Tufts University Math 13 Department of Mathematics November 14, :00 noon to 1:20 pm

Size: px
Start display at page:

Download "Tufts University Math 13 Department of Mathematics November 14, :00 noon to 1:20 pm"

Transcription

1 Tufts Univesit Math 3 Depatment of Mathematics Novembe, Eam : noon to : pm Instuctions: No calculatos, notes o books ae allowed. Unless othewise stated, ou must show all wok to eceive full cedit. Simplif ou answes as much as possible. Please cicle ou answes and coss out an wok ou do not want gaded. You ae equied to sign ou eam book. ith ou signatue ou ae pledging that ou have neithe given no eceived assistance on the eam. Students found violating this pledge will eceive an F in the couse.. ( points) Tue o False - No Patial edit: On the fist page of ou blue book, answe the following questions as Tue o False. (a) + d d + d d Solution: False: the outside integal on the ight has an in its limits, which isn t allowed. (b) The point (,, z) (, 3, ) in atesian coodinates is the same as 3, θ 6, z 6 in clindical coodinates. Solution: False: the z-coodinates of the two points ae diffeent. (c) The point (,, z) (,, ) in atesian coodinates is the same as ρ, ϕ, and θ in spheical coodinates. Solution: Tue: Fist note that ϕ means that the point is in the plane, so has coodinate z. Then compute fom the fomulas: ρ cos θ sinϕ, ρ sinθ sinϕ. (d) The vecto field F(,, z),, is consevative. Solution: Tue: a potential function fo it is f(,, z). (e) If F is a consevative field and is paameteized b (t), a t b, then F d F((b)) F((a)). Solution: False: The integal on the left should give a scala as an answe, since it is the line integal of a vecto field. The values on the ight, howeve, ae vectos.. ( points) (a) Epess the volume of the solid egion, E, that sits above the ectangle in the -plane with vetices (,, ), (,, ), (,, ), and (,, ) and below the suface z in tems of a double integal. Solution: The volume of the egion between z and z within the ectangle [, ] [, ] in the plane is given b the double integal dd. (b) Evaluate the integal ou found in pat (a). Solution: dd d 3 d 3 5.

2 3. (5 points) Let R be the egion in the plane inside the cicle + and above the line. (a) Sketch R. Solution: The cicle + can be ewitten as + ( ), so it is the cicle of adius centeed at (, ). The uppe half of this cicle is above the line. R (b) Epess R in pola coodinates. Solution: Note that we can ewite the line as sin θ, o sin θ. e can also ewite the cicle + as sinθ, o sin θ. Thus, we can wite both the top and bottom boundaies of R b giving in tems of θ. e now need to find limits on θ. To do this, notice that the limits of the egion in θ will occu when sin θ and sinθ ae both satisfied: sin θ sinθ, which gives sin θ, o θ and θ 3. (Thee ae, of couse, othe values of θ that satisf sin θ, but the egion, R, onl etends into the fist and second quadants. Putting this togethe gives R { (, θ) θ 3, sin θ sinθ}. (c) ompute R f(, )da fo f(, ) +.. ( points) Solution: Fist, we make the change of vaiables fom (, ) to (, θ): R f(, )da sin θ sin θ Integating with espect to, we get R f(, )da sin θ sin θ cos θ ddθ cos θdθ sin θ sin θ cos θddθ. ( sin θ ) sin cos θdθ. θ To evaluate this, notice that we can easil make a u-substitution fo u sinθ, giving du cos θdθ, and f(, )da u R udu. (a) Rewite the iteated integal dz d d

3 as an iteated integal in the ode dz d d. Solution: e onl need to echange the outside ode in and, so we don t need to wo about the limits in z. So, we daw the sketch of the egion, D, in the plane: D Fom the pictue, we notice that the maimum limits in ae and while, fo fied, vaies fom to. This gives dz d d dz d d (b) Evaluate one of the integals fom pat (a). Solution: Eithe integal seems easonable to compute. Using the second one, we get dz d d o ( )dd dd 3 3 d 3 3 d (5 points) Let f(,, z) z and let be the egion that is above the cone z + and below the sphee + + z 8. (a) Setup (but do not evaluate) the integal f(,, z)dv in both i. lindical oodinates, and Solution: In clindical coodinates, the cone z + becomes z, while the sphee becomes + z 8. These two sufaces intesect when + 8, o. This gives limits on the z integal as z 8 (since is above the cone and below the sphee), on the integal as (because the maimum etents in the -plane coespond to a cicle of adius ), and on the θ integal as θ (since thee ae no estictions on θ. Thus, 8 z dv zdzddθ.

4 ii. Spheical oodinates. Solution: In spheical coodinates, the sphee is given b ρ 8, o ρ q. The cone is given b z + ρ cos ϕ ( ρ cos θ sin ϕ + ρ sin θ sin ϕ ) ρ sinϕ. So, cos ϕ sinϕ o tanϕ. Above (inside) the cone coesponds to angles smalle than, so the limits on ϕ ae ϕ. The cone gives no limits on ρ, so the limits on ρ ae given b ρ. No limits ae given on θ, so θ. Thus, z dv ρ cos ϕρ sin ϕdρdϕdθ ρ 3 cos ϕ sinϕdρdϕdθ. (b) Evaluate f(,, z)dv using one of the integals in pat (a). Solution: Eithe integal is eas to evaluate. In clindical coodinates: z dv In spheical coodinates: z dv ( points) Evaluate V 8 8. z z zdzddθ z 8 ρ ρ dθ ddθ ρ 3 cos ϕ sin ϕdρdϕdθ. ρ 8 8 sin ϕ ϕ ϕ dθ ( + ) / dv, whee cos ϕ sinϕdϕdθ dθ (6 8)dθ V {(, θ, z) 6, θ, z /}. 8 3 ddθ 6 cos ϕ sinϕdϕdθ

