Hyperbola Notes for IIT JEE, Download PDF!!!

Total Page:16

File Type:pdf, Size:1020Kb

Hyperbola Notes for IIT JEE, Download PDF!!! www.gradeup.co One of the most important topics from JEE point of view is the conic section. Further ellipse and hyperbola constitute of 2-3 questions every year. Read and revise all the important topics from ellipse and hyperbola. Download the pdf of the Short Notes on Ellipse and Hyperbola from the link given at the end of the article. 1.Basic of conic sections Conic Section is the locus of a point which moves such that the ratio of its distance from a fixed point to its perpendicular distance from a fixed line is always constant. The focus is the fixed point, directrix is the fixed straight line, eccentricity is the constant ratio and axis is the line passing through the focus and perpendicular to the directrix. The point of intersection with axis is called vertex of the conic. 1.1 General Equation of the conic PS2 = e2 PM2 Simplifying above, we will get ax2 + 2hxy + by2 + 2gx + 2fy + c = 0, this is the general equation of the conic. 1.2 Nature of the conic The nature of the conic depends on eccentricity and also on the relative position of the fixed point and the fixed line. Discriminant ‘Δ’ of a second-degree equation is defined as: www.gradeup.co Nature of the conic depends on Case 1: When the fixed point ‘S’ lies on the fixed line i.e., on directrix. Then the discriminant will be 0. Then the general equation of the conic will represent two lines Case 2: When the fixed point ‘S’ does not lies on the fixed line i.e., not on directrix. Then the discriminant will not be 0. Then the general equation of the conic will represent parabola, ellipse, and hyperbola. (a) Parabola: When eccentricity is 1; h2 = ab (b) Ellipse: When eccentricity is <1; h2 <ab (c) Hyperbola: When eccentricity is >1; h2 > ab When a+ b = 0 then it becomes rectangular hyperbola. 2. Hyperbola Hyperbola is the locus of a point in a plane such that the difference of its distance from two fixed point in the same plane is always constant. Here, e> 1 and h2 >ab Let P (h, k) Thus, according to the definition, equation would be |PF1 | - |PF2| = 2a Solving this condition will give the equation of hyperbola as: , where b2 = a2 (e2 – 1) www.gradeup.co 2.1 Nomenclature of hyperbola: Eccentricity (e): Foci: (c,0) and (-c,0) or (ae, 0) and (-ae,0) Transverse axis (TA): The line segment containing the foci is known as the transverse axis and the length is 2a Conjugate axis (CA): The line segment containing the points B1 and B2 is called as conjugate axis and the length is 2b. Centre of the hyperbola: Point of the intersection of TA and CA is known as the center. Both TA and CA together known as the principle axes of the hyperbola. Vertices: A1 (a,0) and A2 (-a,0) Focal axis: Line containing the fix points F1 and F2 (called as foci) is called as the focal axis Focal length: The distance between F1 and F2 is called the focal length Focal chord: A chord passing through a focus is called the focal chord. Latus rectum (LR): LR is the focal chord which is perpendicular to TA and whose length is 2b2/a = 2a(e2 – 1)= 2e ( ae – a/e) = 2e (Distance between focus and corresponding foot of directrix) Double ordinate: A chord which is perpendicular to the transverse axis. Directrix: x = ±a/e 2.3 Conjugate Hyperbola Corresponding to every hyperbola there exist a hyperbola such that the conjugate axis and the transverse axis of one is equal to the transverse axis and the conjugate axis of the other. Such hyperbolas are called as the conjugate hyperbola If, hyperbola, H: Then conjugate hyperbola, CH: If e1 is the eccentricity of the hyperbola and e2 is the eccentricity of the conjugate hyperbola then www.gradeup.co 2 2 , whereas e1 = 1 + and e1 = 1 + 2.4 Rectangular Hyperbola A hyperbola will be converted to a rectangular hyperbola if a = b i.e., TA = CA. This hyperbola is also known as an equilateral hyperbola. Eccentricity, e =√2 Length of latus rectum= 2a = CA = TA 2.5 Auxiliary Circle and Eccentric angle The circle described on the transverse