Geometry in Fourth Grade, As Explained in the Chart That Follows
Total Page:16
File Type:pdf, Size:1020Kb
Load more
Recommended publications
-
Models of 2-Dimensional Hyperbolic Space and Relations Among Them; Hyperbolic Length, Lines, and Distances
Models of 2-dimensional hyperbolic space and relations among them; Hyperbolic length, lines, and distances Cheng Ka Long, Hui Kam Tong 1155109623, 1155109049 Course Teacher: Prof. Yi-Jen LEE Department of Mathematics, The Chinese University of Hong Kong MATH4900E Presentation 2, 5th October 2020 Outline Upper half-plane Model (Cheng) A Model for the Hyperbolic Plane The Riemann Sphere C Poincar´eDisc Model D (Hui) Basic properties of Poincar´eDisc Model Relation between D and other models Length and distance in the upper half-plane model (Cheng) Path integrals Distance in hyperbolic geometry Measurements in the Poincar´eDisc Model (Hui) M¨obiustransformations of D Hyperbolic length and distance in D Conclusion Boundary, Length, Orientation-preserving isometries, Geodesics and Angles Reference Upper half-plane model H Introduction to Upper half-plane model - continued Hyperbolic geometry Five Postulates of Hyperbolic geometry: 1. A straight line segment can be drawn joining any two points. 2. Any straight line segment can be extended indefinitely in a straight line. 3. A circle may be described with any given point as its center and any distance as its radius. 4. All right angles are congruent. 5. For any given line R and point P not on R, in the plane containing both line R and point P there are at least two distinct lines through P that do not intersect R. Some interesting facts about hyperbolic geometry 1. Rectangles don't exist in hyperbolic geometry. 2. In hyperbolic geometry, all triangles have angle sum < π 3. In hyperbolic geometry if two triangles are similar, they are congruent. -
A Historical Introduction to Elementary Geometry
i MATH 119 – Fall 2012: A HISTORICAL INTRODUCTION TO ELEMENTARY GEOMETRY Geometry is an word derived from ancient Greek meaning “earth measure” ( ge = earth or land ) + ( metria = measure ) . Euclid wrote the Elements of geometry between 330 and 320 B.C. It was a compilation of the major theorems on plane and solid geometry presented in an axiomatic style. Near the beginning of the first of the thirteen books of the Elements, Euclid enumerated five fundamental assumptions called postulates or axioms which he used to prove many related propositions or theorems on the geometry of two and three dimensions. POSTULATE 1. Any two points can be joined by a straight line. POSTULATE 2. Any straight line segment can be extended indefinitely in a straight line. POSTULATE 3. Given any straight line segment, a circle can be drawn having the segment as radius and one endpoint as center. POSTULATE 4. All right angles are congruent. POSTULATE 5. (Parallel postulate) If two lines intersect a third in such a way that the sum of the inner angles on one side is less than two right angles, then the two lines inevitably must intersect each other on that side if extended far enough. The circle described in postulate 3 is tacitly unique. Postulates 3 and 5 hold only for plane geometry; in three dimensions, postulate 3 defines a sphere. Postulate 5 leads to the same geometry as the following statement, known as Playfair's axiom, which also holds only in the plane: Through a point not on a given straight line, one and only one line can be drawn that never meets the given line. -
Geometry Course Outline
GEOMETRY COURSE OUTLINE Content Area Formative Assessment # of Lessons Days G0 INTRO AND CONSTRUCTION 12 G-CO Congruence 12, 13 G1 BASIC DEFINITIONS AND RIGID MOTION Representing and 20 G-CO Congruence 1, 2, 3, 4, 5, 6, 7, 8 Combining Transformations Analyzing Congruency Proofs G2 GEOMETRIC RELATIONSHIPS AND PROPERTIES Evaluating Statements 15 G-CO Congruence 9, 10, 11 About Length and Area G-C Circles 3 Inscribing and Circumscribing Right Triangles G3 SIMILARITY Geometry Problems: 20 G-SRT Similarity, Right Triangles, and Trigonometry 1, 2, 3, Circles and Triangles 4, 5 Proofs of the Pythagorean Theorem M1 GEOMETRIC MODELING 1 Solving Geometry 7 G-MG Modeling with Geometry 1, 2, 3 Problems: Floodlights G4 COORDINATE GEOMETRY Finding Equations of 15 G-GPE Expressing Geometric Properties with Equations 4, 5, Parallel and 6, 7 Perpendicular Lines G5 CIRCLES AND CONICS Equations of Circles 1 15 G-C Circles 1, 2, 5 Equations of Circles 2 G-GPE Expressing Geometric Properties with Equations 1, 2 Sectors of Circles G6 GEOMETRIC MEASUREMENTS AND DIMENSIONS Evaluating Statements 15 G-GMD 1, 3, 4 About Enlargements (2D & 3D) 2D Representations of 3D Objects G7 TRIONOMETRIC RATIOS Calculating Volumes of 15 G-SRT Similarity, Right Triangles, and Trigonometry 6, 7, 8 Compound Objects M2 GEOMETRIC MODELING 2 Modeling: Rolling Cups 10 G-MG Modeling with Geometry 1, 2, 3 TOTAL: 144 HIGH SCHOOL OVERVIEW Algebra 1 Geometry Algebra 2 A0 Introduction G0 Introduction and A0 Introduction Construction A1 Modeling With Functions G1 Basic Definitions and Rigid -
Geometry (Lines) SOL 4.14?
