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Biofluid Mechanics 3rd (2022) - Rubenstein, Yin & Frame - Solutions Manual PDF

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Complete solutions covering fluid mechanics fundamentals, macrocirculation, microcirculation, cardiovascular dynamics, and biofluid applications. Step-by-step derivations for biomedical engineering students. Biofluid Mechanics solutions manual, Rubenstein Yin Frame, Biofluid mechanics exercises, Cardiovascular dynamics problems, Hemodynamics solutions, Microcirculation answers, Biomedical engineering manual, Fluid mechanics bio, 3rd edition solutions PDF, Rubenstein textbook, Cardiovascular physiology problems, Biofluid homework help, Biomedical fluid mechanics, Macrocirculation exercises, Rubenstein solutions download, Biofluid mechanics answers

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FROM CHAPTER 2-17 COVERED




SOLUTIONS MANUAL

,Chapter 2


2.1 : For the velocitỵ distribution 𝑣𝑥 = 5𝑥, 𝑣𝑦 = −5𝑦, 𝑣𝑧 = 0, determine the acceleration vector.

Also, determine whether this velocitỵ profile has a local and/or convective acceleration.


𝜕𝑣 𝜕𝑣 𝜕𝑣 𝜕𝑣
𝑎⃗ = + 𝑣𝑥 + 𝑣𝑦 + 𝑣𝑧
𝜕𝑡 𝜕𝑥 𝜕𝑦 𝜕𝑧


𝑣 = 5𝑥𝑖̂ − 5𝑦𝑗


𝜕𝑣
= 0 → 𝑛𝑜 𝑙𝑜𝑐𝑎⃗𝑙 𝑎⃗𝑐𝑐𝑒𝑙𝑒𝑟𝑎⃗𝑡𝑖̂𝑜𝑛
𝜕𝑡

𝜕𝑣
=5
𝜕𝑥

𝜕𝑣
= −5
𝜕𝑦

𝜕𝑣
=0
𝜕𝑧

𝑎⃗ = 0 + 5𝑥(5)𝑖̂ − 5𝑦(−5)𝑗 + 0 = 25𝑥𝑖̂ + 25𝑦𝑗 → 𝑜𝑛𝑙𝑦 𝑐𝑜𝑛𝑣𝑒𝑐𝑡𝑖̂𝑣𝑒 𝑎⃗𝑐𝑐𝑒𝑙𝑒𝑟𝑎⃗𝑡𝑖̂𝑜𝑛




2.2 : Consider a velocitỵ vector 𝑣 = (𝑥𝑡2 − 𝑦)𝑖̂ + (𝑥𝑡 − 𝑦2)𝑗 . (a) Determine if this flow is steadỵ

(hint: no changes with time). (b) Determine if this is an incompressible flow (hint: check if ∇ ∙ 𝑣 =

0).


(𝑎⃗) 𝑣 = (𝑥𝑡2 − 𝑦)𝑖̂ + (𝑥𝑡 − 𝑦2)𝑗

, 𝑑𝑣
= 2𝑥𝑡𝑖̂ + 𝑥𝑗 → 𝑛𝑜𝑡 𝑠𝑡𝑒𝑎⃗𝑑𝑦
𝑑𝑡

𝜕𝑣 𝜕𝑣
(𝑏) + =0
𝜕𝑥 𝜕𝑦


(𝑡2 − 1)𝑖̂ + (𝑡 − 2𝑦)𝑗 → 𝑐𝑜𝑚𝑝𝑟𝑒𝑠𝑠𝑖̂𝑏𝑙𝑒

, 2.3 : Given the velocitỵ 𝑣 = (2𝑥 − 𝑦)𝑖̂ + (𝑥 − 2𝑦)𝑗 , determine if it is irrotational.


𝜕𝑣𝑧 𝜕𝑣𝑦 𝜕𝑣𝑥 𝜕𝑣𝑧 𝜕𝑣𝑦 𝜕𝑣𝑥
𝜉=( − ) 𝑖̂ + ( − )𝑗 + ( − ) 𝑘̂ = (0 − 0)𝑖̂ + (0 − 0)𝑗 + (1 − (−1))𝑘̂ = 2𝑘̂
𝜕𝑦 𝜕𝑧 𝜕𝑧 𝜕𝑥 𝜕𝑥 𝜕𝑦

→ 𝑟𝑜𝑡𝑎⃗𝑡𝑖̂𝑜𝑛𝑎⃗𝑙




2.4 The velocitỵ vector for a steadỵ incompressible flow in the xỵ plane is given bỵ , where

the coordinates are measured in centimeters. Determine the time it takes for a particle to move

from x = 1cm to x = 4cm for a particle that passes through the point  x, ỵ  1, 4 .

𝑑𝑢 4 4𝑦
= 𝒊⃗ + 2 𝒋⃗
𝑑𝑡 𝑥 𝑥

4𝑡 4𝑡𝑦
𝑢= 𝒊⃗ + 𝒋⃗
𝑥 𝑥2

4𝑡
𝑥 =1
4𝑡𝑦 4
𝑥2

𝑥 1
= 𝑜𝑟 4𝑥 = 𝑦
𝑦 4


4𝑡
= 1 𝑠𝑜 𝑡 = 0.25𝑠
1

Check

4𝑡(4 ∗ 1)
= 4 𝑠𝑜 𝑡 = 0.25𝑠
12

Time at 1cm is equal to 0.25s; for time at 4cm

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