Integrating 3 equations together

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SUMMARY

The discussion focuses on integrating the Continuity equation, Bernoulli's equation, and Poiseuille's equation to analyze blood flow dynamics in narrowed blood vessels and branching arteries. The Continuity equation (A1v1 = A2v2) demonstrates how blood velocity changes with vessel radius, while Bernoulli's equation (P + 1/2 * ρ * V^2 + ρgh = constant) relates pressure and velocity. The application of Poiseuille's equation is essential for accurately predicting pressure differences in scenarios involving viscous flow, particularly in small arterioles where the effects of viscosity become significant. This integration provides a comprehensive understanding of blood flow variations as vessels narrow and branch.

PREREQUISITES
  • Understanding of the Continuity equation in fluid dynamics
  • Familiarity with Bernoulli's equation and its applications
  • Knowledge of Poiseuille's equation for viscous flow
  • Basic principles of fluid mechanics and blood flow dynamics
NEXT STEPS
  • Study the implications of Poiseuille's equation in real-world vascular scenarios
  • Explore advanced applications of Bernoulli's equation in fluid systems
  • Investigate the effects of viscosity on blood flow in narrow vessels
  • Learn about computational fluid dynamics (CFD) simulations for vascular flow analysis
USEFUL FOR

Medical professionals, biomedical engineers, and researchers in cardiovascular physiology will benefit from this discussion, particularly those interested in understanding blood flow mechanics in relation to vascular health and disease.

ch5112
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There are 3 equations

1/ Continuity equation

Av=constant

2/ Bernoulli's equations

P+1/2*p*V^2+pgy=constant

3/ Poiseiulle's equation


Question1:

If a single blood vessle is narrowed by the build-up of plaque so that its inner radius is reduced. How can I use above three equations to apply in this situation to provide insight into the varation of speed and pressure as the blood vessel become narrower.

Question 2:
A single small artery branches into about six smaller blood vessels, which in turn branch a fewmore times into a total of about 1000 arterioles. The radius of the initial, single small artery is 0.7 mm, and the average radius of each of the 1000 arterioles is 70 μm. Explain how the three equations above could be applied in this situation to provide insight into the variation of speed and pressure as blood travels from the single artery to 1000 arterioles. In particular, why does the Continuity equation together with only Bernoulli’s equation not provide an adequate explanation? What would be wrong with such a prediction, and what is it about this system that means Poiseiulle’s equation is crucial to a fuller explanation.
 
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Let's call the radius of the normal blood vessel r1 and the reduced radius r2. Assume that the blood is of constant viscosity. The continuity equation is (as you stated):

A1v1 = A2v2
A is the area of the cross-section
v is the velocity across that cross-section

The area of a circle is πr2. Substitute that in. The equation becomes:

πr12v1 = πr22v2

v2 = (r12/r22) v1

v22 = (r12/r22)2 v12

Now we need to replace v1 with something more descriptive. Use Bernoulli's equation:

P1+ρv12/2+ρgh1=P2+ρv22/2+ρgh2

ρv12/2=P2-P1+ρgh2-ρgh1+ρv22/2

v12=2(P2-P1)/ρ+2(gh2-gh1)+v22

Subbing into the above:

v22 = (r12/r22)2 * [2(P2-P1)/ρ+2(gh2-gh1)+v22]

Isolate v2.

By now you probably get the point. You can use Poiseiulle's equation for even better (more descriptive) substitutions. Substitute it in for the quantity P2-P1.
 

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