DOCSLIB.ORG

Chapter 12 Transformations: Shapes in Motion

Total Page：16

File Type：pdf, Size：1020Kb

Download full-text PDF Read full-text
Chapter 12 Transformations: Shapes in Motion Chapter 12 Transformations: Shapes in Motion Table of Contents Reflections – Day 1 ……………………………………………..…………….. Page 1 SWBAT: Graph Reflections in the Coordinate Plane HW: Pages #8 - 10 Translations – Day 2 ……………….……….…………….……..…………….. Page 11 SWBAT: Graph Translations in the Coordinate Plane HW: Pages #15 - 16 Rotations – Day 3…………………………………………..………………….. Page 17 SWBAT: Graph Rotations in the Coordinate Plane HW: Pages #23-24 Dilations/Symmetry – Day 4 …………………………………………….….….. Page 25 SWBAT: Graph Dilations in the Coordinate Plane and Identify Line/Rotational Symmetry HW: Pages #31-34 Review – Day 5 ……………………………………………..……..…………….. Page 35 SWBAT: Graph Transformations in the Coordinate Plane HW: Pages #35-38 Compositions – Day 6……………………..……………………………….…….. Page 39 SWBAT: Graph Compositions in the Coordinate Plane HW: Pages #46-49 Overall Review – Day 7……………………….………………………..………….. Page 50 SWBAT: Graph Transformations in the Coordinate Plane HW: Pages #50-61 TRANSFORMATIONS RULES ………….…………………………………………..Page 62 Reflections – Day 1 An Introduction to Transformations 1 Example 1: Example 2: 2 Reflections A reflection (or flip) is an isometry in which a figure and its image have opposite orientations. Thus, a reflected image in a mirror appears "backwards." Reflections in the Coordinate Plane 1. 3 3. 4. Regents Questions 5. 6. 7. 8. 4 Reflecting Over Vertical and Horizontal Lines 9. 10. 5 Identifying a Reflection Write a rule to describe each transformation. 11. 12. Challenge 6 Summary Exit Ticket 7 Homework for Reflections – Day 1 16. 17. 8 Graphing Reflections 9 Identifying Reflections 10 Translations – Day 2 Warm - Up 1. 2. 11 3. 4. 5. 6. 12 You Try It! 1) Triangle DEF is a translation of triangle ABC. Use the diagram to write a rule for the translation of triangle ABC to Triangle DEF. 2) Pentagon ABCDE is drawn on the grid below. On the grid, draw a translation of pentagon ABCDE using the rule T3,-5. 13 Challenge Summary Exit Ticket 14 Homework 15 16. T5,1 17. T-1, 2 18. T0, -3 19. T4, -4 16 Rotations – Day 3 Warm - Up 1. 2. 17 Notice that degree movement on a unit circle goes in a counterclockwise direction. You will want to remember the layout of the unit circle when you are graphing figures and their rotations. 18 Rules (x, y) R90 = ( ___, ____) R180 = ( ___, ____) R270 = ( ___, ____) Practice 3. 4. ( 9, -1) 5. (-4, -8) 19 Rotations in the Coordinate Plane 9. 90 X’( ___, ____) Y’( ___, ____) Z’( ___, ____) 90 10. 180 180 ***NOTE 20 Practice with a Point Reflection in the Origin Identifying a Rotation Write a rule to describe each transformation. a. b. 21 Challenge Summary Exit Ticket 22 Homework 23 24 Dilations/Symmetry – Day 4 Warm – Up 1. 2. 25 To find the image of a point under a dilation, you multiply each coordinate by the scale factor. 1 1 1 a) D4 (x,y) (4x,4y) b) D (x,y) ( x, Y ) 6 6 6 Example- Find a) D2(3,4) b) D (6,9) 1 3 Dilations in the Coordinate Plane 1. 26 2. Regents Questions 3. 4. 5. 6. 7. 27 28 Tell whether each figure has rotational symmetry. If so, give the angle of rotational symmetry. Tell whether each figure has rotational symmetry. If so, give the angle of rotational symmetry. 29 Challenge SUMMARY 30 Homework – Dilations/Symmetry – Day 4 31 22. 23. 32 Symmetry 33 34 Review – Day 5 35 36 37 38 Compositions – Day 6 Warm – Up 1. 2. Which rotation about point O maps B to D? _______ 39 c) 40 Practice Problem #1 You try It! 41 Practice Problem #2 You try It! 42 The symbol for a composition of transformations is an open circle. The notation is read as a reflection in the x-axis following a translation of (x+3, y+4). Be careful!!! The process is done in reverse!! You may see various notations which represent a composition of transformations: could also be indicated by Problem #3 43 You Try It! CHALLENGE 44 SUMMARY Exit Ticket 45 Homework – Compositions – Day 6 1. 2. 3. 46 4. 5. 6. 7. 7. 47 8. 9. 48 10. 49 Review – Day 7 Transformations Review SUMMARY TABLE 50 Section 1: Reflections 51 Line Reflections 52 Section 2: Translations 53 54 Section 3: Rotations 3. Locate and label A’, the image of A under R270 (three quarter-turn about the origin) 55 56 Section 4: Dilations/Symmetry 57 58 Section 5: Compositions 1. 2. fdg 3. 4. 5. Find the composite transformation indicated. 59 6. 7. 60 8. *** Other Properties*** 5. 61 62 .
Load more

