On the Inradius of a Tangential Quadrilateral

Size: px
Start display at page:

Download "On the Inradius of a Tangential Quadrilateral"

Transcription

1 Foum Geometicoum Volume 10 (2010) FORUM GEOM ISSN On the Inadius of a Tangential Quadilateal Matin Josefsson bstact. We give a suvey of known fomulas fo the inadius of a tangential quadilateal, and deive the possibly new fomula (M uvx)(m vxy)(m xyu)(m yuv) =2 uvxy(uv + xy)(ux + vy)(uy + vx) whee u, v, x and y ae the distances fom the incente to the vetices, and M = 1 (uvx + vxy + xyu + yuv) Intoduction tangential quadilateal 1 is a convex quadilateal with an incicle, that is, a cicle which is tangent to all fou sides. Not all quadilateals ae tangential. The most useful chaacteization is that its two pais of opposite sides have equal sums, a + c = b + d, whee a, b, c and d ae the sides in that ode [1, pp ]. 2 h h g g e f e Figue 1. f Klamkin s poblem It is well known that the inadius of the incicle is given by = K s whee K is the aea of the quadilateal and s is the semipeimete 3. The aea of a tangential quadilateal with sides a, b, c and d is accoding to P. Yiu [10] Publication ate: Mach 22, ommunicating Edito: Paul Yiu. 1 Othe names fo these quadilateals ae cicumsciptible quadilateal [10], cicumscibable quadilateal [9] and cicumscibed quadilateal [4]. 2 Thee exists a lot of othe inteesting chaacteizations, see [9] and [7]. 3 This fomula holds fo all polygons with an incicle, whee K in the aea of the polygon.

2 28 M. Josefsson given by 4 K = abcd sin +. 2 Fom the fomulas fo the adius and aea we conclude that the inadius of a tangential quadilateal is not detemined by the sides alone; thee must be at least one angle given, then the opposite angle can be calculated by tigonomety. nothe fomula fo the inadius is efg + fgh+ ghe + hef = e + f + g + h whee e, f, g and h ae the distances fom the fou vetices to the points whee the incicle is tangent to the sides (see Figue 1). This is inteesting, since hee the adius is only a function of fou distances and no angles! The poblem of deiving this fomula was a quickie by M. S. Klamkin, with a solution given in [5]. h 4 h g 3 g e f 1 2 e f Figue 2. Minkus 5 cicles If thee ae fou cicles with adii 1, 2, 3 and 4 inscibed in a tangential quadilateal in such a way, that each of them is tangent to two of the sides and the incicle (see Figue 2), then the adius of the incicle is a oot of the quadatic equation 2 ( ) =0 accoding to J. Minkus in [8, editoial comment]. 5 In [2, p.83] thee ae othe fomulas fo the inadius, whose deivation was only a pat of the solution of a contest poblem fom hina. If the incicle in a tangential quadilateal is tangent to the sides at points W, X, Y and Z, and if E, 4 long synthetic poof can be found in [4]. nothe way of deiving the fomula is to use the fomula K = (s a)(s b)(s c)(s d) abcd cos 2 + fo the aea of a geneal quadilateal, deived in [10, pp ], and the chaacteization a + c = b + d. 2 5 The coesponding poblem fo the tiangle is an old Sangaku poblem, solved in [8], [3, pp. 30, ].

3 On the inadius of a tangential quadilateal 29 F, G and H ae the midpoints of ZW, WX, XY and YZ espectively, then the inadius is given by the fomulas = I IE = I IF = I IG = I IH whee I is the incente (see Figue 3). The deivation is easy. Tiangles IW and IEW ae simila, so I = IE which gives the fist fomula and the othes follow by symmety. Y Z H I G X E F Figue 3. W The poblem fom hina The main pupose of this pape is to deive yet anothe (pehaps new) fomula fo the inadius of a tangential quadilateal. This fomula is also a function of only fou distances, which ae fom the incente I to the fou vetices,, and (see Figue 4). y x I u v Figue 4. The main poblem Theoem 1. If u, v, x and y ae the distances fom the incente to the vetices of a tangential quadilateal, then the inadius is given by the fomula (M uvx)(m vxy)(m xyu)(m yuv) =2 (1) uvxy(uv + xy)(ux + vy)(uy + vx)

4 30 M. Josefsson whee uvx + vxy + xyu + yuv M =. 2 Remak. It is notewothy that fomula (1) is somewhat simila to Paameshvaas fomula fo the cicumadius R of a cyclic quadilateal, 6 R = 1 (ab + cd)(ac + bd)(ad + bc) 4 (s a)(s b)(s c)(s d) whee s is the semipeimete, which is deived in [6, p.17]. 2. Peliminay esults about tiangles The poof of fomula (1) uses two equations that holds fo all tiangles. These ae two cubic equations, and one of them is a sot of coespondence to fomula (1). The fact is, that while it is possible to give as a function of the distances I, I, I and I in a tangential quadilateal, the same poblem of giving as a function of I, I and I in a tiangle is not so easy to solve, since it gives a cubic equation. The second cubic equation is found when solving the poblem, in a tiangle, of finding an exadius as a function of the distances fom the coesponding excente to the vetices. Lemma 2. If x, y and z ae the distances fom the incente to the vetices of a tiangle, then the inadius is a oot of the cubic equation 2xyz 3 +(x 2 y 2 + y 2 z 2 + z 2 x 2 ) 2 x 2 y 2 z 2 =0. (2) z γ x I α β y Figue 5. The incicle 6 quadilateal with a cicumcicle.

5 On the inadius of a tangential quadilateal 31 Poof. If α, β and γ ae the angles between these distances and the inadius (see Figue 5), we have α + β + γ = π, socos (α + β) =cos(π γ) and it follows that cos α cos β sin α sin β = cos γ. Using the fomulas cos α = x, cos β = y and sin 2 α +cos 2 α =1, we get x y 1 2 x y 2 = z o 2 xy + (x z = 2 2 )(y 2 2 ). xy Multiplying both sides with xyz, educing common factos and squaing, we get (z 2 + xy) 2 = z 2 (x 2 2 )(y 2 2 ) which afte expansion and simplification educes to (2). Lemma 3. If u, v and z ae the distances fom an excente to the vetices of a tiangle, then the coesponding exadius c is a oot of the cubic equation 2uvz 3 c (u 2 v 2 + v 2 z 2 + z 2 u 2 ) 2 c + u 2 v 2 z 2 =0. (3) γ γ α α z u v β β c I c x y E Figue 6. Excicle to tiangle and incicle to E Poof. efine angles α, β and γ to be between u, v, z and the sides of the tiangle o thei extensions (see Figue 6). Then 2α + = π, 2β + = π and 2γ =. Fom the sum of angles in a tiangle, + + = π, this simplifies to α+β = π 2 +γ. Hence cos (α + β) =cos(π 2 + γ) and it follows that cos α cos β

