$$CO = \frac{MAP - CVP}{TPR} = SV \cdot HR$$
Stroke volume is affected by preload (sarcomere length at end-diastole) and afterload (the valvular-arterial impedance); the residual effects on stroke volume after controlling for those two factors is termed inotropy.
Inotropy describes the stroke volume with a given preload and afterload.
Three indicies are used to approximate the inotropy.
\(\uparrow[Ca^{2+}]_{intracellular} \to \ \uparrow \text{Toponin-}Ca^{2+} \text{ binding} \to \ \uparrow \text{Active myosin units} \)
(This is how in-vivo way inotropy is modulated and how all intotropes except levosimendan work).
Intracellular calcium is modulated by extracellular calcium concerntration, and calcium conductance during phase 2 of the myocardial action potential.
\(\beta_1\) agonism increases adenylate cyclase \(\to\) increases cAMP \(\to\) increases PKA. PKA then phosphorylates two important targets: the L-type calcium channel of the sarcolemma and the SERCA transporter of the sarcoplasmic reticulum. The first increases calcium conductance into the cell during phase 2, and the second increases calcium export rate during phases 3 and 4.
Things that increase inotropy
Things that decrease intotropy
Preload is the sarcomere length at end-diastole, which is approximated by left ventricular end diastolic volume.
From the definition of compliance, we have immediately
$$LVEDV = C_{\text{LV wall}} \cdot LVEDP$$
Determinants of LVEDP
Determinants of LV compliance
Frank-starling mechanism
The Frank-starling mechanism causes increased stroke volume as sarcomeres length increases. This is probably because
The relationship is concave-down (it plateaus out). With reduced contractility, the curve can begin to decrease beyond a maximum stroke volume.
This matches the LV output to the RV output and adapts to sudden changes in preload.
The afterload of the heart is the hydraulic input impedance of the aortic valve and vascular tree. If we think of this in Pouseillean terms:
$$Q = \frac{\Delta P}{I}$$
$$I = \frac{\Delta P}{Q}$$
$$I = \frac{LVSP}{Q}$$
$$I = \frac{\text{Aortic Systolic Pressure} + \text{Mean LVOT gradient}}{\text{Stroke volume}}$$
And like everything else in cardiology, we should normalize it to body surface area...
$$\text{Valvuloarterial Impedance} = \frac{\text{Aortic Systolic Pressure} + \text{Mean LVOT gradient}}{\text{Stroke volume index}}$$
Basically, if the afterload is high, we need a higher LV systolic pressure to force out the same amount of fluid.
Alternatively, we can think of afterload as the wall tension in the ventricle: the radial force exerted by a unit volume of myocardial tissue given by the Young-Laplace equation for a spherical shell:
$$\rho = \frac{P \cdot r}{2w}$$
$$\rho = \frac{\text{LVSP} \cdot \text{LV radius}}{2 \cdot {\text{LV wall thickness}}}$$
Therefore the things that increase afterload are:
Afterload is decreased by:
The Venous return is the flow of blood from the venous to the heart. It equals cardiac output.
$$VR = CO$$
$$VR = \frac{MSFP - CVP}{\text{Systemic Venous Resistance}}$$
The mean systemic filling pressure (the pressure in the capillaries, or equivalently the pressure throughout the circulation during cardiac arrest). This is determined by:
The Guyton model involves two functions. The independent variable is the CVP. Then we consider the cardiac output and venous return as functions of the CVP.
The cardiac output CO(CVP): This has the usual Frank-Starling shape.
The venous return: this is constant (and maximal) below a CVP of 0cmH2O due to venous collapse, then falls with increasing CVP, because \(VR = \frac{MSFP - CVP}{\text{Systemic Venous Resistance}}\)
Of course, \(CO = \text{Venous return}\) - so the point where these two curves cross is the steady state operating point.
Three things can therefore affect the cardiac output in this model.