Course Hero has millions of student submitted documents similar to the one
below including study guides, practice problems, reference materials, practice exams, textbook help and tutor support.
Find millions of documents on Course Hero - Study Guides, Lecture Notes, Reference Materials, Practice Exams and more.
Course Hero has millions of course specific materials providing students with the best way to expand
their education.
Below is a small sample set of documents:
Allan Hancock College - ELEC - 2400
Fundamentals of Signals, Systems and FilteringBrett Ninness c Brett Ninness, School of Electrical Engineering and Computer Science The University of Newcastle, Australia.2c Brett NinnessContents1 2 Introduction Signal Types and Operations 2.1
Allan Hancock College - ELEC - 2400
2Chapter 2Signal Types and OperationsFirstly, what is a signal? It is the time evolution of a quantity. As examples, all of the following can be considered as signals The price of a share in a publically listed company; The level of water in a
Allan Hancock College - ELEC - 2400
24Chapter 3Modelling, Differential Equations and System PropertiesIn most engineering scenarios, if there are multiple signals of interest, then they will be related to one another by the laws of physics. The process of using these laws in order
Allan Hancock College - ELEC - 2400
Chapter 5Frequency Response, Fourier Analysis and Filter DesignThe Laplace transform analysis of the previous chapter provides a means whereby the response of a rather arbitrary linear (and time invariant) system to a rather arbitrary stimulus may
Allan Hancock College - ELEC - 2400
274Chapter 6Sampling, Reconstruction and the Discrete Time Fourier TransformAs the previous chapter has highlighted via the example of filter synthesis, an essential difficulty in areas of signal processing, feedback control and telecommunicatio
Allan Hancock College - ELEC - 2400
Chapter 7Z Transforms7.1 IntroductionIn continuous time, the linear systems we try to analyse and design have output responses y(t) that satisfy differential equations. In general, it is hard to solve a differential equation, but we make our job
Allan Hancock College - PHYS - 2230
School of Mathematical and Physical Sciences PHYS2230Analytical ray tracingAny ray can be traced through a system exactly, using the refraction equation: ni (ki x un) = nt (kt x un) to calculate how much the ray deviates and a transfer equation
Allan Hancock College - PHYS - 2230
School of Mathematical and Physical Sciences School of Mathematical and Physical Sciences PHYS2230 PHYS2230PHYS2230 Optical Design and Semiconductor DevicesSection 1Dr Chris FellSyllabus:Sections: 2.7 2.10, 3.2, 3.3, 3.5, 4.1 4.7, 4.11, 5.1
Allan Hancock College - PHYS - 2160
SCHOOL OF MATHEMATICAL AND PHYSICAL SCIENCES ASSESSMENT ITEM COVER SHEETSTUDENT NAME:Surname Other nameSTUDENT NUMBER: COURSE:Code TitlePHYS_2160ASSESSMENT ITEM TITLE LECTURER/TUTOR: DATE DUE / TIME:EXTENSION: Applied for Y N Granted until
Allan Hancock College - PHYS - 2160
Incident frequency vs Oscillation amplitudeElectron oscillation amplitude0 0 0 0 0 0 0 0 0 0 1 2 3 4 5 6 7Incident light frequency (x10^15 Hz)Phase difference vs frequency of incident light4.00E+015 Phase difference between electron oscillat
Allan Hancock College - PHYS - 2160
Critically damped oscillation1 0.9 0.8 0.7 0.6 0.5 0.4 0.3 0.2 0.1 0 0 5 10 15 time, t 20 25 30 35x(t)x(t) under t 0.95 0.9 0.86 0.82 0.78 0.74 0.7 0.67 0.64 0.61 0.58 0.55 0.52 0.5 0.47 0.45 0.43 0.41 0.39 0.37 0.35 0.33 0.32 0.3 0.29 0.27 0.26
Allan Hancock College - PHYS - 2160
Ratio of transmitted intensity to incident intensity, vs Voltage1.2Ratio of transmitted intensity to incident intensity10.80.60.40.20 0 5000 10000 Voltage 15000 20000 25000FOR ADP VOLTAGE DELTAw SINdeltaw SIN^2 (V) n 0 0.00E+00 0 0 5
Allan Hancock College - PHYS - 2160
PHYS_2160 Assignment 1 Semester 1, 2004Due: Friday March 12, 11.00 am A material is modeled as a large collection of atoms. Consider the electric field of an incident light wave interacting with a single atom. The field slightly alters the electron
Allan Hancock College - PHYS - 2160
Physics 2160 Assignment 2-2004Due: Wednesday 31th March, at 3.00 pm Question 1: Derive a Muller matrix that describes an optical diode comprising a linear polariser with Jones vector of [1,1], a magneto-optical rotator of 7.5 rotation left and a wav
Allan Hancock College - PHYS - 2160