5 Solution: Using the clindical coodinates desciption of V given to us, we have V ( + dv ) / 6 / 6 sinθddθ sinθ dzddθ sinθdθ cos θ ( ) ( ). 6 / sin θdzddθ 7. ( points) Evaluate the line integal (3 )ds whee is the cuve paameteized b (t) t, 3t fo t. Solution: Fom the definition, f(, )ds omputing (t), 3, so vec (t) 5, we have (3 )ds 8. ( points) Let f(,, z) cos()sin()e z. (a) ompute the gadient field, F f. Solution: B the definition, F f f, f, f z f(t, 3t) (t) dt. ( 3(t) (3t) ) 5dt 5(8t 8t )dt 5t 3. 5t dt sin()sin()e z, cos()cos()e z, cos()sin()e z. (b) ompute the integal, F d, whee is the path given b (t) cos(t), sin(t), cos(t), t. Solution: Since F is defined as the gadient of f(,, z), we know that F is consevative. The integal of an continuous consevative field ove a closed path is alwas zeo, so F d. (Note that is closed: () ().) 9. ( points) Let F(,, z) + e z, sin(), e z + 7. Is F consevative? If so, find a potential function fo F.

6 Solution: e fist check that F is consevative. iting f(,, z) + e z, g(,, z) sin(), and h(,, z) e z + 7, we have f g f z ez h g z h. These thee conditions veif that F is consevative. To find a potential function, φ(,, z), stat b noticing that φ f(,, z) + ez. So φ(,, z) + e z d + e z + (, z). Diffeentiating this with espect to gives φ +. Matching this with g(,, z) gives ( (, z) sin() ) d cos() + K(z), o φ(,, z) + e z + cos() + K(z). Diffeentiating this with espect to z gives φ z ez + dk dz. Matching this with h(,, z) gives K(z) (e z + 7) e z dz 7z + K. Finall, this gives φ(,, z) + e z + cos() + 7z + K. To veif that φ is a potential function fo F, compute φ + e z, sin(), e z + 7. End of Eam

CS 450: COMPUTER GRAPHICS RASTERIZING CONICS SPRING 2016 DR. MICHAEL J. REALE

CS 450: COMPUTER GRAPHICS RASTERIZING CONICS SPRING 2016 DR. MICHAEL J. REALE CS 45: COMPUTER GRAPHICS RASTERIZING CONICS SPRING 6 DR. MICHAEL J. REALE RASTERIZING CURVES OTHER THAN LINES When dealing with othe inds of cuves, we can daw it in one of the following was: Use elicit

More information

4.2. Co-terminal and Related Angles. Investigate

4.2. Co-terminal and Related Angles. Investigate .2 Co-teminal and Related Angles Tigonometic atios can be used to model quantities such as

More information

Electric Field of charged hollow and solid Spheres

Electric Field of charged hollow and solid Spheres lectic Field of chaged hollow and solid Sphees Fits F.M. de Mul -field of a chaged hollow o solid sphee 1 esentations: lectomagnetism: Histoy lectomagnetism: lect. topics lectomagnetism: Magn. topics lectomagnetism:

More information

= dv 3V (r + a 1) 3 r 3 f(r) = 1. = ( (r + r 2

= dv 3V (r + a 1) 3 r 3 f(r) = 1. = ( (r + r 2 Random Waypoint Model in n-dimensional Space Esa Hyytiä and Joma Vitamo Netwoking Laboatoy, Helsinki Univesity of Technology, Finland Abstact The andom waypoint model (RWP) is one of the most widely used

More information

ME 210 Applied Mathematics for Mechanical Engineers

ME 210 Applied Mathematics for Mechanical Engineers Note that the unit vectos, T, N and B ae thee unit vectos pependicula to each othe whose diections ae dictated by the local behavio of the cuve C at its point P. They fom a moving ight handed vecto fame

More information

CALCULUS III Surface Integrals. Paul Dawkins

CALCULUS III Surface Integrals. Paul Dawkins CALCULU III uface Integals Paul awkins Table of Contents Peface... ii uface Integals... 3 Intoduction... 3 Paametic ufaces... 4 uface Integals... uface Integals of Vecto Fields... 9 tokes Theoem... 9 ivegence

More information

(a, b) x y r. For this problem, is a point in the - coordinate plane and is a positive number.

(a, b) x y r. For this problem, is a point in the - coordinate plane and is a positive number. Illustative G-C Simila cicles Alignments to Content Standads: G-C.A. Task (a, b) x y Fo this poblem, is a point in the - coodinate plane and is a positive numbe. a. Using a tanslation and a dilation, show

More information

ISyE 4256 Industrial Robotic Applications

ISyE 4256 Industrial Robotic Applications ISyE 456 Industial Robotic Applications Quiz # Oct. 9, 998 Name This is a closed book, closed notes exam. Show wok fo poblem questions ) ( pts) Please cicle one choice fo each item. a) In an application,

More information

National 5 Revision Booklet Expressions and Formula

National 5 Revision Booklet Expressions and Formula National 5 Revision Booklet Epessions and Fomula This evision coves the following topics.. Suds. Indices. Significant Figues. Suds This is a non calculato eecise.. Simplify: a. b. c. d. e. f. g. h. i..

