{alpha\_d\_T}+\mathrm{beta\_d\_T}}$ $\frac{\mathrm{f\_T\_infinity}-\mathrm{f\_T}}{\mathrm{tau\_f\_T}}$ $15.3e^{\frac{V+61.7}{-83.3}}$ $15e^{\frac{V+61.7}{15.38}}$ $\frac{1}{1+e^{\frac{V+61.7}{5.6}}}$ $\frac{1}{\mathrm{alpha\_f\_T}+\mathrm{beta\_f\_T}}$ $\mathrm{g\_Ca\_T}\mathrm{d\_T}\mathrm{f\_T}(V-\mathrm{E\_Ca\_T})$ $\mathrm{alpha\_y}(1-y)-\mathrm{beta\_y}y$ $\begin{cases}0.0002475 & \text{if $\mathrm{ACh}=0$}\\ \frac{0.01232}{1+\frac{\mathrm{Km\_ACh}}{\mathrm{ACh}}}+0.0002475 & \text{otherwise}\end{cases}$ $0.01e^{0.0133(\mathrm{Vm}+40)}$ $\frac{\mathrm{g\_ACh}(\mathrm{Vm}-\mathrm{E\_K})}{1+e^{\frac{\mathrm{Vm}+20}{20}}}y$ $\frac{1000}{\frac{\mathrm{HR}}{60}}$ $\frac{\mathrm{realtime}-\mathrm{start}-\lfloor \frac{\mathrm{realtime}-\mathrm{start}}{\mathrm{hrf}}\rfloor \mathrm{hrf}}{1000}$ $\begin{cases}\mathrm{realtime} & \text{if $\mathrm{ISAin}< 0$}\end{cases}$ $\mathrm{TsK}\sqrt{\frac{\mathrm{hrf}}{1000}}$ $\begin{cases}\mathrm{Edia}+\frac{(\mathrm{Esys}-\mathrm{Edia})(1-\cos \left(\frac{\pi \mathrm{time\_}}{\mathrm{Ts}}\right))}{2} & \text{if $(\mathrm{time\_}\ge 0)\land (\mathrm{time\_}\le \mathrm{Ts})$}\\ \mathrm{Edia}+\frac{(\mathrm{Esys}-\mathrm{Edia})(1+\cos \left(\frac{2\pi (\mathrm{time\_}-\mathrm{Ts})}{\mathrm{Ts}}\right))}{2} & \text{if $(\mathrm{time\_}< 1.5\mathrm{Ts})\land (\mathrm{time\_}\ge \mathrm{Ts})$}\\ \mathrm{Edia} & \text{otherwise}\end{cases}$ $\frac{\mathrm{F\_LA}-\mathrm{F\_LV}}{1000}$ $\mathrm{E\_LA}(\mathrm{V\_LA}-\mathrm{V\_LA\_0})+\mathrm{P\_LA\_ext}$ $\frac{\mathrm{P\_PV}-\mathrm{P\_LA}}{\mathrm{R\_LA}}$ $\frac{\mathrm{sub\_X\_LA}}{\mathrm{V\_LA}}$ $\frac{\mathrm{conc\_X\_PV}\mathrm{F\_LA}-\mathrm{conc\_X\_LA}\mathrm{F\_LV}}{1000}$ $\frac{\mathrm{F\_LV}-\mathrm{F\_AO}-\mathrm{F\_CO}}{1000}$ $\begin{cases}\frac{\mathrm{P\_LA}-\mathrm{P\_LV}}{\mathrm{R\_LV}} & \text{if $\mathrm{P\_LA}> \mathrm{P\_LV}$}\\ 0 & \text{otherwise}\end{cases}$ $\frac{\mathrm{sub\_X\_LV}}{\mathrm{V\_LV}}$ $\frac{\mathrm{conc\_X\_LA}\mathrm{F\_LV}-\mathrm{conc\_X\_LV}(\mathrm{F\_AO}+\mathrm{F\_CO})}{1000}$ $\mathrm{P\_LVin}+\mathrm{P\_LA\_ext}$ $\frac{\mathrm{F\_AO}-\mathrm{F\_AR}-\mathrm{F\_CR}}{1000}$ $\frac{\frac{1}{\mathrm{L\_AO}}(\mathrm{P\_LV}-\mathrm{P\_AO})-\frac{\mathrm{R\_AO}}{\mathrm{L\_AO}}\mathrm{F\_AOalways}}{1000}$ $\begin{cases}\mathrm{F\_AOalways} & \text{if $\mathrm{P\_LV}> \mathrm{P\_AO}$}\\ 0 & \text{otherwise}\end{cases}$ $\frac{1}{\mathrm{C\_AO}}(\mathrm{V\_AO}-\mathrm{V\_AO\_0})$ $\frac{\mathrm{sub\_X\_AO}}{\mathrm{V\_AO}}$ $\frac{\mathrm{conc\_X\_LV}\mathrm{F\_AO}-\mathrm{conc\_X\_AO}(\mathrm{F\_CR}+\mathrm{F\_AR})}{1000}$ $\begin{cases}\frac{\mathrm{P\_LV}-\mathrm{P\_CO}}{\mathrm{R\_CO}} & \text{if $\mathrm{P\_LV}> \mathrm{P\_CO}$}\\ 0 & \text{otherwise}\end{cases}$ $\frac{\mathrm{P\_CO}-\mathrm{P\_RA}}{\mathrm{R\_COV}}$ $\frac{\mathrm{F\_CO}-\mathrm{F\_COV}}{1000}$ $\frac{1}{\mathrm{C\_CO}}(\mathrm{V\_CO}-\mathrm{V\_CO\_0})$ $\frac{\mathrm{sub\_X\_CO}}{\mathrm{V\_CO}}$ $\frac{\mathrm{conc\_X\_LV}\mathrm{F\_CO}-\mathrm{conc\_X\_CO}\mathrm{F\_COV}}{1000}$ $\frac{\mathrm{P\_AO}-\mathrm{P\_CR}}{\mathrm{R\_CR}}$ $\frac{\mathrm{P\_CR}-\mathrm{P\_VC}}{\mathrm{R\_CRV}}$ $\frac{\mathrm{F\_CR}-\mathrm{F\_CRV}}{1000}$ $\frac{1}{\mathrm{C\_CR}}(\mathrm{V\_CR}-\mathrm{V\_CR\_0})$ $\frac{\mathrm{sub\_X\_CR}}{\mathrm{V\_CR}}$ $\frac{\mathrm{conc\_X\_AO}\mathrm{F\_CR}-\mathrm{conc\_X\_CR}\mathrm{F\_CRV}-(\mathrm{conc\_X\_CR}-\mathrm{conc\_X\_CRtissue})\mathrm{D\_CRtissue}}{1000}$ $\frac{\mathrm{sub\_X\_CRtissue}}{\mathrm{V\_CRtissue}}$ $\frac{(\mathrm{conc\_X\_CR}-\mathrm{conc\_X\_CRtissue})\mathrm{D\_CRtissue}}{1000}$ $\frac{\mathrm{F\_AR}-\mathrm{F\_AD}-\mathrm{F\_MU}-\mathrm{F\_GI}-\mathrm{F\_LI}-\mathrm{F\_KI}-\mathrm{F\_OT}-\mathrm{F\_SK}}{1000}$ $\frac{\mathrm{P\_AO}-\mathrm{P\_AR}}{\mathrm{R\_AR}}$ $\frac{1}{\mathrm{C\_AR}}(\mathrm{V\_AR}-\mathrm{V\_AR\_0})$ $\frac{\mathrm{sub\_X\_AR}}{\mathrm{V\_AR}}$ $\frac{\mathrm{conc\_X\_AO}\mathrm{F\_AR}-\mathrm{conc\_X\_AR}(\mathrm{F\_SK}+\mathrm{F\_AD}+\mathrm{F\_MU}+\mathrm{F\_GI}+\mathrm{F\_LI}+\mathrm{F\_KI}+\mathrm{F\_OT})}{1000}$ $\frac{\mathrm{F\_AD}-\mathrm{F\_ADV}}{1000}$ $\frac{\mathrm{P\_AR}-\mathrm{P\_AD}}{\mathrm{R\_AD}}$ $\frac{\mathrm{P\_AD}-\mathrm{P\_VE}}{\mathrm{R\_ADV}}$ $\frac{1}{\mathrm{C\_AD}}(\mathrm{V\_AD}-\mathrm{V\_AD\_0})$ $\frac{\mathrm{sub\_X\_AD}}{\mathrm{V\_AD}}$ $\frac{\mathrm{conc\_X\_AR}\mathrm{F\_AD}-\mathrm{conc\_X\_AD}\mathrm{F\_ADV}}{1000}$ $\frac{\mathrm{F\_MU}-\mathrm{F\_MUV}}{1000}$ $\frac{\mathrm{P\_AR}-\mathrm{P\_MU}}{\mathrm{R\_MU}}$ $\frac{\mathrm{P\_MU}-\mathrm{P\_VE}}{\mathrm{R\_MUV}}$ $\frac{1}{\mathrm{C\_MU}}(\mathrm{V\_MU}-\mathrm{V\_MU\_0})$ $\frac{\mathrm{sub\_X\_MU}}{\mathrm{V\_MU}}$ $\frac{\mathrm{conc\_X\_AR}\mathrm{F\_MU}-\mathrm{conc\_X\_MU}\mathrm{F\_MUV}}{1000}$ $\frac{\mathrm{F\_GI}-\mathrm{F\_GIV}}{1000}$ $\frac{\mathrm{P\_AR}-\mathrm{P\_GI}}{\mathrm{R\_GI}}$ $\frac{\mathrm{P\_GI}-\mathrm{P\_LI}}{\mathrm{R\_GIV}}$ $\frac{1}{\mathrm{C\_GI}}(\mathrm{V\_GI}-\mathrm{V\_GI\_0})$ $\frac{\mathrm{sub\_X\_GI}}{\mathrm{V\_GI}}$ $\frac{\mathrm{conc\_X\_AR}\mathrm{F\_GI}-\mathrm{conc\_X\_GI}\mathrm{F\_GIV}}{1000}$ $\frac{\mathrm{F\_GIV}+\mathrm{F\_LI}-\mathrm{F\_LIV}}{1000}$ $\frac{\mathrm{P\_AR}-\mathrm{P\_LI}}{\mathrm{R\_LI}}$ $\frac{\mathrm{P\_LI}-\mathrm{P\_VE}}{\mathrm{R\_LIV}}$ $\frac{1}{\mathrm{C\_LI}}(\mathrm{V\_LI}-\mathrm{V\_LI\_0})$ $\frac{\mathrm{sub\_X\_LI}}{\mathrm{V\_LI}}$ $\frac{\mathrm{conc\_X\_GI}\mathrm{F\_GIV}+\mathrm{conc\_X\_AR}\mathrm{F\_LI}-\mathrm{conc\_X\_LI}\mathrm{F\_LIV}+\mathrm{conc\_X\_LI}\mathrm{metabolism}}{1000}$ $\frac{\mathrm{F\_KI}-\mathrm{F\_KIV}}{1000}$ $\frac{\mathrm{P\_AR}-\mathrm{P\_KI}}{\mathrm{R\_KI}}$ $\frac{\mathrm{P\_KI}-\mathrm{P\_VE}}{\mathrm{R\_KIV}}$ $\frac{1}{\mathrm{C\_KI}}(\mathrm{V\_KI}-\mathrm{V\_KI\_0})$ $\frac{\mathrm{sub\_X\_KI}}{\mathrm{V\_KI}}$ $\frac{\mathrm{conc\_X\_AR}\mathrm{F\_KI}-\mathrm{conc\_X\_KI}\mathrm{F\_KIV}}{1000}$ $\frac{\mathrm{F\_SK}-\mathrm{F\_SKV}}{1000}$ $\frac{\mathrm{P\_AR}-\mathrm{P\_SK}}{\mathrm{R\_SK}}$ $\frac{\mathrm{P\_SK}-\mathrm{P\_VE}}{\mathrm{R\_SKV}}$ $\frac{1}{\mathrm{C\_SK}}(\mathrm{V\_SK}-\mathrm{V\_SK\_0})$ $\frac{\mathrm{sub\_X\_SK}}{\mathrm{V\_SK}}$ $\frac{\mathrm{conc\_X\_AR}\mathrm{F\_SK}-\mathrm{conc\_X\_SK}\mathrm{F\_SKV}}{1000}$ $\frac{\mathrm{F\_OT}-\mathrm{F\_OTV}}{1000}$ $\frac{\mathrm{P\_AR}-\mathrm{P\_OT}}{\mathrm{R\_OT}}$ $\frac{\mathrm{P\_OT}-\mathrm{P\_VE}}{\mathrm{R\_OTV}}$ $\frac{1}{\mathrm{C\_OT}}(\mathrm{V\_OT}-\mathrm{V\_OT\_0})$ $\frac{\mathrm{sub\_X\_OT}}{\mathrm{V\_OT}}$ $\frac{\mathrm{conc\_X\_AR}\mathrm{F\_OT}-\mathrm{conc\_X\_OT}\mathrm{F\_OTV}}{1000}$ $\frac{\mathrm{F\_VE}-\mathrm{F\_VEV}}{1000}$ $\mathrm{F\_SKV}+\mathrm{F\_ADV}+\mathrm{F\_MUV}+\mathrm{F\_LIV}+\mathrm{F\_KIV}+\mathrm{F\_OTV}$ $\frac{\mathrm{P\_VE}-\mathrm{P\_VC}}{\mathrm{R\_VEV}}$ $\frac{1}{\mathrm{C\_VE}}(\mathrm{V\_VE}-\mathrm{V\_VE\_0})$ $\frac{\mathrm{sub\_X\_VE}}{\mathrm{V\_VE}}$ $\frac{\mathrm{conc\_X\_SK}\mathrm{F\_SKV}+\mathrm{conc\_X\_AD}\mathrm{F\_ADV}+\mathrm{conc\_X\_MU}\mathrm{F\_MUV}+\mathrm{conc\_X\_LI}\mathrm{F\_LIV}+\mathrm{conc\_X\_KI}\mathrm{F\_KIV}+\mathrm{conc\_X\_OT}\mathrm{F\_OTV}-\mathrm{conc\_X\_VE}\mathrm{F\_VEV}}{1000}$ $\frac{\mathrm{F\_VC}-\mathrm{F\_VCV}}{1000}$ $\mathrm{F\_CRV}+\mathrm{F\_VEV}$ $\frac{\mathrm{P\_VC}-\mathrm{P\_RA}}{\mathrm{R\_VCV}}$ $\frac{1}{\mathrm{C\_VC}}(\mathrm{V\_VC}-\mathrm{V\_VC\_0})$ $\frac{\mathrm{sub\_X\_VC}}{\mathrm{V\_VC}}$ $\frac{\mathrm{conc\_X\_VE}\mathrm{F\_VEV}+\mathrm{conc\_X\_CR}\mathrm{F\_CRV}-\mathrm{conc\_X\_VC}\mathrm{F\_VCV}}{1000}$ $\frac{\mathrm{realtime}-\mathrm{start}-\lfloor \frac{\mathrm{realtime}-\mathrm{start}}{\mathrm{hrf}}\rfloor \mathrm{hrf}}{1000}$ $\begin{cases}\mathrm{realtime} & \text{if $\mathrm{ISAin}< 0$}\end{cases}$ $\mathrm{TsK}\sqrt{\frac{\mathrm{hrf}}{1000}}$ $\begin{cases}\mathrm{Edia}+\frac{(\mathrm{Esys}-\mathrm{Edia})(1-\cos \left(\frac{\pi \mathrm{time\_}}{\mathrm{Ts}}\right))}{2} & \text{if $(\mathrm{time\_}\ge 0)\land (\mathrm{time\_}\le \mathrm{Ts})$}\\ \mathrm{Edia}+\frac{(\mathrm{Esys}-\mathrm{Edia})(1+\cos \left(\frac{2\pi (\mathrm{time\_}-\mathrm{Ts})}{\mathrm{Ts}}\right))}{2} & \text{if $(\mathrm{time\_}< 1.5\mathrm{Ts})\land (\mathrm{time\_}\ge \mathrm{Ts})$}\\ \mathrm{Edia} & \text{otherwise}\end{cases}$ $\frac{\mathrm{F\_RA}-\mathrm{F\_RV}}{1000}$ $\mathrm{E\_RA}(\mathrm{V\_RA}-\mathrm{V\_RA\_0})+\mathrm{P\_RA\_ext}$ $\mathrm{F\_VCV}+\mathrm{F\_COV}$ $\frac{\mathrm{sub\_X\_RA}}{\mathrm{V\_RA}}$ $\frac{\mathrm{conc\_X\_VC}\mathrm{F\_VCV}+\mathrm{conc\_X\_CO}\mathrm{F\_COV}-\mathrm{conc\_X\_RA}\mathrm{F\_RV}}{1000}$ $\frac{\mathrm{F\_RV}-\mathrm{F\_PA}}{1000}$ $\frac{(\mathrm{P\_LV}-\mathrm{lvb})\mathrm{rva}}{\mathrm{lva}-\mathrm{lvb}}+\frac{(\mathrm{lva}-\mathrm{P\_LV})\mathrm{rvb}}{\mathrm{lva}-\mathrm{lvb}}$ $\begin{cases}\frac{\mathrm{P\_RA}-\mathrm{P\_RV}}{\mathrm{R\_RV}} & \text{if $\mathrm{P\_RA}> \mathrm{P\_RV}$}\\ 0 & \text{otherwise}\end{cases}$ $\frac{\mathrm{sub\_X\_RV}}{\mathrm{V\_RV}}$ $\frac{\mathrm{conc\_X\_RA}\mathrm{F\_RV}-\mathrm{conc\_X\_RV}\mathrm{F\_PA}}{1000}$ $\mathrm{EmaxLV}\times 10$ $\mathrm{EmaxRV}\times 10$ $\mathrm{P0lv}(e^{\mathrm{kelv}\mathrm{V\_LV}}-1)$ $\mathrm{P0rv}(e^{\mathrm{kerv}\mathrm{V\_RV}}-1)$ $\begin{cases}\frac{\mathrm{P\_RV}-\mathrm{P\_PA}}{\mathrm{R\_PA}} & \text{if $\mathrm{P\_RV}> \mathrm{P\_PA}$}\\ 0 & \text{otherwise}\end{cases}$ $\frac{\mathrm{F\_PA}-\mathrm{F\_Pa}}{1000}$ $\frac{1}{\mathrm{C\_PA}}(\mathrm{V\_PA}-\mathrm{V\_PA\_0})$ $\frac{\mathrm{sub\_X\_PA}}{\mathrm{V\_PA}}$ $\frac{\mathrm{conc\_X\_RV}\mathrm{F\_PA}-\mathrm{conc\_X\_PA}\mathrm{F\_Pa}}{1000}$ $\frac{\mathrm{F\_Pa}-\mathrm{F\_PC}-\mathrm{F\_SH}}{1000}$ $\frac{\mathrm{P\_PA}-\mathrm{P\_Pa}}{\mathrm{R\_Pa}}$ $\frac{1}{\mathrm{C\_Pa}}(\mathrm{V\_Pa}-\mathrm{V\_Pa\_0})$ $\frac{\mathrm{sub\_X\_Pa}}{\mathrm{V\_Pa}}$ $\frac{\mathrm{conc\_X\_PA}\mathrm{F\_Pa}-\mathrm{conc\_X\_Pa}(\mathrm{F\_PC}+\mathrm{F\_SH})}{1000}$ $\frac{\mathrm{P\_Pa}-\mathrm{P\_PC}}{\mathrm{R\_SH}}$ $\frac{\mathrm{F\_PC}-\mathrm{F\_PCV}}{1000}$ $\frac{\mathrm{P\_Pa}-\mathrm{P\_PC}}{\mathrm{R\_PC}}$ $\frac{\mathrm{P\_PC}-\mathrm{P\_PV}}{\mathrm{R\_PCV}}$ $\frac{1}{\mathrm{C\_PC}}(\mathrm{V\_PC}-\mathrm{V\_PC\_0})$ $\frac{\mathrm{sub\_X\_PC}}{\mathrm{V\_PC}}$ $\frac{\mathrm{conc\_X\_Pa}\mathrm{F\_PC}-\mathrm{conc\_X\_PC}\mathrm{F\_PCV}}{1000}$ $\frac{\mathrm{F\_PV}-\mathrm{F\_LA}}{1000}$ $\mathrm{F\_PCV}+\mathrm{F\_SH}$ $\frac{1}{\mathrm{C\_PV}}(\mathrm{V\_PV}-\mathrm{V\_PV\_0})$ $\frac{\mathrm{sub\_X\_PV}}{\mathrm{V\_PV}}$ $\frac{\mathrm{conc\_X\_PC}\mathrm{F\_PCV}+\mathrm{conc\_X\_Pa}\mathrm{F\_SH}-\mathrm{conc\_X\_PV}\mathrm{F\_LA}}{1000}$ $-\mathrm{Istim}$ $\mathrm{topOUt}-\mathrm{Cai}$ $\frac{-\mathrm{Itotal}}{\mathrm{Cm}}$ $\mathrm{ISAstim}+\mathrm{ICa\_additional}+\mathrm{INa\_additional}+\mathrm{IK\_additional}+\mathrm{INa}+\mathrm{IK1}+\mathrm{Ito}+\mathrm{IKr}+\mathrm{IKs}+\mathrm{ICaL}+\mathrm{INaCa}+\mathrm{INaK}+\mathrm{IbNa}+\mathrm{IbCa}+\mathrm{IpCa}+\mathrm{IpK}$ $\frac{\mathrm{Am}}{\mathrm{vC}F}(\mathrm{IK\_additional}+\mathrm{IK1}+\mathrm{Ito}+\mathrm{IKr}+\mathrm{IKs}+\mathrm{IpK}-\mathrm{INaK}\times 2)$ $\frac{\mathrm{Am}}{\mathrm{vC}F}(\mathrm{INa}+\mathrm{INa\_additional}+\mathrm{IbNa}+\mathrm{INaK}\times 3+\mathrm{INaCa}\times 3)$ $\frac{\mathrm{Am}}{2\mathrm{vC}F}(2\mathrm{INaCa}-\mathrm{ICa\_additional}+\mathrm{ICaL}+\mathrm{IbCa}+\mathrm{IpCa})$ $\mathrm{Jleak}+\mathrm{Jrel}+\mathrm{JCaSR\_additional}-\mathrm{Jup}$ $\mathrm{g\_Na}m^{3}hj(V-\mathrm{E\_Na})$ $\mathrm{g\_K1}\sqrt{\frac{\mathrm{Ko}}{5.4}}\mathrm{K1\_infinity}(V-\mathrm{E\_K})$ $\mathrm{g\_to}rs(V-\mathrm{E\_K})$ $\mathrm{g\_Kr}\sqrt{\frac{\mathrm{Ko}}{5.4}}\mathrm{Xr1}\mathrm{Xr2}(V-\mathrm{E\_K})$ $\mathrm{g\_Ks}\mathrm{Xs}^2(V-\mathrm{E\_Ks})$ $\frac{\mathrm{P\_NaK}\mathrm{Ko}\mathrm{Nai}}{(\mathrm{Ko}+\mathrm{K\_mK})(\mathrm{Nai}+\mathrm{K\_mNa})(1+0.1245e^{\frac{-0.1VF}{RT}}+0.0353e^{\frac{-VF}{RT}})}$ $\frac{\mathrm{g\_pK}(V-\mathrm{E\_K})}{1+e^{\frac{25-V}{5.98}}}$ $\mathrm{g\_bNa}(V-\mathrm{E\_Na})$ $\frac{\frac{\mathrm{g\_CaL}df\mathrm{fCa}\times 4VF^2}{RT}(\mathrm{Cai}e^{\frac{2VF}{RT}}-0.341\mathrm{Cao})}{e^{\frac{2VF}{RT}}-1}$ $\frac{\mathrm{g\_pCa}\mathrm{Cai}}{\mathrm{K\_pCa}+\mathrm{Cai}}$ $\frac{\mathrm{k\_NaCa}(e^{\frac{\mathrm{gamma}VF}{RT}}\mathrm{Nai}^3\mathrm{Cao}-e^{\frac{(\mathrm{gamma}-1)VF}{RT}}\mathrm{Nao}^3\mathrm{Cai}\mathrm{alpha})}{(\mathrm{K\_mNai}^3+\mathrm{Nao}^3)(\mathrm{K\_mCa}+\mathrm{Cao})(1+\mathrm{k\_sat}e^{\frac{(\mathrm{gamma}-1)VF}{RT}})}$ $\mathrm{g\_bCa}(V-\mathrm{E\_Ca})$ $\frac{RT}{zF}\ln \left(\frac{\mathrm{extracellular\_concentration}}{\mathrm{intracellular\_concentration}}\right)$ $\frac{RT}{zF}\ln \left(\frac{\mathrm{extracellular\_concentration}}{\mathrm{intracellular\_concentration}}\right)$ $\frac{RT}{zF}\ln \left(\frac{\mathrm{extracellular\_concentration}}{\mathrm{intracellular\_concentration}}\right)$ $\frac{RT}{zF}\ln \left(\frac{\mathrm{multiplier\_1}\mathrm{extracellular\_concentration\_1}+\mathrm{multiplier\_2}\mathrm{extracellular\_concentration\_2}}{\mathrm{multiplier\_1}\mathrm{intracellular\_concentration\_1}+\mathrm{multiplier\_2}\mathrm{intracellular\_concentration\_2}}\right)$ $-\mathrm{Na\_flux}$ $-\mathrm{K\_flux}$ $\mathrm{Cai\_total}-\mathrm{Cai\_buf}$ $\mathrm{CaSR\_total}-\mathrm{CaSR\_buf}$ $\mathrm{Ca\_flux}+\mathrm{Ca\_SR\_flux}$ $\frac{\mathrm{vC}}{\mathrm{vSR}}-\mathrm{Ca\_SR\_flux}$ $\frac{\sqrt{\mathrm{bCai}^2-4\mathrm{aCai}\mathrm{cCai}}-\mathrm{bCai}}{2\mathrm{aCai}}$ $\frac{\sqrt{\mathrm{bCaSR}^2-4\mathrm{aCaSR}\mathrm{cCaSR}}-\mathrm{bCaSR}}{2\mathrm{aCaSR}}$ $-1$ $\mathrm{Cai\_total}+\mathrm{Kbufc}+\mathrm{Bufc}$ $-\mathrm{Bufc}\mathrm{Cai\_total}$ $-1$ $\mathrm{CaSR\_total}+\mathrm{Kbufsr}+\mathrm{Bufsr}$ $-\mathrm{Bufsr}\mathrm{CaSR\_total}$ $\mathrm{V\_leak}(\mathrm{CaSR}-\mathrm{Cai})$ $\frac{\mathrm{Vmax\_up}}{1+\frac{\mathrm{K\_up}^2}{\mathrm{Cai}^2}}$ $(\frac{\mathrm{a\_rel}\mathrm{CaSR}^2}{\mathrm{b\_rel}^2+\mathrm{CaSR}^2}+\mathrm{c\_rel})dg$ $\frac{\mathrm{m\_infinity}-m}{\mathrm{tau\_m}}$ $1\mathrm{alpha\_m}\mathrm{beta\_m}$ $\frac{1}{(1+e^{\frac{-56.86-V}{9.03}})^2}$ $\frac{1}{1+e^{\frac{-60-V}{5}}}$ $\frac{0.1}{1+e^{\frac{35+V}{5}}}+\frac{0.1}{1+e^{\frac{V-50}{200}}}$ $\frac{\mathrm{h\_infinity}-h}{\mathrm{tau\_h}}$ $\frac{1}{\mathrm{alpha\_h}+\mathrm{beta\_h}}$ $\frac{1}{(1+e^{\frac{71.55+V}{7.43}})^2}$ $\begin{cases}0.057e^{\frac{-(80+V)}{6.8}} & \text{if $V< -40$}\\ 0 & \text{otherwise}\end{cases}$ $\begin{cases}2.7e^{0.079V}+3.1E5e^{0.3485V} & \text{if $V< -40$}\\ \frac{0.77}{0.13(1+e^{\frac{-(V+10.66)}{11.1}})} & \text{otherwise}\end{cases}$ $\frac{\mathrm{j\_infinity}-j}{\mathrm{tau\_j}}$ $\frac{1}{\mathrm{alpha\_j}+\mathrm{beta\_j}}$ $\frac{1}{(1+e^{\frac{71.55+V}{7.43}})^2}$ $\begin{cases}\frac{(-2.5428E4e^{0.2444V}-6.948E-6e^{-0.04391V})(V+37.78)}{1+e^{0.311(V+79.23)}} & \text{if $V< -40$}\\ 0 & \text{otherwise}\end{cases}$ $\begin{cases}\frac{0.02424e^{-0.01052V}}{1+e^{-0.1378(V+40.14)}} & \text{if $V< -40$}\\ \frac{0.6e^{0.057V}}{1+e^{-0.1(V+32)}} & \text{otherwise}\end{cases}$ $\frac{\mathrm{alpha\_K1}}{\mathrm{alpha\_K1}+\mathrm{beta\_K1}}$ $\frac{0.1}{1+e^{0.06(V-\mathrm{E\_K}+200)}}$ $\frac{3e^{0.0002(V-\mathrm{E\_K}+100)}+e^{0.1(V-\mathrm{E\_K}+10)}}{1+e^{-0.5(V-\mathrm{E\_K})}}$ $\frac{\mathrm{r\_infinity}-r}{\mathrm{tau\_r}}$ $\frac{1}{1+e^{\frac{20-V}{6}}}$ $9.5e^{\frac{-(V+40)^2}{1800}}+0.8$ $\frac{\mathrm{s\_infinity}-s}{\mathrm{tau\_s}}$ $\frac{1}{1+e^{\frac{20+V}{5}}}$ $85e^{\frac{-(V+45)^2}{320}}+\frac{5}{1+e^{\frac{V-20}{5}}}+3$ $\frac{\mathrm{Xr1\_infinity}-\mathrm{Xr1}}{\mathrm{tau\_Xr1}}$ $\frac{450}{1+e^{\frac{-45-V}{10}}}$ $\frac{6}{1+e^{\frac{V+30}{11.5}}}$ $\frac{1}{1+e^{\frac{-26-V}{7}}}$ $1\mathrm{alpha\_Xr1}\mathrm{beta\_Xr1}$ $\frac{\mathrm{Xr2\_infinity}-\mathrm{Xr2}}{\mathrm{tau\_Xr2}}$ $\frac{3}{1+e^{\frac{-60-V}{20}}}$ $\frac{1.12}{1+e^{\frac{V-60}{20}}}$ $\frac{1}{1+e^{\frac{88+V}{24}}}$ $1\mathrm{alpha\_Xr2}\mathrm{beta\_Xr2}$ $\frac{\mathrm{Xs\_infinity}-\mathrm{Xs}}{\mathrm{tau\_Xs}}$ $\frac{1100}{\sqrt{1+e^{\frac{-10-V}{6}}}}$ $\frac{1}{1+e^{\frac{V-60}{20}}}$ $\frac{1}{1+e^{\frac{-5-V}{14}}}$ $1\mathrm{alpha\_Xs}\mathrm{beta\_Xs}$ $\frac{\mathrm{d\_infinity}-d}{\mathrm{tau\_d}}$ $\frac{1.4}{1+e^{\frac{-35-V}{13}}}+0.25$ $\frac{1.4}{1+e^{\frac{5+V}{5}}}$ $1\mathrm{alpha\_d}\mathrm{beta\_d}+\mathrm{gamma\_d}$ $\frac{1}{1+e^{\frac{50-V}{20}}}$ $\frac{1}{1+e^{\frac{-5-V}{7.5}}}$ $\frac{\mathrm{f\_infinity}-f}{\mathrm{tau\_f}}$ $1125e^{\frac{-(V+27)^2}{240}}+\frac{165}{1+e^{\frac{25-V}{10}}}+80$ $\frac{1}{1+e^{\frac{20+V}{7}}}$ $\begin{cases}0 & \text{if $(\mathrm{fCa\_infinity}> \mathrm{fCa})\land (V> -60)$}\\ \frac{\mathrm{fCa\_infinity}-\mathrm{fCa}}{\mathrm{tau\_fCa}} & \text{otherwise}\end{cases}$ $\frac{1}{1+\left(\frac{\mathrm{Cai}}{0.000325}\right)^8}$ $\frac{0.1}{1+e^{\frac{\mathrm{Cai}-0.0005}{0.0001}}}$ $\frac{0.2}{1+e^{\frac{\mathrm{Cai}-0.00075}{0.0008}}}$ $\frac{\mathrm{alpha\_fCa}+\mathrm{beta\_fCa}+\mathrm{gamma\_fCa}+0.23}{1.46}$ $\begin{cases}0 & \text{if $(\mathrm{g\_infinity}> g)\land (V> -60)$}\\ \frac{\mathrm{g\_infinity}-g}{\mathrm{tau\_g}} & \text{otherwise}\end{cases}$ $\begin{cases}\frac{1}{1+\frac{\mathrm{Cai}^6}{0.00035^6}} & \text{if $\mathrm{Cai}\le 0.00035$}\\ \frac{1}{1+\frac{\mathrm{Cai}^{16}}{0.00035^{16}}} & \text{otherwise}\end{cases}$ $\frac{10000\times 2\pi \mathrm{radiusLV}}{\mathrm{xDen}}$ $\mathrm{ForceP}+\mathrm{ForceB}$ $\frac{\mathrm{cTnCa}}{e^{R(\mathrm{xHalfSL}-\mathrm{OptiHSL})^2}}$ $\mathrm{Q\_b}\times 1-\mathrm{Q\_a}\times 1$ $\mathrm{Q\_a}\times 1-\mathrm{Q\_r}\times 1-\mathrm{Q\_d1}\times 1$ $\mathrm{Q\_r}\times 1-\mathrm{Q\_d}\times 1-\mathrm{Q\_d2}\times 1$ $\frac{\mathrm{Y\_2}\mathrm{cTnCaEff}}{1}-\frac{\mathrm{Z\_2}\mathrm{cTnCaCB}}{1}$ $\frac{\mathrm{Y\_1}\mathrm{Cai}\mathrm{cTn}}{1}-\frac{\mathrm{Z\_1}\mathrm{cTnCa}}{1}$ $\frac{\mathrm{Y\_3}\mathrm{cTnCaCB}}{1}-\frac{\mathrm{Z\_3}\mathrm{cTnCB}\mathrm{Cai}}{1}$ $\frac{\mathrm{Y\_4}\mathrm{cTnCB}}{1}$ $\frac{\mathrm{Y\_d}(\mathrm{SlidingR}(\mathrm{xHalfSL}-\mathrm{xInext}-\mathrm{xLLimitCB}))^2\mathrm{cTnCaCB}}{1}$ $\frac{\mathrm{Y\_d}(\mathrm{SlidingR}(\mathrm{xHalfSL}-\mathrm{xInext}-\mathrm{xLLimitCB}))^2\mathrm{cTnCB}}{1}$ $\mathrm{SlidingR}(\mathrm{xHalfSL}-\mathrm{xInext}-\mathrm{xLLimitCB})$ $1-\mathrm{cTnCa}-\mathrm{cTnCaCB}-\mathrm{cTnCB}$ $\frac{\mathrm{trpnbar}(\mathrm{Q\_r}+\mathrm{Q\_d2}-\mathrm{Q\_b})}{1}$ $\mathrm{xHalfSL}-\mathrm{xInext}$ $\frac{(\mathrm{cTnCaCB}+\mathrm{cTnCB})\mathrm{trpnbar}}{1}$ $\frac{\mathrm{AForceCB}(\mathrm{cTnCaCB}+\mathrm{cTnCB})\mathrm{trpnbar}}{1}$ $\begin{cases}\mathrm{xKcoeff}(\mathrm{xHalfSL}-0.97)^5 & \text{if $\mathrm{xHalfSL}> 0.97$}\\ \mathrm{xKcoeff2}(\mathrm{xHalfSL}-0.97) & \text{otherwise}\end{cases}$ $\mathrm{xNewCBF}\mathrm{xhhh}$ $\left(\frac{\frac{3\mathrm{V\_LV}}{2}}{\pi }\right)^{\left(\frac{1}{3}\right)}$ $\mathrm{ForceExt}\mathrm{Fmult}$ $\frac{\frac{2\mathrm{Tension}}{\mathrm{radiusLV}}\times 1000}{133}-\mathrm{offset}$ $\mathrm{Cai\_in}$ $\mathrm{F\_PC}\times 0.06$ $\mathrm{F\_MU}\times 0.06$ $\mathrm{V\_PC}$ $\mathrm{V\_MU}$ $\frac{\mathrm{Fpc}(\mathrm{CtO2\_sc}-\mathrm{CtO2\_pc})+\mathrm{DL\_O2}(\mathrm{PA\_O2}-\mathrm{PO2\_pc})\times 0.00267857142857143}{\mathrm{Vpc}(\mathrm{alphaO2}+H\mathrm{CHb}\mathrm{dSHbO2dPO2\_pc})}\times 0.0166666666666667$ $\frac{\mathrm{Fsc}(\mathrm{CtO2\_pc}-\mathrm{CtO2\_sc})+\mathrm{PS}\mathrm{alphaO2}(\mathrm{PO2\_isf}-\mathrm{PO2\_sc})\times 10E-4}{\mathrm{Vsc}(\mathrm{alphaO2}+H\mathrm{CHb}\mathrm{dSHbO2dPO2\_sc})}\times 0.0166666666666667$ $\frac{\left(\frac{\mathrm{PO2\_pc}}{\mathrm{P50\_O2}}\right)^{\mathrm{nH}}}{\left(\frac{\mathrm{PO2\_pc}}{\mathrm{P50\_O2}}\right)^{\mathrm{nH}}+1}$ $\frac{\left(\frac{\mathrm{PO2\_sc}}{\mathrm{P50\_O2}}\right)^{\mathrm{nH}}}{\left(\frac{\mathrm{PO2\_sc}}{\mathrm{P50\_O2}}\right)^{\mathrm{nH}}+1}$ $\frac{\mathrm{nH}\mathrm{PO2\_pc}^{-1}\left(\frac{\mathrm{PO2\_pc}}{\mathrm{P50\_O2}}\right)^{\mathrm{nH}}}{(\left(\frac{\mathrm{PO2\_pc}}{\mathrm{P50\_O2}}\right)^{\mathrm{nH}}+1)^2}$ $\frac{\mathrm{nH}\mathrm{PO2\_sc}^{-1}\left(\frac{\mathrm{PO2\_sc}}{\mathrm{P50\_O2}}\right)^{\mathrm{nH}}}{(\left(\frac{\mathrm{PO2\_sc}}{\mathrm{P50\_O2}}\right)^{\mathrm{nH}}+1)^2}$ $\mathrm{alphaO2}\mathrm{PO2\_pc}+\mathrm{CHb}\mathrm{SHbO2\_pc}H$ $\mathrm{alphaO2}\mathrm{PO2\_sc}+\mathrm{CHb}\mathrm{SHbO2\_sc}H$ $\begin{cases}(\frac{\mathrm{QdotCA}\mathrm{PC\_O2}-\mathrm{PA\_O2}\mathrm{dVAdt}\times 1000000}{\mathrm{VA}}-\frac{\frac{\mathrm{Pstp}\mathrm{Tbody}}{\mathrm{Tstp}}\mathrm{O2flux}}{\mathrm{VA}}\times 0.0166666666666667)\times 1E-6 & \text{if $\mathrm{dVAdt}> 0$}\\ (\frac{\mathrm{QdotCA}\mathrm{PA\_O2}-\mathrm{PA\_O2}\mathrm{dVAdt}\times 1000000}{\mathrm{VA}}-\frac{\frac{\mathrm{Pstp}\mathrm{Tbody}}{\mathrm{Tstp}}\mathrm{O2flux}}{\mathrm{VA}}\times 0.0166666666666667)\times 1E-6 & \text{otherwise}\end{cases}$ $(\sqrt{\frac{\mathrm{Vpc}}{\mathrm{Vpcmax}}}(0.397+0.0085\mathrm{PO2\_pc}-1.3E-4\mathrm{PO2\_pc}^2)+5.1E-7\mathrm{PO2\_pc}^3\times 31.6227766016838)\times 0.0316227766016838$ $(\frac{\mathrm{PS}(\mathrm{PO2\_sc}-\mathrm{PO2\_isf})}{\mathrm{Visf}}-\frac{\mathrm{V\_O2}}{\mathrm{alphaO2}\mathrm{Visf}}\times 1E3)\times 1.66666666666667E-5$ $\frac{\mathrm{Vcytox}\mathrm{alphaO2}\mathrm{PO2\_isf}}{\mathrm{Kcytox}+\mathrm{alphaO2}\mathrm{PO2\_isf}}$ $\mathrm{DL\_O2}(\mathrm{PA\_O2}-\mathrm{PO2\_pc})\times 22400\times 0.00267857142857143$ $\frac{\mathrm{Fpc}(\mathrm{CtCO2\_sc}-\mathrm{CtCO2\_pc})+\mathrm{DL\_CO2}(\mathrm{PA\_CO2}-\mathrm{PCO2\_pc})\times 0.00267857142857143}{\mathrm{Vpc}(\mathrm{alphaCO2}+H\mathrm{CHb}\mathrm{dSHbCO2dPCO2\_pc})}\times 0.0166666666666667$ $\frac{\mathrm{Fsc}(\mathrm{CtCO2\_pc}-\mathrm{CtCO2\_sc})+\mathrm{PS}\mathrm{alphaCO2}(\mathrm{PCO2\_isf}-\mathrm{PCO2\_sc})\times 10E-4}{\mathrm{Vsc}(\mathrm{alphaCO2}+H\mathrm{CHb}\mathrm{dSHbCO2dPCO2\_sc})}\times 0.0166666666666667$ $\frac{\frac{\mathrm{PCO2\_pc}}{\mathrm{P50\_CO2}}}{\frac{\mathrm{PO2\_pc}}{\mathrm{P50\_CO2}}+1}$ $\frac{\frac{\mathrm{PCO2\_sc}}{\mathrm{P50\_CO2}}}{\frac{\mathrm{PCO2\_sc}}{\mathrm{P50\_CO2}}+1}$ $\frac{\frac{\mathrm{PCO2\_pc}^{-1}\mathrm{PCO2\_pc}}{\mathrm{P50\_CO2}}}{(\frac{\mathrm{PCO2\_pc}}{\mathrm{P50\_CO2}}+1)^2}$ $\mathrm{alphaCO2}\mathrm{PCO2\_pc}+\mathrm{CHb}\mathrm{SHbCO2\_pc}H$ $\frac{\frac{\mathrm{PCO2\_sc}^{-1}\mathrm{PCO2\_sc}}{\mathrm{P50\_CO2}}}{(\frac{\mathrm{PCO2\_sc}}{\mathrm{P50\_CO2}}+1)^2}$ $\mathrm{alphaCO2}\mathrm{PCO2\_sc}+\mathrm{CHb}\mathrm{SHbCO2\_sc}H$ $\begin{cases}(\frac{\mathrm{QdotCA}\mathrm{PC\_CO2}-\mathrm{PA\_CO2}\mathrm{dVAdt}\times 1000000}{\mathrm{VA}}-\frac{\frac{\mathrm{Pstp}\mathrm{Tbody}}{\mathrm{Tstp}}\mathrm{CO2flux}}{\mathrm{VA}}\times 0.0166666666666667)\times 1E-6 & \text{if $\mathrm{dVAdt}> 0$}\\ (\frac{\mathrm{QdotCA}\mathrm{PA\_CO2}-\mathrm{PA\_CO2}\mathrm{dVAdt}\times 1000000}{\mathrm{VA}}-\frac{\frac{\mathrm{Pstp}\mathrm{Tbody}}{\mathrm{Tstp}}\mathrm{CO2flux}}{\mathrm{VA}}\times 0.0166666666666667)\times 1E-6 & \text{otherwise}\end{cases}$ $\sqrt{\frac{\mathrm{Vpc}}{\mathrm{Vpcmax}}}\times 16.67\times 0.0316227766016838$ $(\frac{\mathrm{PS}(\mathrm{PCO2\_sc}-\mathrm{PCO2\_isf})}{\mathrm{Visf}}+\frac{\mathrm{V\_CO2}}{\mathrm{alphaCO2}\mathrm{Visf}}\times 1E3)\times 1.66666666666667E-5$ $\mathrm{RQ}\mathrm{V\_O2}$ $\mathrm{DL\_CO2}(\mathrm{PA\_CO2}-\mathrm{PCO2\_pc})\times 22400\times 0.00267857142857143$ $\frac{\mathrm{Pc}+\mathrm{Ppl}-\mathrm{PA}}{\mathrm{Rs}}\times 1000$ $\frac{\mathrm{PD}-\mathrm{Pc}+\mathrm{Ppl}}{\mathrm{Rc}}\times 1000$ $\mathrm{QdotDC}$ $(\mathrm{Pao}-\mathrm{PH2O})\times 0.21$ $(\mathrm{Pao}-\mathrm{PH2O})\times 3E-4$ $\mathrm{Pao}-\mathrm{PH2O}-\mathrm{Pao\_O2}-\mathrm{Pao\_CO2}$ $\begin{cases}\frac{\mathrm{QdotED}\mathrm{Pao\_O2}-\mathrm{QdotDC}\mathrm{PD\_O2}}{\mathrm{VD}}\times 