axis of the hyperbola as the diameter is called an auxiliary circle. Thus, it’s equation would be x2 + y2 = a2 And for conjugate hyperbola, the equation would be x2 + y2 = b2 2.6 Parametric coordinates of a point on the hyperbola P (a sec θ, b tan θ) From point P, a perpendicular line is drawn to meet the TA at (let’s say). From T a tangent is drawn on the auxiliary circle, meeting the circle at Q. These two points: P and Q are called as the corresponding point and Q is called as the eccentric angle of the point P. www.gradeup.co 2.7 Position of a point with respect to the hyperbola Point P lies outside the hyperbola, S1 < 0 : Point is outside the curve S1 > 0: Point is inside the curve S1 = 0: Point is on the curve 2.8 Line and Parabola Let, L: y = mx + c S: A line can be a tangent to the hyperbola, it may cut the hyperbola or it may not cut/touch the hyperbla at all. To find that, we will make a quadratic in ‘x’ using equations of L and S. If discriminant D> 0 ⇒ Two roots ⇒ Intersect ⇒ Secant If D= 0 ⇒ One root ⇒ Touching the ellipse⇒ Tangent If D< 0 ⇒ No roots ⇒ Neither secant nor tangent 2.9 Condition of Tangency D = 0 ⇒ Thus the equation of the tangent would be L: y = mx + c www.gradeup.co 2.10 Number of tangents from a given point (h,k) to the hyperbola We have, P (h,k) Thus, (k – mh)2 =a2m2 - b2 which is a quadratic in m. This suggests that from a given point P(h,k) we can draw at maximum two tangents. 2.11 Angle between the two tangents Let the angle between the tangents be θ From above quadratic equation we know slope: m1 and m2 Thus, From the quadratic equation in m, 2.12 Director circle of the ellipse When θ = 90° then m1m2 = -1 x2 + y2 = a2 - b2 : Equation of director circle. Now, director circle can be imaginary or real. Real director circle: when the length of TA > length of CA Imaginary director circle: when the length of TA < length of CA Point circle: when the length of TA = length of CA ie., in case of a rectangular hyperbola. Thus, director circle is the locus of all those point from where the ellipse can be seen at angle 90. www.gradeup.co 2.13 Equation of the chord of a hyperbola joining α and β on it 2.14 Equation of Tangent, Normal and Chord of Contact Tangents: a) Cartesian Tangent b) Slope form Parametric form Normal: a) Cartesian Normal b) Slope form www.gradeup.co c) Parametric form 2.15 Chord of contact: The equation of chord of contact will be similar to that of the tangent. Thus a line when touches the hyperbola will be tangent and the same line when cuts the hyperbola will be the chord of contact. Equation: T = 0 (Similar to that of tangent equation) 2.16 Pair of tangents: The equation of pair of tangents would be 2 SS1 = T , where S is the equation of the hyperbola, S1 is the equation when a point P (h,k) satisfies S, T is the equation of the tangent. 2.17 Equation of the chord whose middle point is (x1, y1): T = S1 2.18 Rectangular Hyperbola This is a special kind of hyperbola when the length of traverse and conjugate axis are equal. The equation is x2 – y2 = a2 However, rotating the coordinate axis through an angle of 450, we get an another form of this rectangular hyperbola. i.e., XY = c2 2.19 Parametric coordinates of (RH) (ct, c/t ) where t≠ 0 and t ∈ R Two points on this hyperbola can be represented by (ct1,c/t1) and (ct2, c/t2) 2.20 The equation of chord joining t1 and t2 points on the rectangular hyperbola Two points on this hyperbola can be represented by (ct1,) and (ct2,) Slope of the line joining t1 and t2 : Thus, the equation of chord: www.gradeup.co x + t1t2 y = c (t1 + t2) 2.21 Equation of tangent of the rectangular hyperbola a)Cartesian form at the point (x1,y1) b) Parametric form 2.22 The equation of normal of the rectangular hyperbola Parametric form: (y -c/t) = t2 (x – ct) Equation of a chord whose middle point is (h, k) T = S1 Thus, equation is Subscribe to YouTube Channel for JEE Main All the best! Team Gradeup All About JEE Main Examination: https://gradeup.co/engineering-entrance-exams/jee-main Download Gradeup, the best IIT JEE Preparation App www.gradeup.co .
