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1D Finite Different Method Conduction Heat Transfer Tool
01 Sep 2011 | | Contributor(s):: Nicholas Roberts
Simple 1D Finite Difference Method Tool for Undergraduate Heat Transfer Course
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2010 Nano-Biophotonics Summer School @ UIUC Lecture 2 - 2D/3D Fourier transforms & Electromagnetic fields/ Lorentz-Drude model
20 Sep 2010 | | Contributor(s):: Gabriel Popescu
So far, we have discussed Fourier transformations involving one-dimensional functions. Of course, in studying imaging, the conceptmust be generalized to 2D and 3D functions. For example, diffraction and 2D image formation are treated efficiently via 2D Fouriertransforms, while light scattering...
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2010 Nano-Biophotonics Summer School @ UIUC Lecture 4 - Gaussian beam propagation - Elastic light scattering - Dynamic light scattering
20 Sep 2010 | | Contributor(s):: Gabriel Popescu
Often, experiments involve light beams. A light beam can be defined as a distribution of field that fulfills the approximation in Eq. 20,i.e. is characterized by a dominant wave vector component, k(z) >> k(x) , k(y) . A beam is, therefore, the spatial equivalent of quasimonochromaticlight,...
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The boundary conditions do not seem to be set using the interface for the tool.
Q&A|Closed | Responses: 1
When I look at the program output, I noticed that the 6x3 matrix (BDY) values do not seem to be getting set using the interface. The model...
https://nanohub.org/answers/question/1684
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ECE 606 L19.2: PN Junction - Drawing Band-Diagrams in Equilibrium
28 Apr 2023 | | Contributor(s):: Gerhard Klimeck
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ECE 606 L20.2: PN Diode - Derivation of the Forward Bias Formula
28 Apr 2023 | | Contributor(s):: Gerhard Klimeck
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ECE 606 L22.2: PN Diode - Turn-Off and Turn-On Characteristics
28 Apr 2023 | | Contributor(s):: Gerhard Klimeck
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ECE 606 L27.2: Heterojunction Bipolar Transistor - Heterojunction Equilibrium Solution
28 Apr 2023 | | Contributor(s):: Gerhard Klimeck
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Nanoelectronic Modeling Lecture 23: NEMO1D - Importance of New Boundary Conditions
02 Mar 2010 | | Contributor(s):: Gerhard Klimeck
One of the key insights gained during the NEMO1D project was the development of new boundary conditions that enabled the modeling of realistically extended Resonant Tunneling Diodes (RTDs). The new boundary conditions are based on the partitioning of the device into emitter and collector...
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Theory of Heat Conduction with Type 5 Boundary Condition
19 Feb 2014 | | Contributor(s):: Donald E. Amos
In the classical theory, the general solution of the heat conduction problem is expressed in terms of the Green's function. Terms which take into account volumetric heat generation, an initial temperature distribution and boundary conditions can be identified. In the current literature (...