Recommended publications
  • Simple Closed Geodesics on Regular Tetrahedra in Lobachevsky Space
    Simple closed geodesics on regular tetrahedra in Lobachevsky space Alexander A. Borisenko, Darya D. Sukhorebska Abstract. We obtained a complete classification of simple closed geodesics on regular tetrahedra in Lobachevsky space. Also, we evaluated the number of simple closed geodesics of length not greater than L and found the asymptotic of this number as L goes to infinity. Keywords: closed geodesics, simple geodesics, regular tetrahedron, Lobachevsky space, hyperbolic space. MSC: 53С22, 52B10 1 Introduction A closed geodesic is called simple if this geodesic is not self-intersecting and does not go along itself. In 1905 Poincare proposed the conjecture on the existence of three simple closed geodesics on a smooth convex surface in three-dimensional Euclidean space. In 1917 J. Birkhoff proved that there exists at least one simple closed geodesic on a Riemannian manifold that is home- omorphic to a sphere of arbitrary dimension [1]. In 1929 L. Lyusternik and L. Shnirelman obtained that there exist at least three simple closed geodesics on a compact simply-connected two-dimensional Riemannian manifold [2], [3]. But the proof by Lyusternik and Shnirelman contains substantial gaps. I. A. Taimanov gives a complete proof of the theorem that on each smooth Riemannian manifold homeomorphic to the two-dimentional sphere there exist at least three distinct simple closed geodesics [4]. In 1951 L. Lyusternik and A. Fet stated that there exists at least one closed geodesic on any compact Riemannian manifold [5]. In 1965 Fet improved this results. He proved that there exist at least two closed geodesics on a compact Riemannian manifold under the assumption that all closed geodesics are non-degenerate [6].
    [Show full text]
  • Geometry Without Points
    GEOMETRY WITHOUT POINTS Dana S. Scott, FBA, FNAS University Professor Emeritus Carnegie Mellon University Visiting Scholar University of California, Berkeley This is a preliminary report on on-going joint work with Tamar Lando, Philosophy, Columbia University !1 Euclid’s Definitions • A point is that which has no part. • A line is breadthless length. • A surface is that which has length and breadth only. The Basic Questions • Are these notions too abstract ? Or too idealized ? • Can we develop a theory of regions without using points ? • Does it make sense for geometric objects to be only solids ? !2 Famous Proponents of Pointlessness Gottfried Wilhelm von Leibniz (1646 – 1716) Nikolai Lobachevsky (1792 – 1856) Edmund Husserl (1859 – 1938) Alfred North Whitehead (1861 – 1947) Johannes Trolle Hjelmslev (1873 – 1950) Edward Vermilye Huntington (1874 – 1952) Theodore de Laguna (1876 – 1930) Stanisław Leśniewski (1886 – 1939) Jean George Pierre Nicod (1893 – 1924) Leonard Mascot Blumenthal (1901 – 1984) Alfred Tarski (1901 – 1983) Karl Menger (1902 – 1985) John von Neumann (1903 – 1957) Henry S. Leonard (1905 – 1967) Nelson Goodman (1906 – 1998) !3 Two Quotations Mathematics is a part of physics. Physics is an experimental science, a part of natural science. Mathematics is the part of physics where experiments are cheap. -- V.I. Arnol’d, in a lecture, Paris, March 1997 I remember once when I tried to add a little seasoning to a review, but I wasn't allowed to. The paper was by Dorothy Maharam, and it was a perfectly sound contribution to abstract measure theory. The domains of the underlying measures were not sets but elements of more general Boolean algebras, and their range consisted not of positive numbers but of certain abstract equivalence classes.
    [Show full text]
  • Draft Framework for a Teaching Unit: Transformations
    Co-funded by the European Union PRIMARY TEACHER EDUCATION (PrimTEd) PROJECT GEOMETRY AND MEASUREMENT WORKING GROUP DRAFT FRAMEWORK FOR A TEACHING UNIT Preamble The general aim of this teaching unit is to empower pre-service students by exposing them to geometry and measurement, and the relevant pe dagogical content that would allow them to become skilful and competent mathematics teachers. The depth and scope of the content often go beyond what is required by prescribed school curricula for the Intermediate Phase learners, but should allow pre- service teachers to be well equipped, and approach the teaching of Geometry and Measurement with confidence. Pre-service teachers should essentially be prepared for Intermediate Phase teaching according to the requirements set out in MRTEQ (Minimum Requirements for Teacher Education Qualifications, 2019). “MRTEQ provides a basis for the construction of core curricula Initial Teacher Education (ITE) as well as for Continuing Professional Development (CPD) Programmes that accredited institutions must use in order to develop