Assignment 3 PHYS 2160: Due Friday 21st May 11:00 amQuestion1: Determine what filter and where it would have to be placed in the apparatus shown in Figure 1 below to transform the left hand Ronchi grating combination Figure 2 (a) into the image in F
Allan Hancock College - PHYS - 2160
PHYS 2160Assignment 4Due Friday 4th June 1:00 pm The principles of operation of lasers originated from the theoretical and physical insights and research efforts of Maxwell, Boltzmann, Planck and Einstein. (i) Identify the factors that Maxwell, Bo
Allan Hancock College - PHYS - 3320
University of Newcastle PHYS3000 Laboratory3320.2 Erbium-doped Fibre AmplifierPHYS 3320.2 Version 1.03 Prepared by John Holdsworth July, 20063320.2 Erbium-doped Fibre AmplifierThis is a two week experiment to be done in pairs.AIMThe aim of
Allan Hancock College - PHYS - 3320
University of Newcastle PHYS3000 Laboratory3320.1 Optical Adddrop multiplexerPHYS 3320.1 Version 2.01 Prepared by John Holdsworth August, 20053320.1 Optical Add-Drop Multiplexer AIMThe aim of this experiment is to make an add-drop multiplexer
Allan Hancock College - PHYS - 3320
Laboratory roster PHYS3320 Tuesday Mr BUGLER Mr HANDS Mr HAYES Mr MITCHELL Mr MURPHY Mr RYAN Mr WILLIS Mr WHEELDONWeek 2 Garrick Patrick Stuart Andrew David Frederick Jack Matthew Brendan Michael David Benjamin Anthony Scott Glen OADM FOC1&2 OADM F
Allan Hancock College - ELEC - 2200
ELEC22001. AimExperiment 1Diode ApplicationsThe aim of this experiment is to study the operation of some typical diode circuits. 2. Equipment Signal generator Decade Box Resistor Component Board - Two silicon diodes (1N4148) - 0.1 and 0.01
Allan Hancock College - ELEC - 2200
ELEC22001. AimExperiment 2BJT CharacteristicsTo measure the static characteristics of a BJT and identify the low frequency parameters of the Ebers-Moll model. 2. Equipment Semiconductor Thermal Test Board DC milli-ammeter DC milli-voltmet
Allan Hancock College - ELEC - 2200
ELEC22001. AimExperiment 3JFET LaboratoryIn this experiment the characteristics of a JFET will be examined. Further its operation in the following simple circuits will be considered: current source, common source amplifier and source follower.
Allan Hancock College - ELEC - 2200
Half wave rectifier2.782.762.742.722.7 Vout (V)2.682.662.642.622.6 0 0 0 0 Load current (A) 0 0.01 0.01 0.01Full wave rectifier10 9 8 7 6 Vout (V) 5 4 3 2 1 0 0 0 0 0.01 0.01 0.01 Load current (A) 0.01 0.01 0.02 0.02 0.02Curre
Allan Hancock College - PHYS - 3380
University of Newcastle Discipline of Physics PHYS3000 Laboratory3380.8 Erbium doped Fibre AmplifierPHYS 3380.8 Version 1.01 Prepared by John Holdsworth March, 20053380.8 EDFA AIMThe aim of this experiment is to understand the operation and m
Allan Hancock College - PHYS - 2220
Physics 214 Quantum Mechanics Lecturer: Dr Paul DastoorPrescribed Text "Modern Physics for Scientists and Engineers", Thornton and RexPhysics 214 - Quantum Mechanics1PHYS114 Atomic PhysicsExperimental basis of Quantum Theory 4.4, 4.5 Structu
Allan Hancock College - PHYS - 2220
Max Planck presented a paper on 14th December 1900 titled: "On the Theory of the Energy Distribution of the Normal Spectrum" This is regarded as the birth of Quantum Mechanics. He developed a model to explain his empirical formula for S. To do this P
Allan Hancock College - PHYS - 2220
We have seen that measurement and the properties of the system are connected. Schroedinger considered this in the "Schroedinger's cat" thought experiment which illustrates the counterintuitive notions of reality that come along with quantum mechanics
Allan Hancock College - PHYS - 2220
Solids When atoms are brought together electron wavefunctions overlap. The PEP means that all electrons must be in different states so energy levels split from atomic levels and the solution to the S.E. is different to that for an isolated atom. The
Allan Hancock College - PHYS - 2220
Solar cells A solar cell is a reverse biassed pn junction in which the geometry is optimised so incoming photons can generate electron-hole pairs in the depletion region. The external electric field sweeps the carriers away from the depletion region
Allan Hancock College - PHYS - 2220
School of Mathematical and Physical Sciences School of Mathematical and Physical Sciences PHYS 2220 PHYS 2220THE UNIVERSITY OF NEWCASTLE Faculty of Science and Information Technology School of Mathematical and Physical Sciences PHYS 2220 - Electrom