More information

Curl, Divergence, and Gradient in Cylindrical and Spherical Coordinate Systems

Curl, Divergence, and Gradient in Cylindrical and Spherical Coordinate Systems APPENDIX B Cul, Divegence, and Gadient in Cylindical and Spheical Coodinate Systems In Sections 3., 3.4, and 6., we intoduced the cul, divegence, and gadient, espectively, and deived the expessions o them

More information

Gravitational Shift for Beginners

Gravitational Shift for Beginners Gavitational Shift fo Beginnes This pape, which I wote in 26, fomulates the equations fo gavitational shifts fom the elativistic famewok of special elativity. Fist I deive the fomulas fo the gavitational

More information

Goal. Rendering Complex Scenes on Mobile Terminals or on the web. Rendering on Mobile Terminals. Rendering on Mobile Terminals. Walking through images

Goal. Rendering Complex Scenes on Mobile Terminals or on the web. Rendering on Mobile Terminals. Rendering on Mobile Terminals. Walking through images Goal Walking though s -------------------------------------------- Kadi Bouatouch IRISA Univesité de Rennes I, Fance Rendeing Comple Scenes on Mobile Teminals o on the web Rendeing on Mobile Teminals Rendeing

More information

Vector calculus in Cartesian and spherical coordinates

Vector calculus in Cartesian and spherical coordinates SageManifolds.0 Vecto calculus in Catesian and spheical coodinates This woksheet illustates some featues of SageManifolds (vesion.0, as included in SageMath 7.5) egading vecto calculus in the Euclidean

More information

9.3 Volume of Spheres

9.3 Volume of Spheres ? LESSON 9. Volume of Sphees ESSENTIAL QUESTION How do you find the volume of a sphee? Expessions, equations, and elationships Solve poblems involving the volume of sphees. EXPLORE ACTIVITY Modeling the

More information

Lecture 27: Voronoi Diagrams

Lecture 27: Voronoi Diagrams We say that two points u, v Y ae in the same connected component of Y if thee is a path in R N fom u to v such that all the points along the path ae in the set Y. (Thee ae two connected components in the

More information

ANNOUNCEMENT. LECTURE 25 Spherical Refracting Surfaces

ANNOUNCEMENT. LECTURE 25 Spherical Refracting Surfaces ANNUNCEMENT Final: Thusday Dec 3, 208, 7 PM - 9 PM Location: Elliot Hall of Music Coves all eadings, lectues, homewok fom Chaptes 28 though 33 Multiple choice Pactice exams n the couse website and on CHIP

More information

2. PROPELLER GEOMETRY

2. PROPELLER GEOMETRY a) Fames of Refeence 2. PROPELLER GEOMETRY 10 th Intenational Towing Tank Committee (ITTC) initiated the pepaation of a dictionay and nomenclatue of ship hydodynamic tems and this wok was completed in

More information

Image Enhancement in the Spatial Domain. Spatial Domain

Image Enhancement in the Spatial Domain. Spatial Domain 8-- Spatial Domain Image Enhancement in the Spatial Domain What is spatial domain The space whee all pixels fom an image In spatial domain we can epesent an image by f( whee x and y ae coodinates along

More information

Massachusetts Institute of Technology Department of Mechanical Engineering

Massachusetts Institute of Technology Department of Mechanical Engineering cm cm Poblem Massachusetts Institute of echnolog Depatment of Mechanical Engineeing. Intoduction to obotics Sample Poblems and Solutions fo the Mid-em Exam Figue shows a obotic vehicle having two poweed

More information

Introduction To Robotics (Kinematics, Dynamics, and Design)

Introduction To Robotics (Kinematics, Dynamics, and Design) Intoduction o obotics Kinematics Dnamics and Design EION # 9: satial Descitions & ansfomations li Meghdai ofesso chool of Mechanical Engineeing haif Univesit of echnolog ehan IN 365-9567 Homeage: htt://meghdai.shaif.edu

More information

Introduction to Medical Imaging. Cone-Beam CT. Introduction. Available cone-beam reconstruction methods: Our discussion:

Introduction to Medical Imaging. Cone-Beam CT. Introduction. Available cone-beam reconstruction methods: Our discussion: Intoduction Intoduction to Medical Imaging Cone-Beam CT Klaus Muelle Available cone-beam econstuction methods: exact appoximate Ou discussion: exact (now) appoximate (next) The Radon tansfom and its invese

More information

Also available at ISSN (printed edn.), ISSN (electronic edn.) ARS MATHEMATICA CONTEMPORANEA 3 (2010)

Also available at  ISSN (printed edn.), ISSN (electronic edn.) ARS MATHEMATICA CONTEMPORANEA 3 (2010) Also available at http://amc.imfm.si ISSN 1855-3966 (pinted edn.), ISSN 1855-3974 (electonic edn.) ARS MATHEMATICA CONTEMPORANEA 3 (2010) 109 120 Fulleene patches I Jack E. Gave Syacuse Univesity, Depatment

More information

Finding point-pairs. Find Closest Point from Dense Cloud

Finding point-pairs. Find Closest Point from Dense Cloud Finding point-pais Given an a, find a coesponding b on the suface. Then one appoach would be to seach evey possible tiangle o suface point and then take the closest point. The key is to find a moe efficient

More information

Output Primitives. Ellipse Drawing

Output Primitives. Ellipse Drawing Output Pimitives Ellipse Dawing Ellipses. An ellipses is an elongated cicle and can be dawn with modified cicle dawing algoithm.. An ellipse has set of fied points (foci) that will have a constant total

More information

Prof. Feng Liu. Fall /17/2016

Prof. Feng Liu. Fall /17/2016 Pof. Feng Liu Fall 26 http://www.cs.pdx.edu/~fliu/couses/cs447/ /7/26 Last time Compositing NPR 3D Gaphics Toolkits Tansfomations 2 Today 3D Tansfomations The Viewing Pipeline Mid-tem: in class, Nov. 2

More information

Complete Solution to Potential and E-Field of a sphere of radius R and a charge density ρ[r] = CC r 2 and r n

Complete Solution to Potential and E-Field of a sphere of radius R and a charge density ρ[r] = CC r 2 and r n Complete Solution to Potential and E-Field of a sphee of adius R and a chage density ρ[] = CC 2 and n Deive the electic field and electic potential both inside and outside of a sphee of adius R with a

More information

5 4 THE BERNOULLI EQUATION

5 4 THE BERNOULLI EQUATION 185 CHATER 5 the suounding ai). The fictional wok tem w fiction is often expessed as e loss to epesent the loss (convesion) of mechanical into themal. Fo the idealied case of fictionless motion, the last

More information

Elliptic Generation Systems

Elliptic Generation Systems 4 Elliptic Geneation Systems Stefan P. Spekeijse 4.1 Intoduction 4.1 Intoduction 4.2 Two-Dimensional Gid Geneation Hamonic Maps, Gid Contol Maps, and Poisson Systems Discetization and Solution Method Constuction

More information

A Mathematical Implementation of a Global Human Walking Model with Real-Time Kinematic Personification by Boulic, Thalmann and Thalmann.