Recommended publications
  • Automated Study of Isoptic Curves: a New Approach with Geogebra∗
    Automated study of isoptic curves: a new approach with GeoGebra∗ Thierry Dana-Picard1 and Zoltan Kov´acs2 1 Jerusalem College of Technology, Israel [email protected] 2 Private University College of Education of the Diocese of Linz, Austria [email protected] March 7, 2018 Let C be a plane curve. For a given angle θ such that 0 ≤ θ ≤ 180◦, a θ-isoptic curve of C is the geometric locus of points in the plane through which pass a pair of tangents making an angle of θ.If θ = 90◦, the isoptic curve is called the orthoptic curve of C. For example, the orthoptic curves of conic sections are respectively the directrix of a parabola, the director circle of an ellipse, and the director circle of a hyperbola (in this case, its existence depends on the eccentricity of the hyperbola). Orthoptics and θ-isoptics can be studied for other curves than conics, in particular for closed smooth strictly convex curves,as in [1]. An example of the study of isoptics of a non-convex non-smooth curve, namely the isoptics of an astroid are studied in [2] and of Fermat curves in [3]. The Isoptics of an astroid present special properties: • There exist points through which pass 3 tangents to C, and two of them are perpendicular. • The isoptic curve are actually union of disjoint arcs. In Figure 1, the loops correspond to θ = 120◦ and the arcs connecting them correspond to θ = 60◦. Such a situation has been encountered already for isoptics of hyperbolas. These works combine geometrical experimentation with a Dynamical Geometry System (DGS) GeoGebra and algebraic computations with a Computer Algebra System (CAS).
    [Show full text]
  • HYPERBOLA HYPERBOLA a Conic Is Said to Be a Hyperbola If Its Eccentricity Is Greater Than One
    HYPERBOLA HYPERBOLA A Conic is said to be a hyperbola if its eccentricity is greater than one. If S ax22 hxy by 2 2 gx 2 fy c 0 represents a hyperbola then h2 ab 0 and 0 2 2 If S ax2 hxy by 2 gx 2 fy c 0 represents a rectangular hyperbola then h2 ab 0 , 0 and a b 0 x2 y 2 Hyperbola: Equation of the hyperbola in standard form is 1. a2 b2 Hyperbola is symmetric about both the axes. Hyperbola does not passing through the origin and does not meet the Y - axis. Hyperbola curve does not exist between the lines x a and x a . x2 y 2 xx yy x2 y 2 x x y y Notation: S 1 , S1 1 1, S1 1 1, S1 2 1 2 1. a2 b 2 1 a2 b 2 11 a2 b 2 12 a2 b 2 Rectangular hyperbola (or) Equilateral hyperbola : In a hyperbola if the length of the transverse axis (2a) is equal to the length of the conjugate axis (2b) , then the hyperbola is called a rectangular hyperbola or an equilateral hyperbola. The eccentricity of a rectangular hyperbola is 2 . Conjugate hyperbola : The hyperbola whose transverse and conjugate axes are respectively the conjugate and transverse axes of a given hyperbola is called the conjugate hyperbola of the given hyperbola. 2 2 1 x y The equation of the hyperbola conjugate to S 0 is S 1 0 . a2 b 2 If e1 and e2 be the eccentricities of the hyperbola and its conjugate hyperbola then 1 1 2 2 1.