6 32 M. Josefsson sin α sin β = sin γ. Fo the exadius c,wehavesin α = c c u, sin β = v, sin γ = c z, and so 1 2 c u c v 2 c u c v = c z. This can, in the same way as in the poof of Lemma 2, be ewitten as z 2 (u 2 c 2 )(v 2 c 2 )=(zc 2 uv c ) 2 which afte expansion and simplification educes to (3). 3. Poof of the theoem Given a tangential quadilateal E whee the distances fom the incente to the vetices ae u, v, x and y, we see that if we extend the two sides and E to meet at, then the incicle in E is both an incicle in tiangle E and an excicle to tiangle (see Figue 6). The incicle and the excicle theefoe have the same adius, and fom (2) and (3) we get that 2xyz 3 +(x 2 y 2 + y 2 z 2 + z 2 x 2 ) 2 x 2 y 2 z 2 = 0, (4) 2uvz 3 (u 2 v 2 + v 2 z 2 + z 2 u 2 ) 2 + u 2 v 2 z 2 = 0. (5) We shall use these two equations to eliminate the common vaiable z. To do so, equation (4) is multiplied by uv and equation (5) by xy, giving 2uvxyz 3 + uv(x 2 y 2 + y 2 z 2 + z 2 x 2 ) 2 uvx 2 y 2 z 2 = 0, 2uvxyz 3 xy(u 2 v 2 + v 2 z 2 + z 2 u 2 ) 2 + xyu 2 v 2 z 2 = 0. Subtacting the second of these fom the fist gives ( uv(x 2 y 2 + y 2 z 2 + z 2 x 2 )+xy(u 2 v 2 + v 2 z 2 + z 2 u 2 ) ) 2 uvx 2 y 2 z 2 xyu 2 v 2 z 2 =0 fom which it follows uvxy 2 (xy+uv)+z 2 ( (uvy 2 + uvx 2 + xyv 2 + xyu 2 ) 2 uvxy(xy + uv) ) =0. Solving fo z 2, z 2 uvxy(uv + xy) 2 = uvxy(uv + xy) 2 (uvy 2 + uvx 2 + xyv 2 + xyu 2 ). (6) Now we multiply (4) by u 2 v 2 and (5) by x 2 y 2, which gives 2u 2 v 2 xyz 3 + u 2 v 2 (x 2 y 2 + y 2 z 2 + z 2 x 2 ) 2 u 2 v 2 x 2 y 2 z 2 = 0, 2x 2 y 2 uvz 3 x 2 y 2 (u 2 v 2 + v 2 z 2 + z 2 u 2 ) 2 + u 2 v 2 x 2 y 2 z 2 = 0. dding these we get 2uvxyz(uv + xy) 3 +(u 2 v 2 y 2 + u 2 v 2 x 2 x 2 y 2 v 2 x 2 y 2 u 2 )z 2 2 =0 and since z 2 0this educes to 2uvxy(uv + xy) +(u 2 v 2 y 2 + u 2 v 2 x 2 x 2 y 2 v 2 x 2 y 2 u 2 )z =0.

7 On the inadius of a tangential quadilateal 33 Solving fo z, we get 2uvxy(uv + xy) z = u 2 v 2 y 2 + u 2 v 2 x 2 x 2 y 2 v 2 x 2 y 2 u 2. Squaing and substituting z 2 fom (6), we get the equality uvxy(uv + xy) 2 uvxy(uv + xy) 2 (uvy 2 + uvx 2 + xyv 2 + xyu 2 ) 4(uvxy(uv + xy)) 2 2 = (u 2 v 2 y 2 + u 2 v 2 x 2 x 2 y 2 v 2 x 2 y 2 u 2 ) 2, which, since uvxy(uv + xy) 2 0, ewites as 4uvxy(uv + xy)(ux(vx + uy)+vy(uy + vx)) 2 =(2uvxy(uv + xy)) 2 (u 2 v 2 y 2 + u 2 v 2 x 2 x 2 y 2 v 2 x 2 y 2 u 2 ) 2. What is left is to facto this equation. Using the basic algebaic identities a 2 b 2 = (a + b)(a b), a 2 +2ab + b 2 =(a + b) 2 and a 2 2ab + b 2 =(a b) 2 we get 4uvxy(uv + xy)(uy + vx)(ux + vy) 2 = ( 2uvxy(uv + xy)+(uvy) 2 +(uvx) 2 (xyv) 2 (xyu) 2) (2uvxy(uv + xy) (uvy) 2 (uvx) 2 +(xyv) 2 +(xyu) 2) = ( (uvy + uvx) 2 (xyv xyu) 2)( (xyv + xyu) 2 (uvy uvx) 2) =((uvy + uvx + xyv xyu)(uvy + uvx xyv + xyu)) ((xyv + xyu + uvy uvx)(xyv + xyu uvy + uvx)). (7) Now using M = 1 2 (uvx + vxy + xyu + yuv) we get uvy + uvx + xyv xyu =(uvx + vxy + xyu + yuv) 2xyu =2(M xyu) and in the same way Thus, (7) is equivalent to uvy + uvx xyv + xyu =2(M vxy), xyv + xyu + uvy uvx =2(M uvx), xyv + xyu uvy + uvx =2(M uvy). 4uvxy(uv + xy)(uy + vx)(ux + vy) 2 =2(M uxy) 2(M vxy) 2(M uvx) 2(M uvy). Hence 2 4(M uxy)(m vxy)(m uvx)(m uvy) =. uvxy(uv + xy)(uy + vx)(ux + vy) Extacting the squae oot of both sides finishes the deivation of fomula (1).

8 34 M. Josefsson Refeences [1] T. ndeescu and. Enescu, Mathematical Olympiad Teasues, ikhäuse, oston, [2] X. in and L. P. Yee (editos), Mathematical Olympiad in hina, East hina Nomal Univesity Pess, [3] H. Fukagawa and. Pedoe, Japanese Temple Geomety Poblems San Gaku, The hales abbage Reseach ente, Winnipeg, anada, [4]. Ginbeg, icumscibed quadilateals evisited, 2008, available at ginbeg/icumrev.pdf [5] M. S. Klamkin, Five Klamkin Quickies, ux Math., 23 (1997) [6] Z.. Melzak, Invitation to Geomety, John Wiley & Sons, New Yok, 1983; new edition 2008 by ove Publications. [7] N. Minculete, haacteizations of a Tangential Quadilateal, Foum Geom., 9 (2009) [8]. Soland, Poblem 11046, me. Math. Monthly, 110 (2003) 844; solution, ibid., 113 (2006) [9]. Woall, jouney with cicumscibable quadilateals, Mathematics Teache, 98 (2004) [10] P. Yiu, Euclidean Geomety Notes, 1998 p. 157, Floida tlantic Univesity Lectue Notes, available at Matin Josefsson: Västegatan 25d, Makayd, Sweden addess: matin.makayd@hotmail.com

Heronian Triangles of Class K: Congruent Incircles Cevian Perspective

Heronian Triangles of Class K: Congruent Incircles Cevian Perspective Foum Geometicoum Volume 5 (05) 5. FORUM GEOM ISSN 534-78 Heonian Tiangles of lass K: onguent Incicles evian Pespective Fank M. Jackson and Stalislav Takhaev bstact. We elate the popeties of a cevian that

More information

Euclidean Figures and Solids without Incircles or Inspheres

Euclidean Figures and Solids without Incircles or Inspheres Foum Geometicoum Volume 16 (2016) 291 298. FOUM GEOM ISSN 1534-1178 Euclidean Figues and Solids without Incicles o Insphees Dimitis M. Chistodoulou bstact. ll classical convex plana Euclidean figues that

More information

(n 1)n(n + 1)(n + 2) + 1 = (n 1)(n + 2)n(n + 1) + 1 = ( (n 2 + n 1) 1 )( (n 2 + n 1) + 1 ) + 1 = (n 2 + n 1) 2.