A Mathematical Implementation of a Global Human Walking Model with Real-Time Kinematic Personification by Boulic, Thalmann and Thalmann. A Mathematical Implementation of a Global Human Walking Model with Real-Time Kinematic Pesonification by Boulic, Thalmann and Thalmann. Mashall Badley National Cente fo Physical Acoustics Univesity of

More information

Dr. A.B.M. Toufique Hasan. Lecture-13

Dr. A.B.M. Toufique Hasan. Lecture-13 7/5/8 ME 45: Aeodynamics D. A.B.M. Toufique Hasan Pofesso Depatment of Mechanical Engineeing g Bangladesh Univesity of Engineeing & Technology BUET, Dhaka Lectue-3 7/5/8 Doublet & Flow Ove a stationey

More information

Improved Fourier-transform profilometry

Improved Fourier-transform profilometry Impoved Fouie-tansfom pofilomety Xianfu Mao, Wenjing Chen, and Xianyu Su An impoved optical geomety of the pojected-finge pofilomety technique, in which the exit pupil of the pojecting lens and the entance

More information

FACE VECTORS OF FLAG COMPLEXES

FACE VECTORS OF FLAG COMPLEXES FACE VECTORS OF FLAG COMPLEXES ANDY FROHMADER Abstact. A conjectue of Kalai and Eckhoff that the face vecto of an abitay flag complex is also the face vecto of some paticula balanced complex is veified.

More information

Fifth Wheel Modelling and Testing

Fifth Wheel Modelling and Testing Fifth heel Modelling and Testing en Masoy Mechanical Engineeing Depatment Floida Atlantic Univesity Boca aton, FL 4 Lois Malaptias IFMA Institut Fancais De Mechanique Advancee ampus De lemont Feand Les

More information

5. Geometric Transformations and Projections

5. Geometric Transformations and Projections 5. Geometic Tansfomations and ojections 5. Tanslations and Rotations a) Tanslation d d d d d d d d b) Scaling s s s s c) Reflection (about - - lane) d) Rotation about Ais ( ) ( ) CCW 5.. Homogeneous Repesentation

More information

9.5 Volume of Pyramids

9.5 Volume of Pyramids 9.5 Volume of Pyamids and Cones Goal Find the volumes of pyamids and cones. Key Wods pyamid p. 49 cone p. 49 volume p. 500 In the puzzle below, you can see that the squae pism can be made using thee conguent

More information

Conservation Law of Centrifugal Force and Mechanism of Energy Transfer Caused in Turbomachinery

Conservation Law of Centrifugal Force and Mechanism of Energy Transfer Caused in Turbomachinery Poceedings of the 4th WSEAS Intenational Confeence on luid Mechanics and Aeodynamics, Elounda, Geece, August 1-3, 006 (pp337-34) Consevation Law of Centifugal oce and Mechanism of Enegy Tansfe Caused in

More information

Math 2374 Spring 2007 Midterm 3 Solutions - Page 1 of 6 April 25, 2007

Math 2374 Spring 2007 Midterm 3 Solutions - Page 1 of 6 April 25, 2007 Math 374 Spring 7 Midterm 3 Solutions - Page of 6 April 5, 7. (3 points) Consider the surface parametrized by (x, y, z) Φ(x, y) (x, y,4 (x +y )) between the planes z and z 3. (i) (5 points) Set up the

More information

9/5/2018. Physics colloquium today -- 9/05/2018 PHY 711 Fall Lecture /05/2018 PHY 711 Fall Lecture 4 3

9/5/2018. Physics colloquium today -- 9/05/2018 PHY 711 Fall Lecture /05/2018 PHY 711 Fall Lecture 4 3 PHY 7 Classical Mechanics and Mathematical Methods 0-0:50 AM MWF Olin 03 Plan fo Lectue 4: Reading: Chapte F&W. Summay of pevious discussion of scatteing theoy; tansfomation etween la and cente of mass

More information

On a piece of graph paper, draw a circle that has a radius of 5 and center at ( 0, 0 ).

On a piece of graph paper, draw a circle that has a radius of 5 and center at ( 0, 0 ). 10.1 Stat Thinking On a piece of gaph pape, daw a cicle that has a adius of 5 and cente at ( 0, 0 ). 1. aw the segment that connects the points ( 3, 4 ) and ( 4, 3) on the cicle. Is this segment a diamete?

More information

O x 40 O. O x. Determine whether a tangent line is shown in each diagram. Explain

O x 40 O. O x. Determine whether a tangent line is shown in each diagram. Explain -1 Pactice Fom G Tangent Lines lgeba ssume that lines that appea to be tangent ae tangent. is the cente of each cicle. What is the value of? 1. 140 2. 3 3. 20 40 70 51 The cicle at the ight epesents Eath.