    [Show full text]
  • Department of Mathematics Scheme of Studies B.Sc
    BHUPAL NOBLES` UNIVERSITY, UDAIPUR FACULTY OF SCIENCE Department Of Mathematics Scheme of Studies B.Sc. I Year (Annual Scheme) S. No. PAPER NOMENCLATURE COURSE UNIVERSITY INTERNAL MAX. CODE EXAM ASSESSMENT MARKS 1. Paper I Algebra MAT-111 53 22 75 2. Paper II Calculus MAT- 112 53 22 75 3. Paper III Geometry MAT- 113 53 22 75 The marks distribution of internal assessment- 1. Mid Term Examination – 15 marks 2. Attendance – 7 marks B.Sc. II Year (Annual Scheme) S. No. PAPER NOMENCLATURE COURSE UNIVERSITY INTERNAL MAX. CODE EXAM ASSESSMENT MARKS 1. Paper I Advanced Calculus MAT-221 53 22 75 2. Paper II Differential Equation MAT- 222 53 22 75 3. Paper III Mechanics MAT- 223 53 22 75 The marks distribution of internal assessment- 1. Mid Term Examination – 15 marks 2. Attendance – 7 marks B.Sc. III Year (Annual Scheme) S. PAPER NOMENCLATURE COURSE CODE UNIVERSITY INTERNAL MAX. No. EXAM ASSESSMENT MARKS 1. Paper I Real Analysis MAT-331 53 22 75 2. Paper II Advanced Algebra MAT- 332 53 22 75 3. Paper Numerical Analysis MAT-333 (A) 53 22 75 III Mathematical MAT-333 (B) Quantitative Techniques Mathematical MAT-333 (C) Statistics The marks distribution of internal assessment- 1. Mid Term Examination – 15 marks 2. Attendance – 7 marks BHUPAL NOBLES’ UNIVERSITY, UDAIPUR Department of Mathematics Syllabus 2017 -2018 (COMMON FOR THE FACULTIES OF ARTS & SCIENCE) B.A. / B. Sc. FIRST YEAR EXAMINATIONS 2017-2020 MATHEMATICS Theory Papers Name Papers Code Papers Maximum Papers hours/ Marks BA/ week B.Sc. Paper I ALGEBRA MAT-111 3 75 Paper II CALCULUS MAT-112 3 75 Paper III GEOMETRY MAT-113 3 75 Total Marks 225 NOTE: 1.
    [Show full text]
  • Syllabus for Bachelor of Science I-Year (Semester-I) Session 2018
    Syllabus for Bachelor of Science I-Year (Semester-I) Session 2018-2019 Code Description Pd/W Exam CIA ESE Total BSMT111 Algebra 3 3 hrs 20 80 100 BSMT112 Differential Calculus 3 3 hrs 20 80 100 BSMT113 Co-ordinate Geometry of Two and 3 3 hrs 20 80 100 Three Dimensions Total 60 240 300 BSMT111: ALGEBRA Matrix: The characteristic equation of matrix: Eigen Values and Eigen Unit-I Vectors, Diagonalization of matrix, Cayley-Hamilton theorem(Statement 9 and proof),and its use in finding the inverse of a Matrix. Theory of equation: Relation between roots and coefficient of the equation Unit-II Symmetric function of roots. Solution of cubic equation by Cordon’s 9 method and Biquadratic equitation by Ferrari’s method. Infinite series: Convergent series, convergence of geometric series, And Unit-III necessary condition for the convergent series, comparison tests: Cauchy 9 root test. D’Alembert’s Ratio test, Logarithmic test, Raabe’s test, De’ Morgan and Unit-IV Bertrand’s test, Cauchy’s condensation test, Leibnitz’s test of alternative 9 series, Absolute convergent. Unit-V Inequalities and Continued fractions. 9 Suggested Readings: 1. Bhargav and Agarwal:Algebra, Jaipur publishing House, Jaipur. 2. Vashistha and Vashistha : Modern Algebra, Krishna Prakashan, Meerut. 3. Gokhroo, Saini and Tak: Algebra,Navkar prakashan, Ajmer.. 4. M-Ray and H. S. Sharma: A Text book of Higher Algebra, New Delhi, BSMT112: Differential Calculus Unit-I Polar Co-ordinates, Angle between radius vector and the tangents. Angle 9 between curves in polar form, length of polar subs tangent and subnormal, pedal equation of a curve, derivatives of an arc.
    [Show full text]
  • Group B Higher Algebra & Trigonometry
    UNIVERSITY DEPARTMENT OF MATHEMATICS, DSPMU, RANCHI CBCS PATTERN SYLLABUS Semester Mat/ Sem VC1- Analytical Geometry 2D, Trigonometry Instruction: Ten questions will be set. Candidates will be required to answer Seven Questions. Question no. 1 will be Compulsory consisting of 10 short answer type covering entire syllabus uniformly. Each question will be of 2 marks. Out of remaining 9 questions candidates will be required to answer 6 questions selecting at least one from each group. Each question will be of 10 marks. GROUP-A ANALYTICAL GEOMETRY OF TWO DIMENSIONS Change of rectangular axes. Condition for the general equation of second degree to represent parabola, ellipse, hyperbola and reduction into standard forms. Equations of tangent and normal (Using Calculus). Chord of contact, Pole and Polar. Pair of tangents in reference to general equation of conic. Axes, centre, director circle in reference to general equation of conic. Polar equation of conic. 5 Questions GROUP B HIGHER ALGEBRA & TRIGONOMETRY Statement and proof of binomial theorem for any index, exponential and logarithmic series. 1 Question De Moivre's theorem and its applications. Trigonometric and Exponential functions of complex argument and hyperbolic functions. Summation of Trigonometrical series. Factorisation of sin , cos 3 Questions Books Recommended: 1. Analytical Geometry& Vector Analysis - B. K. Kar, Books& Allied Co., Kolkata 2. Analytical Geometry of two dimension - Askwith 3. Coordinate Geometry- SL Loney. 4. Trigonometry- Das and Mukheriee 5. Trigonometry- Dasgupta UNIVERSITY DEPARTMENT OF MATHEMATICS, DSPMU, RANCHI CBCS PATTERN SYLLABUS Semester Mat/ Sem IVC 2- Differential Calculus and Vector Calculus Instruction: Ten questions will be set. Candidates will be required to answer Seven Questions.
