Louisiana Tech University Ruston, LA 71272 Slide 1 Review Steven A. Jones BIEN 501 Friday, May 14, 2007.

Slides:



Advertisements
Similar presentations
Systems and energy pg. 27 in NB. Objectives Define a physical system. Calculate the mechanical energy of a physical system. Demonstrate and apply the.
Advertisements

Chapter 5 Section 4: Complex Numbers. VOCABULARY Not all quadratics have real- number solutions. For instance, x 2 = -1 has no real-number solutions because.
Louisiana Tech University Ruston, LA Slide 1 Co-Current and Counter-Current Exchange in Dialysis Steven A. Jones BIEN 501 Monday, May 5, 2008.
Louisiana Tech University Ruston, LA Slide 1 Energy Balance Steven A. Jones BIEN 501 Wednesday, April 18, 2008.
Louisiana Tech University Ruston, LA Slide 1 Krogh Cylinder Steven A. Jones BIEN 501 Friday, April 20, 2007.
Louisiana Tech University Ruston, LA Slide 1 Final Exam Topics Steven A. Jones BIEN 501 Monday, May 12, 2008.
Louisiana Tech University Ruston, LA Slide 1 Time Averaging Steven A. Jones BIEN 501 Monday, April 14, 2008.
Ch 3.8: Mechanical & Electrical Vibrations
A streakline is the path that a particle will follow in the flow, the locus of particles that have passed sequentially through a prescribed path in the.
Human Body Drug Simulation Nathan Liles Benjamin Munda.
Chapter 13 MIMs - Mobile Immobile Models. Consider the Following Case You have two connected domains that can exchange mass
Experimental Thermo and Fluid Mechanics Lab. 4. Fluid Kinematics 4.1. Velocity Field 4.2. Continuity Equation.
Fluid Kinematics Fluid Dynamics . Fluid Flow Concepts and Reynolds Transport Theorem ä Descriptions of: ä fluid motion ä fluid flows ä temporal and spatial.
1 MECH 221 FLUID MECHANICS (Fall 06/07) Tutorial 6 FLUID KINETMATICS.
Physics 1901 (Advanced) A/Prof Geraint F. Lewis Rm 557, A29
Monroe L. Weber-Shirk S chool of Civil and Environmental Engineering Fluid Kinematics Fluid Mechanics July 14, 2015 
Monroe L. Weber-Shirk S chool of Civil and Environmental Engineering Fluid Kinematics Fluid Mechanics July 15, 2015 Fluid Mechanics July 15, 2015 
Taking a Square Root to Solve an Equation. Solve: In order to solve for x, you have to UNDO the squared first (i.e. square root) What are the number(s)
Louisiana Tech University Ruston, LA Slide 1 Mass Transport Steven A. Jones BIEN 501 Friday, April 13, 2007.
Laplace transformation
Louisiana Tech University Ruston, LA Slide 1 The Rectangular Channel Steven A. Jones BIEN 501 Friday, April 4th, 2008.
Louisiana Tech University Ruston, LA Slide 1 Krogh Cylinder Steven A. Jones BIEN 501 Wednesday, May 7, 2008.
Chapter 4 Transients.
ECE 8443 – Pattern Recognition EE 3512 – Signals: Continuous and Discrete Objectives: Stability and the s-Plane Stability of an RC Circuit 1 st and 2 nd.
CHAPTER III LAPLACE TRANSFORM
ORDINARY DIFFERENTIAL EQUATION (ODE) LAPLACE TRANSFORM.
ELECTRICA L ENGINEERING Principles and Applications SECOND EDITION ALLAN R. HAMBLEY ©2002 Prentice-Hall, Inc. Chapter 4 Transients Chapter 4 Transients.
Louisiana Tech University Ruston, LA Momentum Balance Steven A. Jones BIEN 501/CMEN 513 Monday, March 19, 2007.
Lecture 2 Differential equations
Louisiana Tech University Ruston, LA Slide 1 Compartmental Models Juan M. Lopez BIEN 501 Friday, May 09, 2008.
Fluid Mechanics and Fluid Dynamics Fluid mechanics is the branch of physics that studies fluids (liquids, gases, and plasmas) and the forces on them. Fluid.