(n 1)n(n + 1)(n + 2) + 1 = (n 1)(n + 2)n(n + 1) + 1 = ( (n 2 + n 1) 1 )( (n 2 + n 1) + 1 ) + 1 = (n 2 + n 1) 2. Paabola Volume 5, Issue (017) Solutions 151 1540 Q151 Take any fou consecutive whole numbes, multiply them togethe and add 1. Make a conjectue and pove it! The esulting numbe can, fo instance, be expessed

More information

Generalisations of a Four-Square Theorem. Hiroshi Okumura and John F. Rigby. results on a wooden board and dedicated it to a shrine or a temple.

Generalisations of a Four-Square Theorem. Hiroshi Okumura and John F. Rigby. results on a wooden board and dedicated it to a shrine or a temple. 20 enealisations of a ousquae Theoem Hioshi Okumua and John. Rigby In the 17 th {19 th centuies, Japanese people often wote thei mathematical esults on a wooden boad and dedicated it to a shine o a temple.

More information

The Archimedean Circles of Schoch and Woo

The Archimedean Circles of Schoch and Woo Foum Geometicoum Volume 4 (2004) 27 34. FRUM GEM ISSN 1534-1178 The Achimedean Cicles of Schoch and Woo Hioshi kumua and Masayuki Watanabe Abstact. We genealize the Achimedean cicles in an abelos (shoemake

More information

OLYMON. Produced by the Canadian Mathematical Society and the Department of Mathematics of the University of Toronto. Issue 9:2.

OLYMON. Produced by the Canadian Mathematical Society and the Department of Mathematics of the University of Toronto. Issue 9:2. OLYMON Poduced by the Canadian Mathematical Society and the Depatment of Mathematics of the Univesity of Toonto Please send you solution to Pofesso EJ Babeau Depatment of Mathematics Univesity of Toonto

More information

3.6 Applied Optimization

3.6 Applied Optimization .6 Applied Optimization Section.6 Notes Page In this section we will be looking at wod poblems whee it asks us to maimize o minimize something. Fo all the poblems in this section you will be taking the

More information

MO-ARML --- September, POWER OF A POINT

MO-ARML --- September, POWER OF A POINT M-ML --- Septembe, 208 -- W INT owe of a oint is a set of thee-theoems-in-one about cicles and line segments. * = * 2 = * * = * XISS G 8 8 2 S X H Z 3 6 H 7 T K. = 4 and X < X, find X.. ind HK.. ind TV.

More information

The CENTRE for EDUCATION in MATHEMATICS and COMPUTING cemc.uwaterloo.ca Galois Contest. Wednesday, April 12, 2017

The CENTRE for EDUCATION in MATHEMATICS and COMPUTING cemc.uwaterloo.ca Galois Contest. Wednesday, April 12, 2017 The ENTRE fo EDUATIN in MATHEMATIS and MPUTING cemc.uwateloo.ca 2017 Galois ontest Wednesday, Apil 12, 2017 (in Noth Ameica and South Ameica) Thusday, Apil 13, 2017 (outside of Noth Ameica and South Ameica)

More information

4.3 Area of a Sector. Area of a Sector Section

4.3 Area of a Sector. Area of a Sector Section ea of a Secto Section 4. 9 4. ea of a Secto In geomety you leaned that the aea of a cicle of adius is π 2. We will now lean how to find the aea of a secto of a cicle. secto is the egion bounded by a cental

More information

MATH Non-Euclidean Geometry Exercise Set 3: Solutions

MATH Non-Euclidean Geometry Exercise Set 3: Solutions MATH 68090 NonEuclidean Geomety Execise Set : Solutions Pove that the opposite angles in a convex quadilateal inscibed in a cicle sum to 80º Convesely, pove that if the opposite angles in a convex quadilateal

More information

Online Mathematics Competition Wednesday, November 30, 2016

Online Mathematics Competition Wednesday, November 30, 2016 Math@Mac Online Mathematics Competition Wednesday, Novembe 0, 206 SOLUTIONS. Suppose that a bag contains the nine lettes of the wod OXOMOXO. If you take one lette out of the bag at a time and line them

More information

Double-angle & power-reduction identities. Elementary Functions. Double-angle & power-reduction identities. Double-angle & power-reduction identities

Double-angle & power-reduction identities. Elementary Functions. Double-angle & power-reduction identities. Double-angle & power-reduction identities Double-angle & powe-eduction identities Pat 5, Tigonomety Lectue 5a, Double Angle and Powe Reduction Fomulas In the pevious pesentation we developed fomulas fo cos( β) and sin( β) These fomulas lead natually

More information

d 4 x x 170 n 20 R 8 A 200 h S 1 y 5000 x 3240 A 243

d 4 x x 170 n 20 R 8 A 200 h S 1 y 5000 x 3240 A 243 nswes: (1984-8 HKMO Final Events) eated by: M. Fancis Hung Last updated: 4 pil 017 Individual Events SI a I1 a I a 1 I3 a 4 I4 a I t 8 b 4 b 0 b 1 b 16 b 10 u 13 c c 9 c 3 c 199 c 96 v 4 d 1 d d 16 d 4

More information

New problems in universal algebraic geometry illustrated by boolean equations

New problems in universal algebraic geometry illustrated by boolean equations New poblems in univesal algebaic geomety illustated by boolean equations axiv:1611.00152v2 [math.ra] 25 Nov 2016 Atem N. Shevlyakov Novembe 28, 2016 Abstact We discuss new poblems in univesal algebaic

More information

Solving Problems of Advance of Mercury s Perihelion and Deflection of. Photon Around the Sun with New Newton s Formula of Gravity

Solving Problems of Advance of Mercury s Perihelion and Deflection of. Photon Around the Sun with New Newton s Formula of Gravity Solving Poblems of Advance of Mecuy s Peihelion and Deflection of Photon Aound the Sun with New Newton s Fomula of Gavity Fu Yuhua (CNOOC Reseach Institute, E-mail:fuyh945@sina.com) Abstact: Accoding to

More information

Physics 111 Lecture 5 (Walker: 3.3-6) Vectors & Vector Math Motion Vectors Sept. 11, 2009

Physics 111 Lecture 5 (Walker: 3.3-6) Vectors & Vector Math Motion Vectors Sept. 11, 2009 Physics 111 Lectue 5 (Walke: 3.3-6) Vectos & Vecto Math Motion Vectos Sept. 11, 2009 Quiz Monday - Chap. 2 1 Resolving a vecto into x-component & y- component: Pola Coodinates Catesian Coodinates x y =

More information

THE LAPLACE EQUATION. The Laplace (or potential) equation is the equation. u = 0. = 2 x 2. x y 2 in R 2