    [Show full text]
  • 1 CHAPTER 2 CONIC SECTIONS 2.1 Introduction a Particle Moving Under the Influence of an Inverse Square Force Moves in an Orbit T
    1 CHAPTER 2 CONIC SECTIONS 2.1 Introduction A particle moving under the influence of an inverse square force moves in an orbit that is a conic section; that is to say an ellipse, a parabola or a hyperbola. We shall prove this from dynamical principles in a later chapter. In this chapter we review the geometry of the conic sections. We start off, however, with a brief review (eight equation-packed pages) of the geometry of the straight line. 2.2 The Straight Line It might be thought that there is rather a limited amount that could be written about the geometry of a straight line. We can manage a few equations here, however, (there are 35 in this section on the Straight Line) and shall return for more on the subject in Chapter 4. Most readers will be familiar with the equation y = mx + c 2.2.1 for a straight line. The slope (or gradient) of the line, which is the tangent of the angle that it makes with the x-axis, is m, and the intercept on the y-axis is c. There are various other forms that may be of use, such as x y +=1 2.2.2 x00y yy− 1 yy21− = 2.2.3 xx− 1 xx21− which can also be written x y 1 x1 y1 1 = 0 2.2.4 x2 y2 1 x cos θ + y sin θ = p 2.2.5 2 The four forms are illustrated in figure II.1. y y slope = m y 0 c x x x0 2.2.1 2.2.2 y y • (x2 , y2 ) • ( x1 , y1 ) p x α x 2.2.3 or 4 2.2.5 FIGURE II.1 A straight line can also be written in the form Ax + By + C = 0.
    [Show full text]
  • Geometrical Constructions 1) (See Geometrical Constructions 1)
    GEOMETRICAL CONSTRUCTIONS 2 by Johanna PÉK PhD Budapest University of Technology and Economics Faculty of Architecture Department of Architectural Geometry and Informatics Table of contents • Radical line, radical center. Apollonius’ problem • Conic sections • Basic constructions on ellipses • Basic constructions on parabolas. Basic constructions on hyperbolas • Approximate constructions. Constructions of algebraic operations • Metric problems in space • Polyhedra. Regular polyhedra • Cone, cylinder, sphere • Multi-view representation • Axonometrical representation 2 Power of a point Power of a point (or circle power) The power of a point P with respect to a circle is defined by the product PA ∙ PB where AB is a secant passing through P. Remark: The point P can be an inner point of the circle. 2 Theorem: Using the notation of the figure, PA ∙ PB = PK ∙ PL = PT Sketch of the proof 3 RADICAL LINE, RADICAL CENTER – 1 Radical line (of two circles) is the locus of points of equal (circle) power with respect to two nonconcentric circles. This line is perpendicular to the line of centers. If two circles have common points K, L then their radical line is line KL. Alternative definition: radical line is the locus of points at which tangents drawn to both circles have the same length. (See point P.) lecture & practical 4 Radical line, radical center – 2 Radical center (of three circles): The radical lines of three circles intersect each other in a special pont called the radical center (or power center). lecture & practical 5 Radical line, radical center – 3 The radical line exists even if the two circles have no common points.
