class: center, middle, inverse, title-slide .title[ # Lecture 21 ] .subtitle[ ## There Will Be Blood ] .author[ ### Dr. Christopher Kenaley ] .institute[ ### Boston College ] .date[ ### 2023/04/04 ] --- class: top # There will be blood <!-- Add icon library --> <link rel="stylesheet" href="https://cdnjs.cloudflare.com/ajax/libs/font-awesome/5.14.0/css/all.min.css"> .pull-left[ Today we'll introduce - Hagen-Poiseuille law - Violation of H-P (how it really works) - Laundry list of other important laws/models ] .pull-right[ <iframe width="400" height="200" src="https://www.youtube.com/embed/pwmlP1hLJf0" title="YouTube video player" frameborder="0" allow="accelerometer; autoplay; clipboard-write; encrypted-media; gyroscope; picture-in-picture" allowfullscreen></iframe> ] --- class: top # Flow in tubes (inside you!) Cardiovascular system and elsewhere, too? Where? .center[ <img src="https://www.cvphysiology.com/uploads/images/h006-laminar-flow.png" width="600" /> ] --- class: top # Flow in tubes (inside you!) .center[ <img src="img/tubeflow.png" width="600" /> `$$\Delta p={\frac{8\mu LQ}{\pi R^{4}}}={\frac{8\pi \mu LQ}{A^{2}}}$$` ] - The tube is stiff, straight, and uniform - Blood is Newtonian , i.e., viscosity is constant - The flow is uniform, laminar and steady, not pulsatile, and the velocity at the wall is zero (no slip at the wall) --- class: top # Flow in tubes (inside you!) .center[ <img src="img/tubeflow.png" width="600" /> `$$Q=\frac{R^4\Delta P}{8\mu L}$$` Hagen-Poiseuille law Valid until the flow is turbulent! (Re > ~ 2000) ] --- class: top # Flow in tubes (inside you!) .center[ <img src="https://www.mayoclinic.org/-/media/kcms/gbs/patient-consumer/images/2013/11/15/17/35/ds00525_-ds01120_-ds00064_-ds00178_-ds01052_-ds00537_-ds01179_im00642_ww5r236t_jpg.jpg " width="300" /> `$$Q=\frac{R^4\Delta P}{8\mu L}$$` Hagen-Poiseuille law Effects of ateriosclerosis? ] --- class: top # Flow in tubes (inside you!) .center[ <img src="https://i1.wp.com/www.differencebetween.com/wp-content/uploads/2017/07/Difference-Between-Vasoconstriction-and-Vasodilation-3.png?w=800&ssl=1 " width="400" /> `$$Q=\frac{R^4\Delta P}{8\mu L}$$` Hagen-Poiseuille law Non-linear effects of vasodialation and vasoconstriction? ] --- class: top # Flow in tubes (inside you!) .pull-left[ Flow profile is altered by branches: - Flow entering a side branch results in skewed profile. - It takes a certain inlet length before the velocity develops into a parabolic profile again..... ] .pull-right[ <img src="img/branch.png" width="400" /> `\(\frac{l_{inlet}}{D}\approx 0.6Re\)` `\(l_{inlet}\approx 0.6ReD\)` ] --- class: top # Flow in tubes (inside you!) .pull-left[ Flow profile is altered by branches (non-uniform): - Aorta mean blood flow is about 6 l/min - D=3 cm - Mean velocity is ~ 15 cm/s - Re~1350 ] .pull-right[ <img src="img/aorta.jpg" width="400" /> `\(\frac{l_{inlet}}{D}\approx 0.6Re\)` `\(l_{inlet}\approx 0.6ReD\)` ] --- class: top # Flow in tubes (inside you!) Flow is pulsatile, but not everywhere. .center[ <img src="https://www.researchgate.net/publication/343487724/figure/fig2/AS:921709901271042@1596764173575/Windkessel-model-a-schematic-diagram-of-the-windkessel-effect-redrawn-based-on.ppm" width="400" /> ] --- class: top # Poiseuille, Bernoulli, Leplace, etc. in design .pull-left[ - Number of capillaries (Fick's Law for diffusion) - Diameter of capillaries (Peclet number for balancing diffusion and convection) - Relative diameter of other vessels (Murray's law for minimizing circulatory work) - Relative thickness of vessel walls (Leplace's law for how size sets pressure versus wall tension) - Relative size of capillaries and alveoli (Diffusion coefficients of O2 in air and water.) - Concentration of RBCs (cell density vs. viscosity and Poiseuille pressure drop) ] .pull-right[ <img src="img/circsystem.jpg" width="400" /> ] --- class: center, middle # Thanks! Slides created via the R package [**xaringan**](https://github.com/yihui/xaringan).