More information

Topic 4 Root Finding

Topic 4 Root Finding Couse Instucto D. Ramond C. Rump Oice: A 337 Phone: (915) 747 6958 E Mail: cump@utep.edu Topic 4 EE 4386/531 Computational Methods in EE Outline Intoduction Backeting Methods The Bisection Method False

More information

Section Parametrized Surfaces and Surface Integrals. (I) Parametrizing Surfaces (II) Surface Area (III) Scalar Surface Integrals

Section Parametrized Surfaces and Surface Integrals. (I) Parametrizing Surfaces (II) Surface Area (III) Scalar Surface Integrals Section 16.4 Parametrized Surfaces and Surface Integrals (I) Parametrizing Surfaces (II) Surface Area (III) Scalar Surface Integrals MATH 127 (Section 16.4) Parametrized Surfaces and Surface Integrals

More information

Extract Object Boundaries in Noisy Images using Level Set. Final Report

Extract Object Boundaries in Noisy Images using Level Set. Final Report Extact Object Boundaies in Noisy Images using Level Set by: Quming Zhou Final Repot Submitted to Pofesso Bian Evans EE381K Multidimensional Digital Signal Pocessing May 10, 003 Abstact Finding object contous

More information

Parametric Scattering Models for Bistatic Synthetic Aperture Radar

Parametric Scattering Models for Bistatic Synthetic Aperture Radar Paametic Scatteing Models fo Bistatic Synthetic Apetue Rada Julie Ann Jackson Student Membe, Bian D. Rigling Membe, Randolph L. Moses Senio Membe The Ohio State Univesity, Dept. of Electical and Compute

More information

ME 305 Fluid Mechanics I. Part 3 Introduction to Fluid Flow. Field Representation. Different Viewpoints for Fluid and Solid Mechanics (cont d)

ME 305 Fluid Mechanics I. Part 3 Introduction to Fluid Flow. Field Representation. Different Viewpoints for Fluid and Solid Mechanics (cont d) ME 305 Fluid Mechanics I Pat 3 Intoduction to Fluid Flow Field Repesentation As a fluid moves, its popeties in geneal change fom point to point in space and fom time to time. In field epesentation of a

More information

CS-184: Computer Graphics. Today. Lecture #5: 3D Transformations and Rotations. Transformations in 3D Rotations

CS-184: Computer Graphics. Today. Lecture #5: 3D Transformations and Rotations. Transformations in 3D Rotations CS-184: Compute Gaphics Lectue #5: 3D Tansfomations and Rotations Pof. James O Bien Univesity of Califonia, Bekeley V2009-F-05-1.0 Today Tansfomations in 3D Rotations Matices Eule angles Eponential maps

More information

Lecture # 04. Image Enhancement in Spatial Domain

Lecture # 04. Image Enhancement in Spatial Domain Digital Image Pocessing CP-7008 Lectue # 04 Image Enhancement in Spatial Domain Fall 2011 2 domains Spatial Domain : (image plane) Techniques ae based on diect manipulation of pixels in an image Fequency

More information

Research Article. Regularization Rotational motion image Blur Restoration

Research Article. Regularization Rotational motion image Blur Restoration Available online www.jocp.com Jounal of Chemical and Phamaceutical Reseach, 6, 8(6):47-476 Reseach Aticle ISSN : 975-7384 CODEN(USA) : JCPRC5 Regulaization Rotational motion image Blu Restoation Zhen Chen

More information

A Memory Efficient Array Architecture for Real-Time Motion Estimation

A Memory Efficient Array Architecture for Real-Time Motion Estimation A Memoy Efficient Aay Achitectue fo Real-Time Motion Estimation Vasily G. Moshnyaga and Keikichi Tamau Depatment of Electonics & Communication, Kyoto Univesity Sakyo-ku, Yoshida-Honmachi, Kyoto 66-1, JAPAN

More information

^2 PMAC NC FOR MILL APPLICATION

^2 PMAC NC FOR MILL APPLICATION ^1 SOFTWARE REFERENCE MANUA ^2 PMAC NC FOR MI APPICATION ^3 Integato/Softwae Manual ^4 3xx-603450-xSxx ^5 June 11, 2004 Single Souce Machine Contol Powe // Flexibility // Ease of Use 21314 assen Steet

More information

Math Triple Integrals in Cylindrical Coordinates

Math Triple Integrals in Cylindrical Coordinates Math 213 - Triple Integrals in Cylindrical Coordinates Peter A. Perry University of Kentucky November 2, 218 Homework Re-read section 15.7 Work on section 15.7, problems 1-13 (odd), 17-21 (odd) from Stewart

More information

MAT 1275: Introduction to Mathematical Analysis

MAT 1275: Introduction to Mathematical Analysis MAT 7: Intductin t Mathematical Analysis D A Rzenblyum Tignmetic Functins f Abitay Angles Unit Cicle In the pevius sectin we defined tig functins f acute angles: we cnstucted ight tiangle with given angle,

More information

Math 21a Final Exam Solutions Spring, 2009

Math 21a Final Exam Solutions Spring, 2009 Math a Final Eam olutions pring, 9 (5 points) Indicate whether the following statements are True or False b circling the appropriate letter No justifications are required T F The (vector) projection of

More information

A Description Method of Spatial Complexity in Terms of Visibility

A Description Method of Spatial Complexity in Terms of Visibility IPR IPT IGU UCI CIG ACG Table of contents Table des matièes Authos inde Inde des auteus each Recheches Eit oti A Desciption Method of patial Compleit in Tems of Visibilit Hiotaka uzuki Assistant Pofesso,

More information

Pledge: Signature:

Pledge: Signature: S/PM 0 Final Exam 7 May 005 Name: KEY E-mail ID: @viginia.edu Pledge: Signatue: Thee ae 80 minutes 3 hous fo this exam and 80 oints on the test; don t send too long on any one uestion! Thee is an exam