    [Show full text]
  • An Introduction to Convex and Discrete Geometry Lecture Notes
    An introduction to convex and discrete geometry Lecture Notes Tomasz Tkocz∗ These lecture notes were prepared and written for the undergraduate topics course 21-366 An introduction to convex and discrete geometry that I taught at Carnegie Mellon University in Fall 2019. ∗Carnegie Mellon University; [email protected] 1 Contents 1 Introduction 5 1.1 Euclidean space . .5 1.2 Linear and affine hulls . .7 1.3 Exercises . 10 2 Basic convexity 12 2.1 Convex hulls . 12 2.2 Carath´eodory's theorem . 14 2.3 Exercises . 16 3 Separation 17 3.1 Supporting hyperplanes . 17 3.2 Separation theorems . 21 3.3 Application in linear optimisation { Farkas' lemma . 24 3.4 Exercises . 25 4 Further aspects of convexity 26 4.1 Extreme points and Minkowski's theorem . 26 4.2 Extreme points of polytopes . 27 4.3 Exercises . 29 5 Polytopes I 30 5.1 Duality . 31 5.2 Bounded polyhedra are polytopes . 36 5.3 Exercises . 38 6 Polytopes II 39 6.1 Faces . 39 6.2 Cyclic polytopes have many faces . 40 6.3 Exercises . 45 7 Combinatorial convexity 46 7.1 Radon's theorem . 46 7.2 Helly's theorem . 47 7.3 Centrepoint . 49 7.4 Exercises . 51 8 Arrangements and incidences 52 8.1 Arrangements . 52 8.2 Incidences . 54 2 8.3 The crossing number of a graph . 56 8.4 Proof of the Szemer´edi-Trotter theorem . 58 8.5 Application in additive combinatorics . 59 8.6 Exercises . 61 9 Volume 62 9.1 The Brunn-Minkowski inequality . 62 9.2 Isoperimetric and isodiametric inequality .
    [Show full text]
  • 1 CHAPTER 2 CONIC SECTIONS 2.1 Introduction a Particle Moving
    1 CHAPTER 2 CONIC SECTIONS 2.1 Introduction A particle moving under the influence of an inverse square force moves in an orbit that is a conic section; that is to say an ellipse, a parabola or a hyperbola. We shall prove this from dynamical principles in a later chapter. In this chapter we review the geometry of the conic sections. We start off, however, with a brief review (eight equation-packed pages) of the geometry of the straight line. 2.2 The Straight Line It might be thought that there is rather a limited amount that could be written about the geometry of a straight line. We can manage a few equations here, however, (there are 35 in this section on the Straight Line) and we shall return for more on the subject in Chapter 4. Most readers will be familiar with the equation y = mx + c 2.2.1 for a straight line. The slope (or gradient) of the line, which is the tangent of the angle that it makes with the x-axis, is m, and the intercept on the y-axis is c. There are various other forms that may be of use, such as x y 1 2.2.2 x0 y0 y y y y 1 2 1 2.2.3 x x1 x2 x1 which can also be written x y 1 x1 y1 1 = 0 2.2.4 x2 y2 1 x cos + y sin = p 2.2.5 2 The four forms are illustrated in figure II.1. y y slope = m y0 c x x x0 2.2.1 2.2.2 y y (x2 , y2 ) ( x1 , y1 ) p x x 2.2.3 or 4 2.2.5 FIGURE II.1 A straight line can also be written in the form Ax + By + C = 0.
    [Show full text]
  • Director Circle of a Conic Inscribed in a Triangle Author(S): E. P. Rouse Source: the Mathematical Gazette, No
    Director Circle of a Conic Inscribed in a Triangle Author(s): E. P. Rouse Source: The Mathematical Gazette, No. 2 (Jul., 1894), pp. 12-13 Published by: Mathematical Association Stable URL: http://www.jstor.org/stable/3602373 Accessed: 26-11-2015 04:44 UTC Your use of the JSTOR archive indicates your acceptance of the Terms & Conditions of Use, available at http://www.jstor.org/page/ info/about/policies/terms.jsp JSTOR is a not-for-profit service that helps scholars, researchers, and students discover, use, and build upon a wide range of content in a trusted digital archive. We use information technology and tools to increase productivity and facilitate new forms of scholarship. For more information about JSTOR, please contact [email protected]. Mathematical Association is collaborating with JSTOR to digitize, preserve and extend access to The Mathematical Gazette. http://www.jstor.org This content downloaded from 139.184.14.159 on Thu, 26 Nov 2015 04:44:41 UTC All use subject to JSTOR Terms and Conditions 12 12 1THE MilAT'HEIMATICAL GAZETTE then known, and constructed to indicate tlese correctly above referred to: " Of him it may truly be said that for 17,100 years. It lasted, in fact, but a very few he studied more to serve the public than himself, and years. During the troubles of the civil war it was though he was rich in fame and in the promises of cast away as old rubbish, and in 1646 was found by the great, yet he died poor, to the scandal of an Sir Jonas Moore, and deposited in its dilapidated state ungrateful age." G.