THE LAPLACE EQUATION. The Laplace (or potential) equation is the equation. u = 0. = 2 x 2. x y 2 in R 2 THE LAPLACE EQUATION The Laplace (o potential) equation is the equation whee is the Laplace opeato = 2 x 2 u = 0. in R = 2 x 2 + 2 y 2 in R 2 = 2 x 2 + 2 y 2 + 2 z 2 in R 3 The solutions u of the Laplace

More information

Chapter 2: Introduction to Implicit Equations

Chapter 2: Introduction to Implicit Equations Habeman MTH 11 Section V: Paametic and Implicit Equations Chapte : Intoduction to Implicit Equations When we descibe cuves on the coodinate plane with algebaic equations, we can define the elationship

More information

MATH 417 Homework 3 Instructor: D. Cabrera Due June 30. sin θ v x = v r cos θ v θ r. (b) Then use the Cauchy-Riemann equations in polar coordinates

MATH 417 Homework 3 Instructor: D. Cabrera Due June 30. sin θ v x = v r cos θ v θ r. (b) Then use the Cauchy-Riemann equations in polar coordinates MATH 417 Homewok 3 Instucto: D. Cabea Due June 30 1. Let a function f(z) = u + iv be diffeentiable at z 0. (a) Use the Chain Rule and the fomulas x = cosθ and y = to show that u x = u cosθ u θ, v x = v

More information

When two numbers are written as the product of their prime factors, they are in factored form.

When two numbers are written as the product of their prime factors, they are in factored form. 10 1 Study Guide Pages 420 425 Factos Because 3 4 12, we say that 3 and 4 ae factos of 12. In othe wods, factos ae the numbes you multiply to get a poduct. Since 2 6 12, 2 and 6 ae also factos of 12. The

More information

Force between two parallel current wires and Newton s. third law

Force between two parallel current wires and Newton s. third law Foce between two paallel cuent wies and Newton s thid law Yannan Yang (Shanghai Jinjuan Infomation Science and Technology Co., Ltd.) Abstact: In this pape, the essence of the inteaction between two paallel

More information

COLLAPSING WALLS THEOREM

COLLAPSING WALLS THEOREM COLLAPSING WALLS THEOREM IGOR PAK AND ROM PINCHASI Abstact. Let P R 3 be a pyamid with the base a convex polygon Q. We show that when othe faces ae collapsed (otated aound the edges onto the plane spanned

More information

The Derivative of the Sine and Cosine. A New Derivation Approach

The Derivative of the Sine and Cosine. A New Derivation Approach The Deivative of the Sine and Cosine. A New Deivation Appoach By John T. Katsikadelis Scool of Civil Engineeing, National Technical Univesity of Athens, Athens 15773, Geece. e-mail: jkats@cental.ntua.g

More information

Liquid gas interface under hydrostatic pressure

Liquid gas interface under hydrostatic pressure Advances in Fluid Mechanics IX 5 Liquid gas inteface unde hydostatic pessue A. Gajewski Bialystok Univesity of Technology, Faculty of Civil Engineeing and Envionmental Engineeing, Depatment of Heat Engineeing,

More information

Physics 161 Fall 2011 Extra Credit 2 Investigating Black Holes - Solutions The Following is Worth 50 Points!!!

Physics 161 Fall 2011 Extra Credit 2 Investigating Black Holes - Solutions The Following is Worth 50 Points!!! Physics 161 Fall 011 Exta Cedit Investigating Black Holes - olutions The Following is Woth 50 Points!!! This exta cedit assignment will investigate vaious popeties of black holes that we didn t have time

More information

arxiv: v1 [physics.pop-ph] 3 Jun 2013

arxiv: v1 [physics.pop-ph] 3 Jun 2013 A note on the electostatic enegy of two point chages axiv:1306.0401v1 [physics.pop-ph] 3 Jun 013 A C Tot Instituto de Física Univesidade Fedeal do io de Janeio Caixa Postal 68.58; CEP 1941-97 io de Janeio,

More information

SOME GENERAL NUMERICAL RADIUS INEQUALITIES FOR THE OFF-DIAGONAL PARTS OF 2 2 OPERATOR MATRICES

SOME GENERAL NUMERICAL RADIUS INEQUALITIES FOR THE OFF-DIAGONAL PARTS OF 2 2 OPERATOR MATRICES italian jounal of pue and applied mathematics n. 35 015 (433 44) 433 SOME GENERAL NUMERICAL RADIUS INEQUALITIES FOR THE OFF-DIAGONAL PARTS OF OPERATOR MATRICES Watheq Bani-Domi Depatment of Mathematics

More information

H.W.GOULD West Virginia University, Morgan town, West Virginia 26506

H.W.GOULD West Virginia University, Morgan town, West Virginia 26506 A F I B O N A C C I F O R M U L A OF LUCAS A N D ITS SUBSEQUENT M A N I F E S T A T I O N S A N D R E D I S C O V E R I E S H.W.GOULD West Viginia Univesity, Mogan town, West Viginia 26506 Almost eveyone

More information

What Form of Gravitation Ensures Weakened Kepler s Third Law?

What Form of Gravitation Ensures Weakened Kepler s Third Law? Bulletin of Aichi Univ. of Education, 6(Natual Sciences, pp. - 6, Mach, 03 What Fom of Gavitation Ensues Weakened Keple s Thid Law? Kenzi ODANI Depatment of Mathematics Education, Aichi Univesity of Education,

More information

A Bijective Approach to the Permutational Power of a Priority Queue

A Bijective Approach to the Permutational Power of a Priority Queue A Bijective Appoach to the Pemutational Powe of a Pioity Queue Ia M. Gessel Kuang-Yeh Wang Depatment of Mathematics Bandeis Univesity Waltham, MA 02254-9110 Abstact A pioity queue tansfoms an input pemutation

More information

Solving Some Definite Integrals Using Parseval s Theorem

Solving Some Definite Integrals Using Parseval s Theorem Ameican Jounal of Numeical Analysis 4 Vol. No. 6-64 Available online at http://pubs.sciepub.com/ajna///5 Science and Education Publishing DOI:.69/ajna---5 Solving Some Definite Integals Using Paseval s

More information

11.2 Proving Figures are Similar Using Transformations

11.2 Proving Figures are Similar Using Transformations Name lass ate 11. Poving igues ae Simila Using Tansfomations ssential Question: How can similait tansfomations be used to show two figues ae simila? esouce ocke ploe onfiming Similait similait tansfomation

More information

Using Laplace Transform to Evaluate Improper Integrals Chii-Huei Yu

Using Laplace Transform to Evaluate Improper Integrals Chii-Huei Yu Available at https://edupediapublicationsog/jounals Volume 3 Issue 4 Febuay 216 Using Laplace Tansfom to Evaluate Impope Integals Chii-Huei Yu Depatment of Infomation Technology, Nan Jeon Univesity of

More information

radians). Figure 2.1 Figure 2.2 (a) quadrant I angle (b) quadrant II angle is in standard position Terminal side Terminal side Terminal side

radians). Figure 2.1 Figure 2.2 (a) quadrant I angle (b) quadrant II angle is in standard position Terminal side Terminal side Terminal side . TRIGONOMETRIC FUNCTIONS OF GENERAL ANGLES In ode to etend the definitions of the si tigonometic functions to geneal angles, we shall make use of the following ideas: In a Catesian coodinate sstem, an

