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Rensselaer Polytechnic Institute Documents (16,630)

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  • 15 pages MT-11-Ch05-1.ppt
    • MT-11-Ch05-1.ppt
    • Rensselaer Polytechnic Institute
    • Microelectronics Technology
    • ECSE 2210 - Fall 2014
    • Chapter 5-1. PN-junction electrostatics In this chapter you will learn about pn junction electrostatics: Charge density, electric field and electrostatic potential existing inside the diode under equilibrium and steady state conditions. You will also lear
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    MT-11-Ch05-1.ppt

  • 10 pages MT-12-Ch05-2.ppt
    • MT-12-Ch05-2.ppt
    • Rensselaer Polytechnic Institute
    • Microelectronics Technology
    • ECSE 2210 - Fall 2014
    • Chapter 5-2 Quantitative electrostatic relationships We make the analysis in 1 dimension, even though actual diode as shown may not be a one-dimensional system. This makes the analysis simple. The metallurgical junction is located at x = 0. Quantitative a
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    MT-12-Ch05-2.ppt

  • 9 pages MT-10-Ch03-5.ppt
    • MT-10-Ch03-5.ppt
    • Rensselaer Polytechnic Institute
    • Microelectronics Technology
    • ECSE 2210 - Fall 2014
    • Chapter 3-5. Continuity equation The continuity equation satisfies the condition that particles should be conserved! Electrons and holes cannot mysteriously appear or disappear at a given point, but must be transported to or created at the given point via
    • Register Now

    MT-10-Ch03-5.ppt

  • 13 pages MT-09-Ch03-4.ppt
    • MT-09-Ch03-4.ppt
    • Rensselaer Polytechnic Institute
    • Microelectronics Technology
    • ECSE 2210 - Fall 2014
    • Chapter 3-4. R-G statistics R-G statistics is the mathematical characterization of R-G processes An important generation process in device operation is photogeneration If the photon energy (h) is greater than the band gap energy, then the light will be
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    MT-09-Ch03-4.ppt

  • 18 pages MT-02-Ch02-1.ppt
    • MT-02-Ch02-1.ppt
    • Rensselaer Polytechnic Institute
    • Microelectronics Technology
    • ECSE 2210 - Fall 2014
    • Chapter 2-1. Semiconductor models The subatomic particles responsible for charge transport in metallic wires electrons The subatomic particles responsible for charge transport in semiconductors electrons & holes In this chapter, we will study these topics
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    MT-02-Ch02-1.ppt

  • 19 pages MT-06-Ch03-1.ppt
    • MT-06-Ch03-1.ppt
    • Rensselaer Polytechnic Institute
    • Microelectronics Technology
    • ECSE 2210 - Fall 2014
    • Chapter 3-1. Carrier action Topics to be covered in this chapter: Response of carriers (holes and electrons) under perturbed conditions: Drift Diffusion Recombination-generation Equations of state Thermodynamic equilibrium vs. steady state Thermodynam
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    MT-06-Ch03-1.ppt

  • 15 pages MT-05-Ch02-4.ppt
    • MT-05-Ch02-4.ppt
    • Rensselaer Polytechnic Institute
    • Microelectronics Technology
    • ECSE 2210 - Fall 2014
    • Chapter 2-4. Equilibrium carrier concentrations Equilibrium electron concentration is given by: E top n0 gC ( E ) f ( E ) dE EC Equilibrium hole concentration is given by: EV p0 g V ( E ) 1 f ( E ) dE E Bottom This integral cannot be solved in closed f
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    MT-05-Ch02-4.ppt

  • 11 pages MT-07-Ch03-2.ppt
    • MT-07-Ch03-2.ppt
    • Rensselaer Polytechnic Institute
    • Microelectronics Technology
    • ECSE 2210 - Fall 2014
    • Chapter 3-2. Diffusion and band bending We will learn two new topics in this lecture: Diffusion a process whereby particles tend to spread out or redistribute as a result of their random thermal motion, migrating on a macroscopic scale from regions of hig
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    MT-07-Ch03-2.ppt

  • 13 pages MT-01-Ch01-1.ppt
    • MT-01-Ch01-1.ppt
    • Rensselaer Polytechnic Institute
    • Microelectronics Technology
    • ECSE 2210 - Fall 2014
    • Semiconductors: A general introduction Classification of Materials in terms of electrical resistivity: Insulators Semiconductors Conductors 1010 1018 cm 104 108 cm 106 104 cm The uniqueness of semiconductors is that their conductivity can be varied by us
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    MT-01-Ch01-1.ppt