    [Show full text]
  • 24Th Conference on Applications of Computer Algebra
    SPECIAL SESIONS Applications of Computer Algebra - ACA2018 Santiago de Compostela 2018 24th Conference on Applications of Computer Algebra June 18–22, 2018 Santiago de Compostela, Spain S8 Dynamic Geometry and Mathematics Education Wednesday Wed 20th, 10:00 - 10:30, Aula 10 − Thierry Dana-Picard: A new approach to automated study of isoptic curves Wed 20th, 10:30 - 11:00, Aula 10 − Roman Hašek: Exploration of dual curves using dynamic geometry and computer algebra system Wed 20th, 11:30 - 12:00, Aula 10 − Setsuo Takato: Programming in KeTCindy with Combined Use of Cinderella and Maxima Wed 20th, 12:00 - 12:30, Aula 10 − Raúl M. Falcón: Discovering properties of bar linkage mechanisms based on partial Latin squares by means of Dynamic Geometry Systems Wed 20th, 12:30 - 13:00, Aula 10 − Philippe R. Richard: Issues and challenges about instrumental proof Wed 20th, 13:00 - 13:30, Aula 10 − Round table: Dynamic Geometry and Computer Algebra Systems in Mathematics instruction 2 Organizers Tomás Recio Universidad de Cantabria Santander, Spain Philippe R. Richard Université de Montréal Montréal, Canada M. Pilar Vélez Universidad Antonio de Nebrija Madrid, Spain Aim and cope Dynamic geometry environments (DGE) have emerged in the last half-century with an ever-increasing impact in mathematics education. DGE enlarges the field of ge- ometric objects subject to formal reasoning, for instance, simultaneous operations with many geometric objects. Today DGE open the possibility of investigating vi- sually and formulating conjectures, comparing objects, discovering or proving rigor- ously properties over geometric constructions, and Euclidean elementary geometry is required to reason about them. Along these decades various utilities have been added to these environments, such as the manipulation of algebraic equations of geometric objects or the auto- mated proving and discovering, based on computer algebra algorithms, of elemen- tary geometry statements.
    [Show full text]
  • Contributions to the Theory of Surfaces in a 4-Space of Constant Curvature
    CONTRIBUTIONS TO THE THEORY OF SURFACES IN A 4-SPACE OF CONSTANT CURVATURE BY YUNG-CHOWWONG?) 1.1. Introduction. A Riemannian 4-space is a space of constant curvature and is denoted by 54, if its Riemann tensor is of the form R.\u = — C(aK\öß — atßo\) (p, k, X, u = 1, • • • , 4), where a,\ is the fundamental tensor, ô* the Kronecker delta and C a scalar, which is automatically a constant. A Euclidean 4-space, which we denote by Ri, is a special case of 54. In this paper we study a few special surfaces Vi in an 54, including those in an P4. The method used is invariant and is similar to those of Ricci (2) [14] and Graustein [9] for their studies of surfaces in a Euclidean 3-space. In essence, we first set up a suitable system of in- variant fundamental equations for a Vi in 54 and then express the imbedding requirements of F2 in 54 in terms of the intrinsic properties of Vt. §1.2 con- tains some formulas in the intrinsic theory of Vt which are useful for our later work. In §2, the curvature tensor H¿¿' and the curvature conic (G) for a Vt in 54 are introduced and discussed. Regarding Ha' as a pencil of tensors, we find a certain relationship between the nature of the pencil and that of the conic (G). Some formulas concerning (G) are then given, including one which leads to an interesting interpretation of the Gaussian curvature of Vt in terms of (G). §3 contains the fundamental equations for Vt in 54 in invariant form and an outline of the method used for the study of some sur- faces with preassigned curvature properties.
    [Show full text]