1E-6 & \text{if $\mathrm{dVAdt}> 0$}\\ \frac{\mathrm{QdotED}\mathrm{PD\_O2}-\mathrm{QdotDC}\mathrm{PC\_O2}}{\mathrm{VD}}\times 1E-6 & \text{otherwise}\end{cases}$ $\begin{cases}\frac{\mathrm{QdotDC}\mathrm{PD\_O2}-\mathrm{QdotCA}\mathrm{PC\_O2}-\mathrm{PC\_O2}\mathrm{dVcdt}\times 1000000}{\mathrm{Vc}}\times 1E-6 & \text{if $\mathrm{dVAdt}> 0$}\\ \frac{\mathrm{QdotDC}\mathrm{PC\_O2}-\mathrm{QdotCA}\mathrm{PA\_O2}-\mathrm{PC\_O2}\mathrm{dVcdt}\times 1000000}{\mathrm{Vc}}\times 1E-6 & \text{otherwise}\end{cases}$ $(\mathrm{PD}+\mathrm{Pao}\times 1.3565-\mathrm{PD\_O2}\times 1.3565-\mathrm{PD\_CO2}\times 1.3565)\times 0.737191301142647$ $(\mathrm{Pc}+\mathrm{Ppl}+\mathrm{Pao}\times 1.3565-\mathrm{PC\_O2}\times 1.3565-\mathrm{PC\_CO2}\times 1.3565)\times 0.737191301142647$ $(\mathrm{PA}+\mathrm{Pao}\times 1.3565-\mathrm{PA\_O2}\times 1.3565-\mathrm{PA\_CO2}\times 1.3565)\times 0.737191301142647$ $\mathrm{As}e^{\frac{\mathrm{Ks}(\mathrm{VA}-\mathrm{RV})}{\mathrm{Vstar}-\mathrm{RV}}}+\mathrm{Bs}$ $\mathrm{Kc}\left(\frac{\mathrm{Vcmax}}{\mathrm{Vc}}\right)^2$ $\mathrm{Au}+\mathrm{Ku}\left|\mathrm{dVdt}\right|\times 1000$ $(\frac{\mathrm{Pmus}-\mathrm{Pc}-\mathrm{Pcw}}{\mathrm{Ru}+\mathrm{Rs}}-\frac{\mathrm{Pc}-\mathrm{Pl}-\mathrm{Pve}}{\mathrm{Rs}})\times 0.001$ $\frac{\mathrm{Vcw}-\mathrm{dV}}{\mathrm{tau}}\times 0.001$ $\mathrm{VA}+\mathrm{VD}$ $(\frac{\mathrm{Pc}-\mathrm{Pl}-\mathrm{Pve}}{\mathrm{Rs}}-\frac{\mathrm{Pstp}\mathrm{Tbody}}{(\mathrm{PA}+1030.94)\mathrm{Tstp}}(\mathrm{O2flux}+\mathrm{CO2flux})\times 2.26083333333333E-5)\times 0.001$ $\mathrm{Acw}\times -1+\mathrm{Bcw}\ln (\frac{\mathrm{TLC}-\mathrm{RV}}{\mathrm{Vcw}-\mathrm{RV}}-0.999)$ $\mathrm{Al}e^{\mathrm{Kl}\mathrm{VA}}+\mathrm{Bl}$ $\mathrm{Ppl}+\mathrm{Pl}+\mathrm{Pve}$ $\begin{cases}\mathrm{Ac}-\mathrm{Bc}(\frac{\mathrm{Vc}}{\mathrm{Vcmax}}-0.7)^2 & \text{if $\frac{\mathrm{Vc}}{\mathrm{Vcmax}}< 0.5$}\\ 5.6-\mathrm{Bcp}\ln (\frac{\mathrm{Vcmax}}{\mathrm{Vc}}-0.999) & \text{otherwise}\end{cases}$ $\frac{\mathrm{Vve}}{\mathrm{Cve}}$ $\mathrm{Pcw}-\mathrm{Pmus}$ $\mathrm{Ppl}\times 0.737191301142647$ $\mathrm{Pc}+\mathrm{Ppl}+\mathrm{Rc}(\mathrm{dVcdt}+\frac{\mathrm{Pc}+\mathrm{Ppl}-\mathrm{PA}}{\mathrm{Rs}}\times 0.001)\times 1E3$ $\mathrm{Amus}\sin (6.28318530717959f\mathrm{time\_}\times 1.66666666666667E-5)+\mathrm{Amus}$ $\begin{cases}\frac{\mathrm{QdotED}\mathrm{Pao\_CO2}-\mathrm{QdotDC}\mathrm{PD\_CO2}}{\mathrm{VD}}\times 1E-6 & \text{if $\mathrm{dVAdt}> 0$}\\ \frac{\mathrm{QdotED}\mathrm{PD\_CO2}-\mathrm{QdotDC}\mathrm{PC\_CO2}}{\mathrm{VD}}\times 1E-6 & \text{otherwise}\end{cases}$ $\begin{cases}\frac{\mathrm{QdotDC}\mathrm{PD\_CO2}-\mathrm{QdotCA}\mathrm{PC\_CO2}-\mathrm{PC\_CO2}\mathrm{dVcdt}\times 1000000}{\mathrm{Vc}}\times 1E-6 & \text{if $\mathrm{dVAdt}> 0$}\\ \frac{\mathrm{QdotDC}\mathrm{PC\_CO2}-\mathrm{QdotCA}\mathrm{PA\_CO2}-\mathrm{PC\_CO2}\mathrm{dVcdt}\times 1000000}{\mathrm{Vc}}\times 1E-6 & \text{otherwise}\end{cases}$ $\frac{\mathrm{Vcw}-\mathrm{dV}}{\mathrm{tau}}\times 0.001$ $(\frac{\mathrm{Pmus}-\mathrm{Pc}-\mathrm{Pcw}}{\mathrm{Ru}+\mathrm{Rs}}-\frac{\mathrm{Pc}-\mathrm{Pl}-\mathrm{Pve}}{\mathrm{Rs}})\times 0.001$ $(\frac{\mathrm{Pc}-\mathrm{Pl}-\mathrm{Pve}}{\mathrm{Rs}}-\frac{\mathrm{Pstp}\mathrm{Tbody}}{(\mathrm{PA}+1030.94)\mathrm{Tstp}}(\mathrm{O2flux}+\mathrm{CO2flux})\times 2.26083333333333E-5)\times 0.001$