More information

Research Article On Alzer and Qiu s Conjecture for Complete Elliptic Integral and Inverse Hyperbolic Tangent Function

Research Article On Alzer and Qiu s Conjecture for Complete Elliptic Integral and Inverse Hyperbolic Tangent Function Abstact and Applied Analysis Volume 011, Aticle ID 697547, 7 pages doi:10.1155/011/697547 Reseach Aticle On Alze and Qiu s Conjectue fo Complete Elliptic Integal and Invese Hypebolic Tangent Function Yu-Ming

More information

Section 8.2 Polar Coordinates

Section 8.2 Polar Coordinates Section 8. Pola Coodinates 467 Section 8. Pola Coodinates The coodinate system we ae most familia with is called the Catesian coodinate system, a ectangula plane divided into fou quadants by the hoizontal

More information

No. 32. R.E. Woodrow. As a contest this issue we give the Junior High School Mathematics

No. 32. R.E. Woodrow. As a contest this issue we give the Junior High School Mathematics 334 THE SKOLIAD CORNER No. 32 R.E. Woodow As a contest this issue we give the Junio High School Mathematics Contest, Peliminay Round 1998 of the Bitish Columbia Colleges which was witten Mach 11, 1998.

More information

AMC 10 Contest B. Solutions Pamphlet. Wednesday, FEBRUARY 21, American Mathematics Competitions

AMC 10 Contest B. Solutions Pamphlet. Wednesday, FEBRUARY 21, American Mathematics Competitions The MATHEMATICAL ASSOCIATION of AMERICA Ameican Mathematics Competitions 8 th Annual Ameican Mathematics Contest 10 AMC 10 Contest B Solutions Pamphlet Wednesday, FEBRUARY 21, 2007 This Pamphlet gives

More information

Australian Intermediate Mathematics Olympiad 2017

Australian Intermediate Mathematics Olympiad 2017 Austalian Intemediate Mathematics Olympiad 207 Questions. The numbe x is when witten in base b, but it is 22 when witten in base b 2. What is x in base 0? [2 maks] 2. A tiangle ABC is divided into fou

More information

ESTIMATION MODELS USING MATHEMATICAL CONCEPTS AND NEWTON S LAWS FOR CONIC SECTION TRAJECTORIES ON EARTH S SURFACE

ESTIMATION MODELS USING MATHEMATICAL CONCEPTS AND NEWTON S LAWS FOR CONIC SECTION TRAJECTORIES ON EARTH S SURFACE Fundamental Jounal of Mathematical Physics Vol. 3 Issue 1 13 Pages 33-44 Published online at http://www.fdint.com/ ESTIMATION MODELS USING MATHEMATICAL CONCEPTS AND NEWTON S LAWS FOR CONIC SECTION TRAJECTORIES

More information

SUFFICIENT CONDITIONS FOR MAXIMALLY EDGE-CONNECTED AND SUPER-EDGE-CONNECTED GRAPHS DEPENDING ON THE CLIQUE NUMBER

SUFFICIENT CONDITIONS FOR MAXIMALLY EDGE-CONNECTED AND SUPER-EDGE-CONNECTED GRAPHS DEPENDING ON THE CLIQUE NUMBER Discussiones Mathematicae Gaph Theoy 39 (019) 567 573 doi:10.7151/dmgt.096 SUFFICIENT CONDITIONS FOR MAXIMALLY EDGE-CONNECTED AND SUPER-EDGE-CONNECTED GRAPHS DEPENDING ON THE CLIQUE NUMBER Lutz Volkmann

More information

A NEW GENERALIZED PARETO DISTRIBUTION. Abstract

A NEW GENERALIZED PARETO DISTRIBUTION. Abstract NEW GENERLIZED PRETO DISTRIBUTION bd Elfattah,. M. * Elshepieny, E.. * Hussein, E.. * a_afattah@hotmail.com ahmedc55@hotmail.com bstact In this pape, we intoduce a new genealized Paeto distibution and

More information

Dynamic Visualization of Complex Integrals with Cabri II Plus

Dynamic Visualization of Complex Integrals with Cabri II Plus Dynamic Visualiation of omplex Integals with abi II Plus Sae MIKI Kawai-juu, IES Japan Email: sand_pictue@hotmailcom Abstact: Dynamic visualiation helps us undestand the concepts of mathematics This pape

More information

Math 1105: Calculus I (Math/Sci majors) MWF 11am / 12pm, Campion 235 Written homework 3

Math 1105: Calculus I (Math/Sci majors) MWF 11am / 12pm, Campion 235 Written homework 3 Math : alculus I Math/Sci majos MWF am / pm, ampion Witten homewok Review: p 94, p 977,8,9,6, 6: p 46, 6: p 4964b,c,69, 6: p 47,6 p 94, Evaluate the following it by identifying the integal that it epesents:

More information

DonnishJournals

DonnishJournals DonnishJounals 041-1189 Donnish Jounal of Educational Reseach and Reviews. Vol 1(1) pp. 01-017 Novembe, 014. http:///dje Copyight 014 Donnish Jounals Oiginal Reseach Pape Vecto Analysis Using MAXIMA Savaş

More information

No. 39. R.E. Woodrow. This issue we give another example of a team competition with the problems

No. 39. R.E. Woodrow. This issue we give another example of a team competition with the problems 282 THE SKOLIAD CORNER No. 39 R.E. Woodow This issue we give anothe example of a team competition with the poblems of the 998 Floida Mathematics Olympiad, witten May 4, 998. The contest was oganized by

More information

Weighted least-squares estimators of parametric functions of the regression coefficients under a general linear model

Weighted least-squares estimators of parametric functions of the regression coefficients under a general linear model Ann Inst Stat Math (2010) 62:929 941 DOI 10.1007/s10463-008-0199-8 Weighted least-squaes estimatos of paametic functions of the egession coefficients unde a geneal linea model Yongge Tian Received: 9 Januay

More information

Magnetic Field. Conference 6. Physics 102 General Physics II

Magnetic Field. Conference 6. Physics 102 General Physics II Physics 102 Confeence 6 Magnetic Field Confeence 6 Physics 102 Geneal Physics II Monday, Mach 3d, 2014 6.1 Quiz Poblem 6.1 Think about the magnetic field associated with an infinite, cuent caying wie.

More information

KOEBE DOMAINS FOR THE CLASSES OF FUNCTIONS WITH RANGES INCLUDED IN GIVEN SETS

KOEBE DOMAINS FOR THE CLASSES OF FUNCTIONS WITH RANGES INCLUDED IN GIVEN SETS Jounal of Applied Analysis Vol. 14, No. 1 2008), pp. 43 52 KOEBE DOMAINS FOR THE CLASSES OF FUNCTIONS WITH RANGES INCLUDED IN GIVEN SETS L. KOCZAN and P. ZAPRAWA Received Mach 12, 2007 and, in evised fom,

More information

An Estimate of Incomplete Mixed Character Sums 1 2. Mei-Chu Chang 3. Dedicated to Endre Szemerédi for his 70th birthday.