  • 15 pages MT-08-Ch03-3.ppt
    • MT-08-Ch03-3.ppt
    • Rensselaer Polytechnic Institute
    • Microelectronics Technology
    • ECSE 2210 - Fall 2014
    • Chapter 3-3. Relating diffusion coefficients and mobilities In this class, we will learn about: Constancy of Fermi-level Indicates equilibrium conditions Current flow under thermal equilibrium Net hole current (diffusion + drift) should be zero Net electr
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    MT-08-Ch03-3.ppt

  • 2 pages Paul Scalia tensile testing.docx
    • Paul Scalia tensile testing.docx
    • Rensselaer Polytechnic Institute
    • Materials Science for Engineers
    • MTLE 1600 - Spring 2008
    • Paul Scalia Materials Science Tensile Test Post Lab Charts: Aluminum Chart Title 6000 5000 4000 3000 2000 1000 0 -1000 stress Strain Extensometer Chart Title 8000 7000 6000 5000 4000 3000 2000 1000 0 -1000 Stress Strain Polymer Chart Title 6000 5000 4000
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    Paul Scalia tensile testing.docx

  • 1 pages Paul Scalia tg lab 2.docx
    • Paul Scalia tg lab 2.docx
    • Rensselaer Polytechnic Institute
    • Materials Science for Engineers
    • MTLE 1600 - Spring 2008
    • Paul Scalia Materials Science Undeclared Engineering RPI 2020 Lab 3 Post Lab Bounce height/intial bounce height over time 7 6 5 4 H/H0 3 2 1 0 time (sec) 1) The minimum is at t = 900 seconds. 2) Our determined Tg: -130 degrees C. Class Average Tg: -142 de
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    Paul Scalia tg lab 2.docx

  • 2 pages lab 6 diffusion.xlsx
    • lab 6 diffusion.xlsx
    • Rensselaer Polytechnic Institute
    • Materials Science for Engineers
    • MTLE 1600 - Spring 2008
    • Time (min)D P.P. D M.B. 1 8.54 7.12 2 9.67 7.59 3 11.58 8.17 4 11.55 8.41 5 11.61 8.49 6 12.95 8.71 7 13.26 8.78 8 14.39 9.09 9 14.87 9.6 10 15.2 9.46 11 15.79 9.84 12 16.03 10.14 13 16.36 10.47 14 16.58 10.11 15 17.32 10.37 16 17.92 10.5 17 17.94 10.71 1
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    lab 6 diffusion.xlsx

  • 7 pages brittlefracturelabreportPaulScalia.pdf
    • brittlefracturelabreportPaulScalia.pdf
    • Rensselaer Polytechnic Institute
    • Materials Science for Engineers
    • MTLE 1600 - Spring 2008
    • Brittle Fracture Lab Author: Paul Scalia RPI 2020 Date: March 7, 2017 Group members: Ngai To Yu and Abdullah Kose Abstract: In our experiment, we use a tensile testing machine to place a load on slides with different surface conditions to determine their
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    brittlefracturelabreportPaulScalia.pdf

  • 6 pages Polymer Synthesis Lab.docx
    • Polymer Synthesis Lab.docx
    • Rensselaer Polytechnic Institute
    • Materials Science for Engineers
    • MTLE 1600 - Spring 2008
    • Polymer Synthesis Lab Author: Paul Scalia RPI 2020 Date: February 5, 2017 Group members: Ngai To Yu and Abdullah Kose Abstract: In our experiment, we created two polymers from two different mixtures of solutions. To create the first polymer, 1 gram of Pht
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    Polymer Synthesis Lab.docx