Geometry (Lines) lines, segments, rays, points, angles, intersecting, parallel, & perpendicular Point “A point is an exact location in space. It has no length or width.” Points have names; represented with a Capital Letter. – Example: A a Lines “A line is a collection of points going on and on infinitely in both directions. It has no endpoints.” A straight line that continues forever It can go – Vertically – Horizontally – Obliquely (diagonally) It is identified because it has arrows on the ends. It is named by “a single lower case letter”. – Example: “line a” A B C D Line Segment “A line segment is part of a line. It has two endpoints and includes all the points between those endpoints. “ A straight line that stops It can go – Vertically – Horizontally – Obliquely (diagonally) It is identified by points at the ends It is named by the Capital Letter End Points – Example: “line segment AB” or “line segment AD” C B A Ray “A ray is part of a line. It has one endpoint and continues on and on in one direction.” A straight line that stops on one end and keeps going on the other. It can go – Vertically – Horizontally – Obliquely (diagonally) It is identified by a point at one end and an arrow at the other. It can be named by saying the endpoint first and then say the name of one other point on the ray. – Example: “Ray AC” or “Ray AB” C Angles A B Two Rays That Have the Same Endpoint Form an Angle. This Endpoint Is Called the Vertex. -
Unsteadiness in Flow Over a Flat Plate at Angle-Of-Attack at Low Reynolds Numbers∗
Unsteadiness in Flow over a Flat Plate at Angle-of-Attack at Low Reynolds Numbers∗ Kunihiko Taira,† William B. Dickson,‡ Tim Colonius,§ Michael H. Dickinson¶ California Institute of Technology, Pasadena, California, 91125 Clarence W. Rowleyk Princeton University, Princeton, New Jersey, 08544 Flow over an impulsively started low-aspect-ratio flat plate at angle-of-attack is inves- tigated for a Reynolds number of 300. Numerical simulations, validated by a companion experiment, are performed to study the influence of aspect ratio, angle of attack, and plan- form geometry on the interaction of the leading-edge and tip vortices and resulting lift and drag coefficients. Aspect ratio is found to significantly influence the wake pattern and the force experienced by the plate. For large aspect ratio plates, leading-edge vortices evolved into hairpin vortices that eventually detached from the plate, interacting with the tip vor- tices in a complex manner. Separation of the leading-edge vortex is delayed to some extent by having convective transport of the spanwise vorticity as observed in flow over elliptic, semicircular, and delta-shaped planforms. The time at which lift achieves its maximum is observed to be fairly constant over different aspect ratios, angles of attack, and planform geometries during the initial transient. Preliminary results are also presented for flow over plates with steady actuation near the leading edge. I. Introduction In recent years, flows around flapping insect wings have been investigated and, in particular, it has been observed that the leading-edge vortex (LEV) formed during stroke reversal remains stably attached throughout the wing stroke, greatly enhancing lift.1, 2 Such LEVs are found to be stable over a wide range of angles of attack and for Reynolds number over a range of Re ≈ O(102) − O(104). -
Points, Lines, and Planes a Point Is a Position in Space. a Point Has No Length Or Width Or Thickness
Points, Lines, and Planes A Point is a position in space. A point has no length or width or thickness. A point in geometry is represented by a dot. To name a point, we usually use a (capital) letter. A A (straight) line has length but no width or thickness. A line is understood to extend indefinitely to both sides. It does not have a beginning or end. A B C D A line consists of infinitely many points. The four points A, B, C, D are all on the same line. Postulate: Two points determine a line. We name a line by using any two points on the line, so the above line can be named as any of the following: ! ! ! ! ! AB BC AC AD CD Any three or more points that are on the same line are called colinear points. In the above, points A; B; C; D are all colinear. A Ray is part of a line that has a beginning point, and extends indefinitely to one direction. A B C D A ray is named by using its beginning point with another point it contains. −! −! −−! −−! In the above, ray AB is the same ray as AC or AD. But ray BD is not the same −−! ray as AD. A (line) segment is a finite part of a line between two points, called its end points. A segment has a finite length. A B C D B C In the above, segment AD is not the same as segment BC Segment Addition Postulate: In a line segment, if points A; B; C are colinear and point B is between point A and point C, then AB + BC = AC You may look at the plus sign, +, as adding the length of the segments as numbers. -