Louisiana Tech University Ruston, LA Slide 1 Mass Transport & Boundary Layers Steven A. Jones BIEN 501 Friday, May 2, 2008.
Sturm-Liouville Cylinder
Mathematical Models and Block Diagrams of Systems Regulation And Control Engineering.
Using square roots to solve quadratic equations. 2x² = 8 22 x² = 4 The opposite of squaring a number is taking its square root √ 4= ± 2.
Imaginary Numbers ???. In real life, complex numbers are used by engineers and physicists to measure electrical currents, to analyze stresses in structures.
PHARMACOKINETIC MODELS
Chapter 4 Transients. 1.Solve first-order RC or RL circuits. 2. Understand the concepts of transient response and steady-state response.
Wednesday, Nov. 19, 2003PHYS , Fall 2003 Dr. Jaehoon Yu 1 PHYS 1443 – Section 003 Lecture #21 Wednesday, Nov. 19, 2003 Dr. Mystery Lecturer 1.Fluid.
METR February Review Hydrostatic balance Pressure decreases exponentially with height, isothermal atmosphere: Zeroth law of thermodynamics:
Systems and energy. Equations For any closed system that undergoes a change, the total energy before the change is the same as the total energy after.
Vectors n v What is the projection of the vector (1, 3, 2) onto the plane described by ? Louisiana Tech University Ruston, LA
Chapter 4 Fluid Kinematics CE Fluid Mechanics Diogo Bolster.
Imaginary Numbers Historyand Practical Applications Practical Applications.
Conservation of Energy. Equations For any closed system that undergoes a change, the total energy before the change is the same as the total energy after.
Louisiana Tech University Ruston, LA Boundary Layer Theory Steven A. Jones BIEN 501 Friday, April
Chapter 5.9 Complex Numbers. Objectives To simplify square roots containing negative radicands. To solve quadratic equations that have pure imaginary.
Chapter 14 Systems of Particles.
Differential Analysis of Fluid Flow. Navier-Stokes equations Example: incompressible Navier-Stokes equations.
The Laplace Transform.
Louisiana Tech University Ruston, LA Flows With More Than One Dependent Variable - 2D Example Juan M. Lopez Steven A. Jones BIEN 501 Wednesday, April.
Chapter 4.6 Complex Numbers. Imaginary Numbers The expression does not have a real solution because squaring a number cannot result in a negative answer.
1 ECE 3301 General Electrical Engineering Section 30 Natural Response of a Parallel RLC Circuit.
Course : Civil Engineering Division : C (3 rd Semester). Subject : Fluid Mechanics Subject Code : Guided By :HIREN JARIWALA(H.O.D) :DIXIT CHAUHAN(ASSI.PROF.)
3.4 Chapter 3 Quadratic Equations. x 2 = 49 Solve the following Quadratic equations: 2x 2 – 8 = 40.
Mathematical Models of Control Systems
Physiology for Engineers
Chapter 4 Fluid Mechanics Frank White
CHAPTER III LAPLACE TRANSFORM
CHAPTER 4: Systems of Particles
Complex integers? Here a and b are integers.
Dosimetry and Kinetics
Peristaltic Pumping Steven A. Jones BIEN 501 Friday, April 18, 2008
Fluid Kinematics Fluid Dynamics.
Systems of Linear and Quadratic Equations
Relaxation Technique CFD
Unsteady Diffusion into a Sphere
Mathematical Models of Control Systems
Find the set of points (x, y) such that F(x, y) = 0 if F(x, y) = (r - 4)x, {image} , and r = |x|
Stream Function & Velocity Potential
Presentation transcript:

Louisiana Tech University Ruston, LA Slide 1 Review Steven A. Jones BIEN 501 Friday, May 14, 2007

Louisiana Tech University Ruston, LA Slide 2 Simple Flow Field What is the pathline?