  • 6 pages lab 6b.xlsx
    • lab 6b.xlsx
    • Rensselaer Polytechnic Institute
    • Materials Science for Engineers
    • MTLE 1600 - Spring 2008
    • t (ps) 1000k 1500k 2000k 2500k t^1/2 (ps) 2500k 5 0.639148 2.84959 3.43588 1.33164 2.236068 1.33164 15 1.08962 1.68337 1.98143 2.26835 3.872983 2.26835 25 1.4634 2.14417 2.59202 2.932 5 2.932 35 1.68562 2.51648 3.063937 3.6245 5.91608 3.6245 45 1.91665 2.
    • Register Now

    lab 6b.xlsx

  • 1 pages Paul Scalia lab 3.docx
    • Paul Scalia lab 3.docx
    • Rensselaer Polytechnic Institute
    • Materials Science for Engineers
    • MTLE 1600 - Spring 2008
    • Paul Scalia Materials Science Undeclared Engineering RPI 2020 Lab 3 Post Lab 1) These calculations for the angles were found by doing inverse tan of the length of the lines over 9.86cm (height). The shapes found where A=hexagonal, B=rectangle, C=linear, a
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    Paul Scalia lab 3.docx

  • 6 pages lab 7 data.xlsx
    • lab 7 data.xlsx
    • Rensselaer Polytechnic Institute
    • Materials Science for Engineers
    • MTLE 1600 - Spring 2008
    • time Press (torr)Temp C time(m) 5:22 38.38 0.8 0 5:29 52.54 7.3 7 530 53.1 8 8 532 54.6 9.1 10 534 56.81 10.3 12 535 58.35 11.1 13 537 60.3 11.8 15 538 61.92 12.4 16 540 63.65 13.4 18 541 64.98 13.8 19 542 66.75 14.3 20 543 67.22 14.4 21 544 68.44 15 22 5
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    lab 7 data.xlsx

  • 8 pages One component phase diagram report Paul Scalia.pdf
    • One component phase diagram report Paul Scalia.pdf
    • Rensselaer Polytechnic Institute
    • Materials Science for Engineers
    • MTLE 1600 - Spring 2008
    • Scalia 1 One Component Phase Diagram Author: Paul Scalia RPI 2020 Date: March 29, 2017 Group members: Ngai To Yu and Abdullah Kose Scalia 2 Abstract: In this experiment we studied to boiling of cyclohexane. By using the apparatus, that is both described a
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    One component phase diagram report Paul Scalia.pdf

  • 3 pages lab 10.xlsx
    • lab 10.xlsx
    • Rensselaer Polytechnic Institute
    • Materials Science for Engineers
    • MTLE 1600 - Spring 2008
    • CW Cu d=0.64 RT= Ann Cu d=0.64 Brass d=0.5 Rm Temp Liquid N Boiling W CW Cu 9.81 1.385 12.5 Ann Cu 0.6 9.07 1.135 12 Ann Cu 0.3 52.1 32.8 57.6 Brass 33.5 4.18 45.1 Ann Cu d=0.3 Resistance vs Temp CW Cu (d=0.64m) Resis 150 100 f(x) = 26.3929486501x - 233.7
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    lab 10.xlsx

  • 3 pages Update3-ENGR1600_Syllabus_MSE_Summer2017.pdf
    • Update3-ENGR1600_Syllabus_MSE_Summer2017.pdf
    • Rensselaer Polytechnic Institute
    • Mat Sci
    • ENGR 1600 - Fall 2014
    • Syllabus for Materials Science for Engineers (ENGR-1600) Summer 2017, May 22-June 30 Course Instructor Dr. Ganpati Ramanath John Tod Horton Professor of Engineering MRC 111 Email: [email protected] Office hours: Tues 1 -2 PM, Thu 1 - 2 PM Goal: The goal of
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    Update3-ENGR1600_Syllabus_MSE_Summer2017.pdf

  • 29 pages 1600_lecture22ElectrochemistryPDF (1).pdf
    • 1600_lecture22ElectrochemistryPDF (1).pdf
    • Rensselaer Polytechnic Institute
    • Mat Sci
    • ENGR 1600 - Fall 2014
    • ENGR-1600 Materials Science for Engineers Lecture 22: Electrochemistry 1 Important Criteria in Materials Selection Criteria that are important in the process of selecting materials to meet design requirements: 1) conditions to which th
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    1600_lecture22ElectrochemistryPDF (1).pdf

  • 30 pages 1600_Lecture6Polymer Morphology (4).pdf
    • 1600_Lecture6Polymer Morphology (4).pdf
    • Rensselaer Polytechnic Institute
    • Mat Sci
    • ENGR 1600 - Fall 2014
    • ENGR-1600 Materials Science for Engineers Lecture 6: Polymers 1 Linear Polymer Morphology Molecular chains bend, coil and kink Neighboring chains may intertwine and entangle Large elastic extensions of rubbers correspond to unraveli
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    1600_Lecture6Polymer Morphology (4).pdf