Historical Introduction to Geometry
i A HISTORICAL INTRODUCTION TO ELEMENTARY GEOMETRY Geometry is an word derived from ancient Greek meaning “earth measure” ( ge = earth or land ) + ( metria = measure ) . Euclid wrote the Elements of geometry between 330 and 320 B.C. It was a compilation of the major theorems on plane and solid geometry presented in an axiomatic style. Near the beginning of the first of the thirteen books of the Elements, Euclid enumerated five fundamental assumptions called postulates or axioms which he used to prove many related propositions or theorems on the geometry of two and three dimensions. POSTULATE 1. Any two points can be joined by a straight line. POSTULATE 2. Any straight line segment can be extended indefinitely in a straight line. POSTULATE 3. Given any straight line segment, a circle can be drawn having the segment as radius and one endpoint as center. POSTULATE 4. All right angles are congruent. POSTULATE 5. (Parallel postulate) If two lines intersect a third in such a way that the sum of the inner angles on one side is less than two right angles, then the two lines inevitably must intersect each other on that side if extended far enough. The circle described in postulate 3 is tacitly unique. Postulates 3 and 5 hold only for plane geometry; in three dimensions, postulate 3 defines a sphere. Postulate 5 leads to the same geometry as the following statement, known as Playfair's axiom, which also holds only in the plane: Through a point not on a given straight line, one and only one line can be drawn that never meets the given line. -
The Mass of an Asymptotically Flat Manifold
The Mass of an Asymptotically Flat Manifold ROBERT BARTNIK Australian National University Abstract We show that the mass of an asymptotically flat n-manifold is a geometric invariant. The proof is based on harmonic coordinates and, to develop a suitable existence theory, results about elliptic operators with rough coefficients on weighted Sobolev spaces are summarised. Some relations between the mass. xalar curvature and harmonic maps are described and the positive mass theorem for ,c-dimensional spin manifolds is proved. Introduction Suppose that (M,g) is an asymptotically flat 3-manifold. In general relativity the mass of M is given by where glJ, denotes the partial derivative and dS‘ is the normal surface element to S,, the sphere at infinity. This expression is generally attributed to [3]; for a recent review of this and other expressions for the mass and other physically interesting quantities see (41. However, in all these works the definition depends on the choice of coordinates at infinity and it is certainly not clear whether or not this dependence is spurious. Since it is physically quite reasonable to assume that a frame at infinity (“observer”) is given, this point has not received much attention in the literature (but see [15]). It is our purpose in this paper to show that, under appropriate decay conditions on the metric, (0.1) generalises to n-dimensions for n 2 3 and gives an invariant of the metric structure (M,g). The decay conditions roughly stated (for n = 3) are lg - 61 = o(r-’12), lag1 = o(f312), etc, and thus include the usual falloff conditions. -
Lesson 5: Three-Dimensional Space
NYS COMMON CORE MATHEMATICS CURRICULUM Lesson 5 M3 GEOMETRY Lesson 5: Three-Dimensional Space Student Outcomes . Students describe properties of points, lines, and planes in three-dimensional space. Lesson Notes A strong intuitive grasp of three-dimensional space, and the ability to visualize and draw, is crucial for upcoming work with volume as described in G-GMD.A.1, G-GMD.A.2, G-GMD.A.3, and G-GMD.B.4. By the end of the lesson, students should be familiar with some of the basic properties of points, lines, and planes in three-dimensional space. The means of accomplishing this objective: Draw, draw, and draw! The best evidence for success with this lesson is to see students persevere through the drawing process of the properties. No proof is provided for the properties; therefore, it is imperative that students have the opportunity to verify the properties experimentally with the aid of manipulatives such as cardboard boxes and uncooked spaghetti. In the case that the lesson requires two days, it is suggested that everything that precedes the Exploratory Challenge is covered on the first day, and the Exploratory Challenge itself is covered on the second day. Classwork Opening Exercise (5 minutes) The terms point, line, and plane are first introduced in Grade 4. It is worth emphasizing to students that they are undefined terms, meaning they are part of the assumptions as a basis of the subject of geometry, and they can build the subject once they use these terms as a starting place. Therefore, these terms are given intuitive descriptions, and it should be clear that the concrete representation is just that—a representation. -