An Estimate of Incomplete Mixed Character Sums 1 2. Mei-Chu Chang 3. Dedicated to Endre Szemerédi for his 70th birthday. An Estimate of Incomlete Mixed Chaacte Sums 2 Mei-Chu Chang 3 Dedicated to Ende Szemeédi fo his 70th bithday. 4 In this note we conside incomlete mixed chaacte sums ove a finite field F n of the fom x

More information

On the Quasi-inverse of a Non-square Matrix: An Infinite Solution

On the Quasi-inverse of a Non-square Matrix: An Infinite Solution Applied Mathematical Sciences, Vol 11, 2017, no 27, 1337-1351 HIKARI Ltd, wwwm-hikaicom https://doiog/1012988/ams20177273 On the Quasi-invese of a Non-squae Matix: An Infinite Solution Ruben D Codeo J

More information

Mean Curvature and Shape Operator of Slant Immersions in a Sasakian Space Form

Mean Curvature and Shape Operator of Slant Immersions in a Sasakian Space Form Mean Cuvatue and Shape Opeato of Slant Immesions in a Sasakian Space Fom Muck Main Tipathi, Jean-Sic Kim and Son-Be Kim Abstact Fo submanifolds, in a Sasakian space fom, which ae tangential to the stuctue

More information

Surveillance Points in High Dimensional Spaces

Surveillance Points in High Dimensional Spaces Société de Calcul Mathématique SA Tools fo decision help since 995 Suveillance Points in High Dimensional Spaces by Benad Beauzamy Januay 06 Abstact Let us conside any compute softwae, elying upon a lage

More information

Journal of Inequalities in Pure and Applied Mathematics

Journal of Inequalities in Pure and Applied Mathematics Jounal of Inequalities in Pue and Applied Mathematics COEFFICIENT INEQUALITY FOR A FUNCTION WHOSE DERIVATIVE HAS A POSITIVE REAL PART S. ABRAMOVICH, M. KLARIČIĆ BAKULA AND S. BANIĆ Depatment of Mathematics

More information

FORUM GEOMETRICORUM. A Journal on Classical Euclidean Geometry and Related Areas published by

FORUM GEOMETRICORUM. A Journal on Classical Euclidean Geometry and Related Areas published by FORUM GEOMETRICORUM A Journal on Classical Euclidean Geometry and Related Areas published by Department of Mathematical Sciences Florida Atlantic University FORUM GEOM Volume 10 2010 http://forumgeom.fau.edu

More information

On the integration of the equations of hydrodynamics

On the integration of the equations of hydrodynamics Uebe die Integation de hydodynamischen Gleichungen J f eine u angew Math 56 (859) -0 On the integation of the equations of hydodynamics (By A Clebsch at Calsuhe) Tanslated by D H Delphenich In a pevious

More information

PHYS 1114, Lecture 21, March 6 Contents:

PHYS 1114, Lecture 21, March 6 Contents: PHYS 1114, Lectue 21, Mach 6 Contents: 1 This class is o cially cancelled, being eplaced by the common exam Tuesday, Mach 7, 5:30 PM. A eview and Q&A session is scheduled instead duing class time. 2 Exam

More information

9.1 The multiplicative group of a finite field. Theorem 9.1. The multiplicative group F of a finite field is cyclic.

9.1 The multiplicative group of a finite field. Theorem 9.1. The multiplicative group F of a finite field is cyclic. Chapte 9 Pimitive Roots 9.1 The multiplicative goup of a finite fld Theoem 9.1. The multiplicative goup F of a finite fld is cyclic. Remak: In paticula, if p is a pime then (Z/p) is cyclic. In fact, this

More information

Measure Estimates of Nodal Sets of Polyharmonic Functions

Measure Estimates of Nodal Sets of Polyharmonic Functions Chin. Ann. Math. Se. B 39(5), 08, 97 93 DOI: 0.007/s40-08-004-6 Chinese Annals of Mathematics, Seies B c The Editoial Office of CAM and Spinge-Velag Belin Heidelbeg 08 Measue Estimates of Nodal Sets of

More information

Part V: Closed-form solutions to Loop Closure Equations

Part V: Closed-form solutions to Loop Closure Equations Pat V: Closed-fom solutions to Loop Closue Equations This section will eview the closed-fom solutions techniques fo loop closue equations. The following thee cases will be consideed. ) Two unknown angles

More information

Absorption Rate into a Small Sphere for a Diffusing Particle Confined in a Large Sphere

Absorption Rate into a Small Sphere for a Diffusing Particle Confined in a Large Sphere Applied Mathematics, 06, 7, 709-70 Published Online Apil 06 in SciRes. http://www.scip.og/jounal/am http://dx.doi.og/0.46/am.06.77065 Absoption Rate into a Small Sphee fo a Diffusing Paticle Confined in

More information

The Congestion of n-cube Layout on a Rectangular Grid S.L. Bezrukov J.D. Chavez y L.H. Harper z M. Rottger U.-P. Schroeder Abstract We consider the pr

The Congestion of n-cube Layout on a Rectangular Grid S.L. Bezrukov J.D. Chavez y L.H. Harper z M. Rottger U.-P. Schroeder Abstract We consider the pr The Congestion of n-cube Layout on a Rectangula Gid S.L. Bezukov J.D. Chavez y L.H. Hape z M. Rottge U.-P. Schoede Abstact We conside the poblem of embedding the n-dimensional cube into a ectangula gid

More information

of the contestants play as Falco, and 1 6

of the contestants play as Falco, and 1 6 JHMT 05 Algeba Test Solutions 4 Febuay 05. In a Supe Smash Bothes tounament, of the contestants play as Fox, 3 of the contestants play as Falco, and 6 of the contestants play as Peach. Given that thee

More information

Chapter Eight Notes N P U1C8S4-6

Chapter Eight Notes N P U1C8S4-6 Chapte Eight Notes N P UC8S-6 Name Peiod Section 8.: Tigonometic Identities An identit is, b definition, an equation that is alwas tue thoughout its domain. B tue thoughout its domain, that is to sa that

More information

Auchmuty High School Mathematics Department Advanced Higher Notes Teacher Version

Auchmuty High School Mathematics Department Advanced Higher Notes Teacher Version The Binomial Theoem Factoials Auchmuty High School Mathematics Depatment The calculations,, 6 etc. often appea in mathematics. They ae called factoials and have been given the notation n!. e.g. 6! 6!!!!!