Louisiana Tech University Ruston, LA Slide 3 Simple Flow Field

Louisiana Tech University Ruston, LA Slide 4 Simple Flow Field Pathline follows the particle

Louisiana Tech University Ruston, LA Slide 5 Simple Flow Field What is the streakline?

Louisiana Tech University Ruston, LA Slide 6 What is the Differential Equation that Describes a Streamline? Assume we know that: Answer: Since So

Louisiana Tech University Ruston, LA Slide 7 Continuity For a two-dimensional flow: Use the equation of continuity to determine v.

Louisiana Tech University Ruston, LA Slide 8 Answer

Louisiana Tech University Ruston, LA Slide 9 What is the equation for a pathline? A pathline follows a fluid particle. Assume that you know the entire velocity field: and that the particle passes through the point at time 0. Answer:

Louisiana Tech University Ruston, LA Slide 10 Example Assume that: Answer: Is continuity satisfied?

Louisiana Tech University Ruston, LA Slide 11 What is the equation for a pathline? Answer: Assume that: What is the equation for the pathline through (1,2)?

Louisiana Tech University Ruston, LA Slide 12 What is the equation for a pathline? Write:

Louisiana Tech University Ruston, LA Slide 13 What is the equation for a pathline? so

Louisiana Tech University Ruston, LA Slide 14 Answer (Continued)

Louisiana Tech University Ruston, LA Slide 15 Two Compartment Model Conservation of Mass C1C1 C2C2 Clearance Central Compartment Peripheral Compartment

Louisiana Tech University Ruston, LA Slide 16 Two Compartment Model Conservation of Mass In terms of the volume ratio Initial Conditions Solve the two ODEs for C 1

Louisiana Tech University Ruston, LA Slide 17 ICs in terms of C 1

Louisiana Tech University Ruston, LA Slide 18 Solution The solution to: With Is Where:

Louisiana Tech University Ruston, LA Slide 19 Two Compartment Model Rapid Release Slow Release One Compartment

Louisiana Tech University Ruston, LA Slide 20 Two Compartment Model The two-compartment model obeys the same differential equations as the simple RLC circuit. It is useful to compare the individual components to the RLC circuit: Damping Transfer from L to C

Louisiana Tech University Ruston, LA Slide 21 Two Compartment Model One might expect that overshoot (ringing) could happen. However, ringing will only happen for imaginary values of. In our case: And for the RLC Circuit: Can make the square root imaginary with small R or large C. As you increase k 2 or k e, you must also increase (k 1 +k 2 +k 3 ).

Louisiana Tech University Ruston, LA Slide 22 Two Compartment Model To see if the square root can become imaginary, minimize it’s argument w.r.t. k e and see if it can be less than 0.

Louisiana Tech University Ruston, LA Slide 23 Two Compartment Model What value does the argument of the square root take on at the minimum? Since k 2 and k 1 cannot be negative, the argument of the square root can never be negative. I.e. no ringing.

Louisiana Tech University Ruston, LA Slide 24 Pharmacokinetic Models Vascular Interstitial Cellular PBPK: Physiologically-Based Pharmocokinetic Model Q : Plasma Flow L : Lymph Flow J s, q: Exchange rates

Louisiana Tech University Ruston, LA Slide 25 Pharmacokinetic Models Z : Equilibrium concentration ratio between interstitium and lymph.

Louisiana Tech University Ruston, LA Slide 26 More Complicated Models Plasma Liver Kidney Muscle G.I. Track

Louisiana Tech University Ruston, LA Slide 27 Note on Complexity While the equations become more complicated as more components are added, the basic concepts remain the same, and the systems can be analyzed with the same tools you would use to analyze a linear system in electrical engineering (e.g. transfer functions, Laplace transforms, Mason’s rule).

Louisiana Tech University Ruston, LA Slide 28

Louisiana Tech University Ruston, LA Slide 29 What is the Differential Equation that Describes a Streamline?