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:
- Increased total peripheral resistance to flow (principally vessel radius and blood viscosity)
- Decreased aortic and peripheral compliance (which results in increased hydraulic reactance)
- Aortic stenosis and LVOT outlet obstruction
- Increased chamber size
Afterload is decreased by:
- Increasing wall thickness