More information

No. 48. R.E. Woodrow. Mathematics Contest of the British Columbia Colleges written March 8, Senior High School Mathematics Contest

No. 48. R.E. Woodrow. Mathematics Contest of the British Columbia Colleges written March 8, Senior High School Mathematics Contest 341 THE SKOLIAD CORNER No. 48 R.E. Woodow This issue we give the peliminay ound of the Senio High School Mathematics Contest of the Bitish Columbia Colleges witten Mach 8, 2000. My thanks go to Jim Totten,

More information

Quasi-Randomness and the Distribution of Copies of a Fixed Graph

Quasi-Randomness and the Distribution of Copies of a Fixed Graph Quasi-Randomness and the Distibution of Copies of a Fixed Gaph Asaf Shapia Abstact We show that if a gaph G has the popety that all subsets of vetices of size n/4 contain the coect numbe of tiangles one

More information

r cos, and y r sin with the origin of coordinate system located at

r cos, and y r sin with the origin of coordinate system located at Lectue 3-3 Kinematics of Rotation Duing ou peious lectues we hae consideed diffeent examples of motion in one and seeal dimensions. But in each case the moing object was consideed as a paticle-like object,

More information

3D-Central Force Problems I

3D-Central Force Problems I 5.73 Lectue #1 1-1 Roadmap 1. define adial momentum 3D-Cental Foce Poblems I Read: C-TDL, pages 643-660 fo next lectue. All -Body, 3-D poblems can be educed to * a -D angula pat that is exactly and univesally

More information

FORMULAE. 8. a 2 + b 2 + c 2 ab bc ca = 1 2 [(a b)2 + (b c) 2 + (c a) 2 ] 10. (a b) 3 = a 3 b 3 3ab (a b) = a 3 3a 2 b + 3ab 2 b 3

FORMULAE. 8. a 2 + b 2 + c 2 ab bc ca = 1 2 [(a b)2 + (b c) 2 + (c a) 2 ] 10. (a b) 3 = a 3 b 3 3ab (a b) = a 3 3a 2 b + 3ab 2 b 3 FORMULAE Algeba 1. (a + b) = a + b + ab = (a b) + 4ab. (a b) = a + b ab = (a + b) 4ab 3. a b = (a b) (a + b) 4. a + b = (a + b) ab = (a b) + ab 5. (a + b) + (a b) = (a + b ) 6. (a + b) (a b) = 4ab 7. (a

More information

Functions Defined on Fuzzy Real Numbers According to Zadeh s Extension

Functions Defined on Fuzzy Real Numbers According to Zadeh s Extension Intenational Mathematical Foum, 3, 2008, no. 16, 763-776 Functions Defined on Fuzzy Real Numbes Accoding to Zadeh s Extension Oma A. AbuAaqob, Nabil T. Shawagfeh and Oma A. AbuGhneim 1 Mathematics Depatment,

More information

Green s Identities and Green s Functions

Green s Identities and Green s Functions LECTURE 7 Geen s Identities and Geen s Functions Let us ecall The ivegence Theoem in n-dimensions Theoem 7 Let F : R n R n be a vecto field ove R n that is of class C on some closed, connected, simply

More information

ON INDEPENDENT SETS IN PURELY ATOMIC PROBABILITY SPACES WITH GEOMETRIC DISTRIBUTION. 1. Introduction. 1 r r. r k for every set E A, E \ {0},

ON INDEPENDENT SETS IN PURELY ATOMIC PROBABILITY SPACES WITH GEOMETRIC DISTRIBUTION. 1. Introduction. 1 r r. r k for every set E A, E \ {0}, ON INDEPENDENT SETS IN PURELY ATOMIC PROBABILITY SPACES WITH GEOMETRIC DISTRIBUTION E. J. IONASCU and A. A. STANCU Abstact. We ae inteested in constucting concete independent events in puely atomic pobability

More information

Polar Coordinates. a) (2; 30 ) b) (5; 120 ) c) (6; 270 ) d) (9; 330 ) e) (4; 45 )

Polar Coordinates. a) (2; 30 ) b) (5; 120 ) c) (6; 270 ) d) (9; 330 ) e) (4; 45 ) Pola Coodinates We now intoduce anothe method of labelling oints in a lane. We stat by xing a oint in the lane. It is called the ole. A standad choice fo the ole is the oigin (0; 0) fo the Catezian coodinate

More information

2 x 8 2 x 2 SKILLS Determine whether the given value is a solution of the. equation. (a) x 2 (b) x 4. (a) x 2 (b) x 4 (a) x 4 (b) x 8

2 x 8 2 x 2 SKILLS Determine whether the given value is a solution of the. equation. (a) x 2 (b) x 4. (a) x 2 (b) x 4 (a) x 4 (b) x 8 5 CHAPTER Fundamentals When solving equations that involve absolute values, we usually take cases. EXAMPLE An Absolute Value Equation Solve the equation 0 x 5 0 3. SOLUTION By the definition of absolute

More information

f h = u, h g = v, we have u + v = f g. So, we wish

f h = u, h g = v, we have u + v = f g. So, we wish Answes to Homewok 4, Math 4111 (1) Pove that the following examples fom class ae indeed metic spaces. You only need to veify the tiangle inequality. (a) Let C be the set of continuous functions fom [0,

More information

FREE Download Study Package from website: &

FREE Download Study Package from website:  & .. Linea Combinations: (a) (b) (c) (d) Given a finite set of vectos a b c,,,... then the vecto xa + yb + zc +... is called a linea combination of a, b, c,... fo any x, y, z... R. We have the following

More information

I. CONSTRUCTION OF THE GREEN S FUNCTION

I. CONSTRUCTION OF THE GREEN S FUNCTION I. CONSTRUCTION OF THE GREEN S FUNCTION The Helmohltz equation in 4 dimensions is 4 + k G 4 x, x = δ 4 x x. In this equation, G is the Geen s function and 4 efes to the dimensionality. In the vey end,

More information

6 PROBABILITY GENERATING FUNCTIONS

6 PROBABILITY GENERATING FUNCTIONS 6 PROBABILITY GENERATING FUNCTIONS Cetain deivations pesented in this couse have been somewhat heavy on algeba. Fo example, detemining the expectation of the Binomial distibution (page 5.1 tuned out to

More information

KEPLER S LAWS OF PLANETARY MOTION

KEPLER S LAWS OF PLANETARY MOTION EPER S AWS OF PANETARY MOTION 1. Intoduction We ae now in a position to apply what we have leaned about the coss poduct and vecto valued functions to deive eple s aws of planetay motion. These laws wee

More information

Geometry of the homogeneous and isotropic spaces

Geometry of the homogeneous and isotropic spaces Geomety of the homogeneous and isotopic spaces H. Sonoda Septembe 2000; last evised Octobe 2009 Abstact We summaize the aspects of the geomety of the homogeneous and isotopic spaces which ae most elevant

More information

Math 124B February 02, 2012

Math 124B February 02, 2012 Math 24B Febuay 02, 202 Vikto Gigoyan 8 Laplace s equation: popeties We have aleady encounteed Laplace s equation in the context of stationay heat conduction and wave phenomena. Recall that in two spatial

More information

EXTRA HOTS PROBLEMS. (5 marks) Given : t 3. = a + (n 1)d = 3p 2q + (n 1) (q p) t 10. = 3p 2q + (10 1) (q p) = 3p 2q + 9 (q p) = 3p 2q + 9q 9p = 7q 6p

EXTRA HOTS PROBLEMS. (5 marks) Given : t 3. = a + (n 1)d = 3p 2q + (n 1) (q p) t 10. = 3p 2q + (10 1) (q p) = 3p 2q + 9 (q p) = 3p 2q + 9q 9p = 7q 6p MT EDUCARE LTD. EXTRA HOTS PROBLEMS HOTS SUMS CHAPTER : - ARITHMETIC PROGRESSION AND GEOMETRIC PROGRESSION. If 3 d tem of an A.P. is p and the 4 th tem is q. Find its n th tem and hence find its 0 th tem.