  • 24 pages 1600_lecture16Diffusion (1).pdf
    • 1600_lecture16Diffusion (1).pdf
    • Rensselaer Polytechnic Institute
    • Mat Sci
    • ENGR 1600 - Fall 2014
    • ENGR-1600 Materials Science for Engineers Lecture 16: Diffusion 1 www.doitpoms.ac.uk TLP library Diffusion Mechanisms Diffusion Coefficient or Diffusivity Arrhenius equation D = diffusion coefficient [m2/s] D0 = pre-exponential [m2/s] Qd = activatio
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    1600_lecture16Diffusion (1).pdf

  • 21 pages 1600_lecture18PhaseEquilibria (2).pdf
    • 1600_lecture18PhaseEquilibria (2).pdf
    • Rensselaer Polytechnic Institute
    • Mat Sci
    • ENGR 1600 - Fall 2014
    • ENGR-1600 Materials Science for Engineers Lecture 18: Phase Equilibria, part 2 1 2 Component Phase Diagram: Solid Solution If we know T and C0, we can determine: 1600 Liquid (L) 1400 Tm Ni T(C) L + 1200 Tm Cu 1000 0 Solid () 20 40 60
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    1600_lecture18PhaseEquilibria (2).pdf

  • 41 pages 1600_Lecture5Polymers (2).pdf
    • 1600_Lecture5Polymers (2).pdf
    • Rensselaer Polytechnic Institute
    • Mat Sci
    • ENGR 1600 - Fall 2014
    • ENGR-1600 Materials Science for Engineers Lecture 5: Polymers 1 Lecture #5 Polymers: Synthesis and Chemical Structure 2 Poly mer What is a Polymer? many repeat unit repeat unit repeat unit repeat unit H H H H H H H H H H H H H H C C C
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    1600_Lecture5Polymers (2).pdf

  • 33 pages 1600_Lecture9MechPropsPDF (2).pdf
    • 1600_Lecture9MechPropsPDF (2).pdf
    • Rensselaer Polytechnic Institute
    • Mat Sci
    • ENGR 1600 - Fall 2014
    • ENGR-1600 Materials Science for Engineers Lecture 9: Mechanical Properties Macroscopic point of view 1 Why Mechanical Properties Are Important to Engineering Engineers design structures and mechanisms that must operate under demanding con
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    1600_Lecture9MechPropsPDF (2).pdf

  • 26 pages 1600_Lecture8XRDPDF (5).pdf
    • 1600_Lecture8XRDPDF (5).pdf
    • Rensselaer Polytechnic Institute
    • Mat Sci
    • ENGR 1600 - Fall 2014
    • ENGR-1600 Materials Science for Engineers Lecture 8: X-Ray Diffraction 1 Diffraction of Waves http:/www.rodenburg.org/index.html 2 Youngs Double Slit Experiment Intensity Interference of waves 4 Bragg Diffraction: Animation http:/www.doitpoms.ac.
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    1600_Lecture8XRDPDF (5).pdf

  • 18 pages 1600_lecture24ElectricalConductivityPDF (1).pdf
    • 1600_lecture24ElectricalConductivityPDF (1).pdf
    • Rensselaer Polytechnic Institute
    • Mat Sci
    • ENGR 1600 - Fall 2014
    • ENGR-1600 Materials Science for Engineers Lecture 24: Electrical Conductivity 1 Electrical Conductivity Copper vs. Aluminum wiring 2 Electrical Conductivity Electrical conductivity between different materials varies by over 20 order
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    1600_lecture24ElectricalConductivityPDF (1).pdf

  • 29 pages 1600_lecture20Microstructure1 (2).pdf
    • 1600_lecture20Microstructure1 (2).pdf
    • Rensselaer Polytechnic Institute
    • Mat Sci
    • ENGR 1600 - Fall 2014
    • ENGR-1600 Materials Science for Engineers Lecture 20: Microstructure 1 Phase Diagram (thermodynamics) where do you want to go? Binary Eutectic Phase Diagram Nucleation & Growth (kinetics) how long does it take to get there? Avrami Equati
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    1600_lecture20Microstructure1 (2).pdf

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    hoofed mammal

    • Bio Quiz 1 - ungulates
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