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ChE 3723 F2020 Lecture 37 HW 14 Discussion 12/3/2020In this final lecture of the semester we look at the solution of HW 14 to illustrate the use of the method of lines for solving PDEs. There is also a comparison to the explicit method, the implicit…
From Jeffrey Harwell
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ChE/CEES 5673 Colloid Science Lecture 24 Surfactant TypesIn this last session of the semester we'll take a quick overview of the principle surfactant types found in commercial and industrial applications of surfactants, today. This session goes with…
From Jeffrey Harwell
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ChE 3723 F2020 Lecture 36 Other Methods for Parabolic PDEsWe previously looked at using the Method of Lines to integrate the system of ordinary differential equations we obtain when we discretize a PDE in the spatial dimension. This enables us to use our RK…
From Jeffrey Harwell
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ChE/CEES 5673 Lecture 23 Cleaning System Technology 11/30/2020In today's lecture we look at the scientific basis for the $100 B detergent industry and the closely associated industrial and institutional cleaning industries. These industries are large…
From Jeffrey Harwell
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ChE 3723 F2020 Lecture 34 Solving a Parabolic PDE in Excel with VBA 11/23/2020Here we introduce the method of lines as a straight-forward extension of the Runge-Kutta methods developed in chapters 8 and 9 to the solution of partial differential equations. We also discuss the…
From Jeffrey Harwell
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ChE/CEES Colloid Science Lecture 22 FoamsIn this session we discuss the mechanisms of foam formation and foam stability, which we explain in terms of film elasticity and film drainage. We look at the Gibbs/Marangoni effect and Plateau…
From Jeffrey Harwell
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ChE 3723 F2020 Lecture 32 Using dimensionless variables with a PDEWe continue our discussion of PDE solution methods with a discussion of the value of using dimensionless variables, and the pluses and minuses of this transformation of the PDE.
From Jeffrey Harwell
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ChE 3723 F2020 11/20/2020 Lecture 33 PDEs and Finite DifferencesIllustrates the use of numerical derivatives to represent the solution to a partial differential equation using discrete points on a multidimensional grid.
From Jeffrey Harwell
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ChE/CEES Colloid Science Lecture 21 Dispersions Part 3A continuation of our discussion of dispersions including a look at points of zero charge and how knowledge of the point of zero charge effects selection of a surfactant to use as a dispersant.
From Jeffrey Harwell
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ChE/CEES Colloid Science Lecture 20 Dispersions Part 2Here we continue our discussion of dispersions, specifically, solids dispersed in liquids. We distinguish between colloidal or Brownian dispersions, where particles stay suspended by Brownian motion,…
From Jeffrey Harwell
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ChE 3723 F2020 Lecture 28 HW 13 and BVPs 10/19/2020In this session we look at my solutions to HW 13 and review the types of BVPs that might occur on your 3rd exam and final exam.
From Jeffrey Harwell
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ChE/CEES Colloid Science Lecture 19 Demulsification Theory and Dispersion Stability Part 1This session begins with wrapping up our discussion of emulsions by looking at the problem of emulsion breaking, then begins the discussion of dispersion stability.
From Jeffrey Harwell
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ChE 3723 F2020 Lecture 29 HW 12 Review and More Boundary Value Problems 11/11/2020In this class session we go over the solutions to HW 12 and then look at the solution to the ODE in HW 12 after converting it into a BVP. The point to be made, here, is that the same Runge-Kutta…
From Jeffrey Harwell
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ChE/CEES Colloid Science Lecture 18 Emulsions Part 3We continue our discussion of emulsions and microemulsions with a look at the HLB model and introduce HLD theory.
From Jeffrey Harwell
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ChE 3723 F2020 Lecture 26 Solving Boundary Value ProblemsHere we look at using the same Runge-Kutta code we developed for solving 2nd order initial value problems (IVP) to solve a boundary value problem (BVP). The process is basically identical, but for…
From Jeffrey Harwell
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