More information

Elastohydrodynamic Lubrication Analysis of Journal Bearings Using CAD

Elastohydrodynamic Lubrication Analysis of Journal Bearings Using CAD The 3d Intenational Confeence on Design Engineeing and Science, ICDES 1 Pilsen, Czech Repulic, August 31 Septeme 3, 1 Elastohydodynamic Luication Analysis of Jounal Beaings Using CAD Toshihio OZASA *1,

More information

Computer Graphics and Animation 3-Viewing

Computer Graphics and Animation 3-Viewing Compute Gaphics and Animation 3-Viewing Pof. D. Chales A. Wüthich, Fakultät Medien, Medieninfomatik Bauhaus-Univesität Weima caw AT medien.uni-weima.de Ma 5 Chales A. Wüthich Viewing Hee: Viewing in 3D

More information

Lecture 5: Rendering Equation Chapter 2 in Advanced GI

Lecture 5: Rendering Equation Chapter 2 in Advanced GI Lectue 5: Rendeing Equation Chapte in Advanced GI Fall 004 Kavita Bala Compute Science Conell Univesity Radiomety Radiomety: measuement of light enegy Defines elation between Powe Enegy Radiance Radiosity

More information

Modelling of real kinematics situation as a method of the system approach to the algorithm development thinking

Modelling of real kinematics situation as a method of the system approach to the algorithm development thinking Issue 4, Volume 4, 010 83 Modelling of eal kinematics situation as a method of the sstem appoach to the algoithm development thinking Stepan Hubalovsk Abstact - One of the most impotant tasks in teaching

More information

ART GALLERIES WITH INTERIOR WALLS. March 1998

ART GALLERIES WITH INTERIOR WALLS. March 1998 ART GALLERIES WITH INTERIOR WALLS Andé Kündgen Mach 1998 Abstact. Conside an at galley fomed by a polygon on n vetices with m pais of vetices joined by inteio diagonals, the inteio walls. Each inteio wall

More information

Directional Stiffness of Electronic Component Lead

Directional Stiffness of Electronic Component Lead Diectional Stiffness of Electonic Component Lead Chang H. Kim Califonia State Univesit, Long Beach Depatment of Mechanical and Aeospace Engineeing 150 Bellflowe Boulevad Long Beach, CA 90840-830, USA Abstact

More information

MATH 261 EXAM III PRACTICE PROBLEMS

MATH 261 EXAM III PRACTICE PROBLEMS MATH 6 EXAM III PRACTICE PROBLEMS These practice problems are pulled from actual midterms in previous semesters. Exam 3 typically has 5 (not 6!) problems on it, with no more than one problem of any given

More information

Title. Author(s)NOMURA, K.; MOROOKA, S. Issue Date Doc URL. Type. Note. File Information

Title. Author(s)NOMURA, K.; MOROOKA, S. Issue Date Doc URL. Type. Note. File Information Title CALCULATION FORMULA FOR A MAXIMUM BENDING MOMENT AND THE TRIANGULAR SLAB WITH CONSIDERING EFFECT OF SUPPO UNIFORM LOAD Autho(s)NOMURA, K.; MOROOKA, S. Issue Date 2013-09-11 Doc URL http://hdl.handle.net/2115/54220

More information

Derivation of the Nodal Forces Equivalent to Uniform Pressure for Quadratic Isoparametric Elements RAWB, Last Update: 30 September 2008

Derivation of the Nodal Forces Equivalent to Uniform Pressure for Quadratic Isoparametric Elements RAWB, Last Update: 30 September 2008 Deivation of the odal oces Equivalent to Unifom Pessue fo Quadatic sopaametic Elements RWB, Last Update: 0 Septembe 008 The displacement vecto u at an point within a single element, E, is lineal elated

More information

Math 241, Final Exam. 12/11/12.

Math 241, Final Exam. 12/11/12. Math, Final Exam. //. No notes, calculator, or text. There are points total. Partial credit may be given. ircle or otherwise clearly identify your final answer. Name:. (5 points): Equation of a line. Find

More information

A New and Efficient 2D Collision Detection Method Based on Contact Theory Xiaolong CHENG, Jun XIAO a, Ying WANG, Qinghai MIAO, Jian XUE

A New and Efficient 2D Collision Detection Method Based on Contact Theory Xiaolong CHENG, Jun XIAO a, Ying WANG, Qinghai MIAO, Jian XUE 5th Intenational Confeence on Advanced Mateials and Compute Science (ICAMCS 2016) A New and Efficient 2D Collision Detection Method Based on Contact Theoy Xiaolong CHENG, Jun XIAO a, Ying WANG, Qinghai

More information

2D Transformations. Why Transformations. Translation 4/17/2009

2D Transformations. Why Transformations. Translation 4/17/2009 4/7/9 D Tansfomations Wh Tansfomations Coodinate sstem tansfomations Placing objects in the wold Move/animate the camea fo navigation Dawing hieachical chaactes Animation Tanslation + d 5,4 + d,3 d 4,

More information

Monte Carlo Techniques for Rendering

Monte Carlo Techniques for Rendering Monte Calo Techniques fo Rendeing CS 517 Fall 2002 Compute Science Conell Univesity Announcements No ectue on Thusday Instead, attend Steven Gotle, Havad Upson Hall B17, 4:15-5:15 (efeshments ealie) Geomety

More information

UNIVERSITI TEKNOLOGI MALAYSIA SSCE 1993 ENGINEERING MATHEMATICS II TUTORIAL 2. 1 x cos dy dx x y dy dx. y cosxdy dx

UNIVERSITI TEKNOLOGI MALAYSIA SSCE 1993 ENGINEERING MATHEMATICS II TUTORIAL 2. 1 x cos dy dx x y dy dx. y cosxdy dx UNIVESITI TEKNOLOI MALAYSIA SSCE 99 ENINEEIN MATHEMATICS II TUTOIAL. Evaluate the following iterated integrals. (e) (g) (i) x x x sinx x e x y dy dx x dy dx y y cosxdy dx xy x + dxdy (f) (h) (y + x)dy