Barycentric Coordinates in Tetrahedrons
Computational Geometry Lab: BARYCENTRIC COORDINATES IN TETRAHEDRONS John Burkardt Information Technology Department Virginia Tech http://people.sc.fsu.edu/∼jburkardt/presentations/cg lab barycentric tetrahedrons.pdf December 23, 2010 1 Introduction to this Lab In this lab we consider the barycentric coordinate system for a tetrahedron. This coordinate system will give us a common map that can be used to relate all tetrahedrons. This will give us a unified way of dealing with the computational tasks that must take into account the varying geometry of tetrahedrons. We start our exploration by asking whether we can come up with an arithmetic formula that measures the position of a point relative to a plane. The formula we arrive at will actually return a signed distance which is positive for points on one side of the plane, and negative on the other side. The extra information that the sign of the distance gives us is enough to help us answer the next question, which is whether we can determine if a point is inside a tetrahedron. This turns out to be simple if we apply the signed distance formula in the right way. The distance function turns out to have another crucial use. Given any face of the tetrahedron, we know that the tetrahedral point that is furthest from that face is the vertex opposite to the face. Therefore, any other point in the tetrahedron has a relative distance to the face that is strictly less than 1. For a given point, if we compute all four possible relative distances, we come up with our crucial barycentric coordinate system. -
Combinatorial Properties of Complex Hyperplane Arrangements
Combinatorial Properties of Complex Hyperplane Arrangements by Ben Helford A Thesis Submitted in Partial Fulfillment of the Requirements for the Degree of Master of Science in Mathematics Northern Arizona University December 2006 Approved: Michael Falk, Ph.D., Chair N´andor Sieben, Ph.D. Stephen E. Wilson, Ph.D. Abstract Combinatorial Properties of Complex Hyperplane Arrangements Ben Helford Let A be a complex hyperplane arrangement, and M(A) be the com- [ plement, that is C` − H. It has been proven already that the co- H∈A homology algebra of M(A) is determined by its underlying matroid. In fact, in the case where A is the complexification of a real arrangement, one can determine the homotopy type by its oriented matroid. This thesis uses complex oriented matroids, a tool developed recently by D Biss, in order to combinatorially determine topological properties of M(A) for A an arbitrary complex hyperplane arrangement. The first chapter outlines basic properties of hyperplane arrange- ments, including defining the underlying matroid and, in the real case, the oriented matroid. The second chapter examines topological proper- ties of complex arrangements, including the Orlik-Solomon algebra and Salvetti’s theorem. The third chapter introduces complex oriented ma- troids and proves some ways that this codifies topological properties of complex arrangements. Finally, the fourth chapter examines the differ- ence between complex hyperplane arrangements and real 2-arrangements, and examines the problem of formulating the cone/decone theorem at the level of posets. ii Acknowledgements It almost goes without saying in my mind that this thesis could not be possible without the direction and expertise provided by Dr. -
Perpendicular and Parallel Line Segments
Name: Date: r te p a h Perpendicular and C Parallel Line Segments Practice 1 Drawing Perpendicular Line Segments Use a protractor to draw perpendicular line segments. Example Draw a line segment perpendicular to RS through point T. S 0 180 10 1 70 160 20 150 30 140 40 130 50 0 120 180 6 0 10 11 0 170 70 20 100 30 160 80 40 90 80 150 50 70 60 140 100 130 110 120 R T © Marshall Cavendish International (Singapore) Private Limited. Private (Singapore) International © Marshall Cavendish 1. Draw a line segment perpendicular to PQ. P Q 2. Draw a line segment perpendicular to TU through point X. X U T 67 Lesson 10.1 Drawing Perpendicular Line Segments 08(M)MIF2015CC_WBG4B_Ch10.indd 67 4/30/13 11:18 AM Use a drawing triangle to draw perpendicular line segments. Example M L N K 3. Draw a line segment 4. Draw a line segment perpendicular to EF . perpendicular to CD. C E F D © Marshall Cavendish International (Singapore) Private Limited. Private (Singapore) International © Marshall Cavendish 5. Draw a line segment perpendicular to VW at point P. Then, draw another line segment perpendicular to VW through point Q. Q V P W Line Segments 68 and Parallel Chapter 10 Perpendicular 08(M)MIF2015CC_WBG4B_Ch10.indd 68 4/30/13 11:18 AM Name: Date: Practice 2 Drawing Parallel Line Segments Use a drawing triangle and a straightedge to draw parallel line segments. Example Draw a line segment parallel to AB . A B 1. Draw a pair of parallel line segments.