More information

K.S.E.E.B., Malleshwaram, Bangalore SSLC Model Question Paper-1 (2015) Mathematics

K.S.E.E.B., Malleshwaram, Bangalore SSLC Model Question Paper-1 (2015) Mathematics K.S.E.E.B., Malleshwaam, Bangaloe SSLC Model Question Pape-1 (015) Mathematics Max Maks: 80 No. of Questions: 40 Time: Hous 45 minutes Code No. : 81E Fou altenatives ae given fo the each question. Choose

More information

ME 210 Applied Mathematics for Mechanical Engineers

ME 210 Applied Mathematics for Mechanical Engineers Tangent and Ac Length of a Cuve The tangent to a cuve C at a point A on it is defined as the limiting position of the staight line L though A and B, as B appoaches A along the cuve as illustated in the

More information

MAC Module 12 Eigenvalues and Eigenvectors

MAC Module 12 Eigenvalues and Eigenvectors MAC 23 Module 2 Eigenvalues and Eigenvectos Leaning Objectives Upon completing this module, you should be able to:. Solve the eigenvalue poblem by finding the eigenvalues and the coesponding eigenvectos

More information

Math Section 4.2 Radians, Arc Length, and Area of a Sector

Math Section 4.2 Radians, Arc Length, and Area of a Sector Math 1330 - Section 4. Radians, Ac Length, and Aea of a Secto The wod tigonomety comes fom two Geek oots, tigonon, meaning having thee sides, and mete, meaning measue. We have aleady defined the six basic

More information

Chapter 2: Basic Physics and Math Supplements

Chapter 2: Basic Physics and Math Supplements Chapte 2: Basic Physics and Math Supplements Decembe 1, 215 1 Supplement 2.1: Centipetal Acceleation This supplement expands on a topic addessed on page 19 of the textbook. Ou task hee is to calculate

More information

$ i. !((( dv vol. Physics 8.02 Quiz One Equations Fall q 1 q 2 r 2 C = 2 C! V 2 = Q 2 2C F = 4!" or. r ˆ = points from source q to observer

$ i. !((( dv vol. Physics 8.02 Quiz One Equations Fall q 1 q 2 r 2 C = 2 C! V 2 = Q 2 2C F = 4! or. r ˆ = points from source q to observer Physics 8.0 Quiz One Equations Fall 006 F = 1 4" o q 1 q = q q ˆ 3 4" o = E 4" o ˆ = points fom souce q to obseve 1 dq E = # ˆ 4" 0 V "## E "d A = Q inside closed suface o d A points fom inside to V =

More information

arxiv: v1 [math.co] 6 Mar 2008

arxiv: v1 [math.co] 6 Mar 2008 An uppe bound fo the numbe of pefect matchings in gaphs Shmuel Fiedland axiv:0803.0864v [math.co] 6 Ma 2008 Depatment of Mathematics, Statistics, and Compute Science, Univesity of Illinois at Chicago Chicago,

More information

Relating Branching Program Size and. Formula Size over the Full Binary Basis. FB Informatik, LS II, Univ. Dortmund, Dortmund, Germany

Relating Branching Program Size and. Formula Size over the Full Binary Basis. FB Informatik, LS II, Univ. Dortmund, Dortmund, Germany Relating Banching Pogam Size and omula Size ove the ull Binay Basis Matin Saueho y Ingo Wegene y Ralph Wechne z y B Infomatik, LS II, Univ. Dotmund, 44 Dotmund, Gemany z ankfut, Gemany sauehof/wegene@ls.cs.uni-dotmund.de

More information

Math 2263 Solutions for Spring 2003 Final Exam

Math 2263 Solutions for Spring 2003 Final Exam Math 6 Solutions fo Sping Final Exam ) A staightfowad appoach to finding the tangent plane to a suface at a point ( x, y, z ) would be to expess the cuve as an explicit function z = f ( x, y ), calculate

More information

Duality between Statical and Kinematical Engineering Systems

Duality between Statical and Kinematical Engineering Systems Pape 00, Civil-Comp Ltd., Stiling, Scotland Poceedings of the Sixth Intenational Confeence on Computational Stuctues Technology, B.H.V. Topping and Z. Bittna (Editos), Civil-Comp Pess, Stiling, Scotland.

More information

11.2. Area of a Circle. Lesson Objective. Derive the formula for the area of a circle.

11.2. Area of a Circle. Lesson Objective. Derive the formula for the area of a circle. 11.2 Aea of a Cicle Lesson Objective Use fomulas to calculate the aeas of cicles, semicicles, and quadants. Lean Deive the fomula fo the aea of a cicle. A diamete divides a cicle of adius into 2 semicicles.

More information

Semicanonical basis generators of the cluster algebra of type A (1)

Semicanonical basis generators of the cluster algebra of type A (1) Semicanonical basis geneatos of the cluste algeba of type A (1 1 Andei Zelevinsky Depatment of Mathematics Notheasten Univesity, Boston, USA andei@neu.edu Submitted: Jul 7, 006; Accepted: Dec 3, 006; Published:

More information

Vanishing lines in generalized Adams spectral sequences are generic

Vanishing lines in generalized Adams spectral sequences are generic ISSN 364-0380 (on line) 465-3060 (pinted) 55 Geomety & Topology Volume 3 (999) 55 65 Published: 2 July 999 G G G G T T T G T T T G T G T GG TT G G G G GG T T T TT Vanishing lines in genealized Adams spectal

More information

Title. Author(s)Y. IMAI; T. TSUJII; S. MOROOKA; K. NOMURA. Issue Date Doc URL. Type. Note. File Information

Title. Author(s)Y. IMAI; T. TSUJII; S. MOROOKA; K. NOMURA. Issue Date Doc URL. Type. Note. File Information Title CALCULATION FORULAS OF DESIGN BENDING OENTS ON TH APPLICATION OF THE SAFETY-ARGIN FRO RC STANDARD TO Autho(s)Y. IAI; T. TSUJII; S. OROOKA; K. NOURA Issue Date 013-09-1 Doc URL http://hdl.handle.net/115/538

More information

Fall 2014 Randomized Algorithms Oct 8, Lecture 3

Fall 2014 Randomized Algorithms Oct 8, Lecture 3 Fall 204 Randomized Algoithms Oct 8, 204 Lectue 3 Pof. Fiedich Eisenband Scibes: Floian Tamè In this lectue we will be concened with linea pogamming, in paticula Clakson s Las Vegas algoithm []. The main

More information

1.6. Trigonometric Functions. 48 Chapter 1: Preliminaries. Radian Measure

1.6. Trigonometric Functions. 48 Chapter 1: Preliminaries. Radian Measure 48 Chapte : Peliminaies.6 Tigonometic Functions Cicle B' B θ C A Unit of cicle adius FIGURE.63 The adian measue of angle ACB is the length u of ac AB on the unit cicle centeed at C. The value of u can

More information