More information

Math 52 Homework 2 Solutions

Math 52 Homework 2 Solutions Math 52 Homework 2 Solutions October 3, 28 Problem. If is a verticall simple region then we know that the double integral da computes the area of. On the other hand, one can also compute the area of as

More information

TESSELLATIONS. This is a sample (draft) chapter from: MATHEMATICAL OUTPOURINGS. Newsletters and Musings from the St. Mark s Institute of Mathematics

TESSELLATIONS. This is a sample (draft) chapter from: MATHEMATICAL OUTPOURINGS. Newsletters and Musings from the St. Mark s Institute of Mathematics TESSELLATIONS This is a sample (daft) chapte fom: MATHEMATICAL OUTPOURINGS Newslettes and Musings fom the St. Mak s Institute of Mathematics James Tanton www.jamestanton.com This mateial was and can still

More information

A Resource for Free-standing Mathematics Units

A Resource for Free-standing Mathematics Units A Resouce fo Fee-stnding Mthemtics Units A od tunnel is designed to hve coss section tht consists of m ectngle sumounted by semi-cicle s shown in the sketch. The height of the side of the tunnel is to

More information

Physical simulation for animation

Physical simulation for animation Physical simulation fo animation Case study: The jello cube The Jello Cube Mass-Sping System Collision Detection Integatos Septembe 17 2002 1 Announcements Pogamming assignment 3 is out. It is due Tuesday,

More information

Flux Integrals. Solution. We want to visualize the surface together with the vector field. Here s a picture of exactly that:

Flux Integrals. Solution. We want to visualize the surface together with the vector field. Here s a picture of exactly that: Flu Integrals The pictures for problems # - #4 are on the last page.. Let s orient each of the three pictured surfaces so that the light side is considered to be the positie side. Decide whether each of

More information

GTOC 9, Multiple Space Debris Rendezvous Trajectory Design in the J2 environment

GTOC 9, Multiple Space Debris Rendezvous Trajectory Design in the J2 environment GTOC 9, Multiple Space Debis Rendezvous Tajectoy Design in the J envionment Macus Hallmann, Makus Schlottee, Ansga Heidecke, Maco Sagliano Fedeico Fumenti, Volke Maiwald, René Schwaz Institute of Space

More information

Calculus III. Math 233 Spring In-term exam April 11th. Suggested solutions

Calculus III. Math 233 Spring In-term exam April 11th. Suggested solutions Calculus III Math Spring 7 In-term exam April th. Suggested solutions This exam contains sixteen problems numbered through 6. Problems 5 are multiple choice problems, which each count 5% of your total

More information

Optical Flow for Large Motion Using Gradient Technique

Optical Flow for Large Motion Using Gradient Technique SERBIAN JOURNAL OF ELECTRICAL ENGINEERING Vol. 3, No. 1, June 2006, 103-113 Optical Flow fo Lage Motion Using Gadient Technique Md. Moshaof Hossain Sake 1, Kamal Bechkoum 2, K.K. Islam 1 Abstact: In this

More information

EYE DIRECTION BY STEREO IMAGE PROCESSING USING CORNEAL REFLECTION ON AN IRIS

EYE DIRECTION BY STEREO IMAGE PROCESSING USING CORNEAL REFLECTION ON AN IRIS EYE DIRECTION BY STEREO IMAGE PROCESSING USING CORNEAL REFLECTION ON AN IRIS Kumiko Tsuji Fukuoka Medical technology Teikyo Univesity 4-3-14 Shin-Katsutachi-Machi Ohmuta Fukuoka 836 Japan email: c746g@wisdomcckyushu-uacjp

More information

Applications of Triple Integrals

Applications of Triple Integrals Chapter 14 Multiple Integrals 1 Double Integrals, Iterated Integrals, Cross-sections 2 Double Integrals over more general regions, Definition, Evaluation of Double Integrals, Properties of Double Integrals

More information

Calculus IV. Exam 2 November 13, 2003

Calculus IV. Exam 2 November 13, 2003 Name: Section: Calculus IV Math 1 Fall Professor Ben Richert Exam November 1, Please do all your work in this booklet and show all the steps. Calculators and note-cards are not allowed. Problem Possible

More information

a Not yet implemented in current version SPARK: Research Kit Pointer Analysis Parameters Soot Pointer analysis. Objectives

a Not yet implemented in current version SPARK: Research Kit Pointer Analysis Parameters Soot Pointer analysis. Objectives SPARK: Soot Reseach Kit Ondřej Lhoták Objectives Spak is a modula toolkit fo flow-insensitive may points-to analyses fo Java, which enables expeimentation with: vaious paametes of pointe analyses which

More information

Color Interpolation for Single CCD Color Camera

Color Interpolation for Single CCD Color Camera Colo Intepolation fo Single CCD Colo Camea Yi-Ming Wu, Chiou-Shann Fuh, and Jui-Pin Hsu Depatment of Compute Science and Infomation Engineeing, National Taian Univesit, Taipei, Taian Email: 88036@csie.ntu.edu.t;

More information

On Error Estimation in Runge-Kutta Methods

On Error Estimation in Runge-Kutta Methods Leonado Jounal of Sciences ISSN 1583-0233 Issue 18, Januay-June 2011 p. 1-10 On Eo Estimation in Runge-Kutta Methods Ochoche ABRAHAM 1,*, Gbolahan BOLARIN 2 1 Depatment of Infomation Technology, 2 Depatment

More information

17/5/2009. Introduction

17/5/2009. Introduction 7/5/9 Steeo Imaging Intoduction Eample of Human Vision Peception of Depth fom Left and ight eye images Diffeence in elative position of object in left and ight eyes. Depth infomation in the views?? 7/5/9

More information

Conversion Functions for Symmetric Key Ciphers

Conversion Functions for Symmetric Key Ciphers Jounal of Infomation Assuance and Secuity 2 (2006) 41 50 Convesion Functions fo Symmetic Key Ciphes Deba L. Cook and Angelos D. Keomytis Depatment of Compute Science Columbia Univesity, mail code 0401

More information

MATH203 Calculus. Dr. Bandar Al-Mohsin. School of Mathematics, KSU

MATH203 Calculus. Dr. Bandar Al-Mohsin. School of Mathematics, KSU School of Mathematics, KSU Theorem The rectangular coordinates (x, y, z) and the cylindrical coordinates (r, θ, z) of a point P are related as follows: x = r cos θ, y = r sin θ, tan θ = y x, r 2 = x 2

More information

DISTRIBUTION MIXTURES

DISTRIBUTION MIXTURES Application Example 7 DISTRIBUTION MIXTURES One fequently deals with andom vaiables the distibution of which depends on vaious factos. One example is the distibution of atmospheic paametes such as wind

More information

Math Exam III Review

Math Exam III Review Math 213 - Exam III Review Peter A. Perry University of Kentucky April 10, 2019 Homework Exam III is tonight at 5 PM Exam III will cover 15.1 15.3, 15.6 15.9, 16.1 16.2, and identifying conservative vector

More information

CSE 165: 3D User Interaction

CSE 165: 3D User Interaction CSE 165: 3D Use Inteaction Lectue #6: Selection Instucto: Jugen Schulze, Ph.D. 2 Announcements Homewok Assignment #2 Due Fiday, Januay 23 d at 1:00pm 3 4 Selection and Manipulation 5 Why ae Selection and

More information

Lecture 3: Rendering Equation

Lecture 3: Rendering Equation Lectue 3: Rendeing Equation CS 660, Sping 009 Kavita Bala Compute Science Conell Univesity Radiomety Radiomety: measuement of light enegy Defines elation between Powe Enegy Radiance Radiosity 1 Hemispheical

More information

MATH 010B - Spring 2018 Worked Problems - Section 6.2. ze x2 +y 2

MATH 010B - Spring 2018 Worked Problems - Section 6.2. ze x2 +y 2 MATH B - Spring 8 orked Problems - Section 6.. Compute the following double integral x +y 9 z 3 ze x +y dv Solution: Here, we can t hope to integrate this directly in Cartesian coordinates, since the the

More information

Illumination methods for optical wear detection

Illumination methods for optical wear detection Illumination methods fo optical wea detection 1 J. Zhang, 2 P.P.L.Regtien 1 VIMEC Applied Vision Technology, Coy 43, 5653 LC Eindhoven, The Nethelands Email: jianbo.zhang@gmail.com 2 Faculty Electical

More information

MATH 200 EXAM 2 SPRING April 27, 2011

MATH 200 EXAM 2 SPRING April 27, 2011 MATH 00 EXAM SPRING 00-0 April 7, 0 Name: Section: ONLY THE CORRECT ANSWER AND ALL WORK USED TO REACH IT WILL EARN FULL CREDIT. Simplify all answers as much as possible unless eplicitly stated otherwise.

More information

UCLA Papers. Title. Permalink. Authors. Publication Date. Localized Edge Detection in Sensor Fields. https://escholarship.org/uc/item/3fj6g58j

UCLA Papers. Title. Permalink. Authors. Publication Date. Localized Edge Detection in Sensor Fields. https://escholarship.org/uc/item/3fj6g58j UCLA Papes Title Localized Edge Detection in Senso Fields Pemalink https://escholashipog/uc/item/3fj6g58j Authos K Chintalapudi Govindan Publication Date 3-- Pee eviewed escholashipog Poweed by the Califonia

More information

sf3 RESTRICTED QUADTREE (VON HERZEN/BARR)

sf3 RESTRICTED QUADTREE (VON HERZEN/BARR) SURFACE DATA HIERARCHICAL TRIANGULAR DECOMPOSITION Appoximate suface S y plana tiangula patches whose vetices ae a suset of data points defining S Fo each patch, compute an appoximation eo. maximum eo

More information

This document contains the draft version of the following paper:

This document contains the draft version of the following paper: This document contains the daft vesion of the following pape: R. Sinha, S.K. Gupta, C.J. Paedis, P.K. Khosla. Extacting aticulation models fom CAD models of pats with cuved sufaces. ASME Jounal of Mechanical

More information

Coordinate Systems. Ioannis Rekleitis

Coordinate Systems. Ioannis Rekleitis Coodinate Systems Ioannis ekleitis Position epesentation Position epesentation is: P p p p x y z P CS-417 Intoduction to obotics and Intelligent Systems Oientation epesentations Descibes the otation of

More information

Double Integrals over Polar Coordinate

Double Integrals over Polar Coordinate 1. 15.4 DOUBLE INTEGRALS OVER POLAR COORDINATE 1 15.4 Double Integrals over Polar Coordinate 1. Polar Coordinates. The polar coordinates (r, θ) of a point are related to the rectangular coordinates (x,y)

More information

UCB CS61C : Machine Structures

UCB CS61C : Machine Structures inst.eecs.bekeley.edu/~cs61c UCB CS61C : Machine Stuctues Lectue SOE Dan Gacia Lectue 28 CPU Design : Pipelining to Impove Pefomance 2010-04-05 Stanfod Reseaches have invented a monitoing technique called

More information

Historical perspective of laser beam shaping

Historical perspective of laser beam shaping Histoical pespective of lase beam shaping David L. Shealy Univesity of Alabama at Bimingham Depatment of Physics, 530 3 d Avenue South, CH30 Bimingham, AL 3594-70 USA ABSTRACT An oveview of the histoy

More information