programmes leading to teacher education qualifications.” [p6]. Competent learning… a mixture of Theoretical & Pure & Extrinsic & Potential & Competent learning represents the acquisition, integration & application of different types of knowledge. Each type implies the mastering of specific related skills Disciplinary Subject matter knowledge & specific specialized subject Pedagogical Knowledge of learners, learning, curriculum & general instructional & assessment strategies & specialized Learning in & from practice – the study of practice using Practical learning case studies, videos & lesson observations to theorize practice & form basis for learning in practice – authentic & simulated classroom environments, i.e. Work-integrated Fundamental Learning to converse in a second official language (LOTL), ability to use ICT & acquisition of academic literacies Knowledge of varied learning situations, contexts & Situational environments of education – classrooms, schools, communities, etc.
    [Show full text]
  • Hands-On Explorations of Plane Transformations
    Hands-On Explorations of Plane Transformations James King University of Washington Department of Mathematics [email protected] http://www.math.washington.edu/~king The “Plan” • In this session, we will explore exploring. • We have a big math toolkit of transformations to think about. • We have some physical objects that can serve as a hands- on toolkit. • We have geometry relationships to think about. • So we will try out at many combinations as we can to get an idea of how they work out as a real-world experience. • I expect that we will get some new ideas from each other as we try out different tools for various purposes. Our Transformational Case of Characters • Line Reflection • Point Reflection (a rotation) • Translation • Rotation • Dilation • Compositions of any of the above Our Physical Toolkit • Patty paper • Semi-reflective plastic mirrors • Graph paper • Ruled paper • Card Stock • Dot paper • Scissors, rulers, protractors Reflecting a point • As a first task, we will try out tools for line reflection of a point A to a point B. Then reflecting a shape. A • Suggest that you try the semi-reflective mirrors and the patty paper for folding and tracing. Also, graph paper is an option. Also, regular paper and cut-outs M • Note that pencils and overhead pens work on patty paper but not ballpoints. Also not that overhead dots are easier to see with the mirrors. B • Can we (or your students) conclude from your C tool that the mirror line is the perpendicular bisector of AB? Which tools best let you draw this reflection? • When reflecting shapes, consider how to reflect some polygon when it is not all on one side of the mirror line.
    [Show full text]
  • Rigid Motion – a Transformation That Preserves Distance and Angle Measure (The Shapes Are Congruent, Angles Are Congruent)
    REVIEW OF TRANSFORMATIONS GEOMETRY Rigid motion – A transformation that preserves distance and angle measure (the shapes are congruent, angles are congruent). Isometry – A transformation that preserves distance (the shapes are congruent). Direct Isometry – A transformation that preserves orientation, the order of the lettering (ABCD) in the figure and the image are the same, either both clockwise or both counterclockwise (the shapes are congruent). Opposite Isometry – A transformation that DOES NOT preserve orientation, the order of the lettering (ABCD) is reversed, either clockwise or counterclockwise becomes clockwise (the shapes are congruent). Composition of transformations – is a combination of 2 or more transformations. In a composition, you perform each transformation on the image of the preceding transformation. Example: rRx axis O,180 , the little circle tells us that this is a composition of transformations, we also execute the transformations from right to left (backwards). If you would like a visual of this information or if you would like to quiz yourself, go to http://www.mathsisfun.com/geometry/transformations.html. Line Reflection Point Reflection Translations (Shift) Rotations (Turn) Glide Reflection Dilations (Multiply) Rigid Motion Rigid Motion Rigid Motion Rigid Motion Rigid Motion Not a rigid motion Opposite isometry Direct isometry Direct isometry Direct isometry Opposite isometry NOT an isometry Reverse orientation Same orientation Same orientation Same orientation Reverse orientation Same orientation Properties preserved: Properties preserved: Properties preserved: Properties preserved: Properties preserved: Properties preserved: 1. Distance 1. Distance 1. Distance 1. Distance 1. Distance 1. Angle measure 2. Angle measure 2. Angle measure 2. Angle measure 2. Angle measure 2. Angle measure 2.
    [Show full text]
  • Symmetry Groups of Platonic Solids
    Symmetry Groups of Platonic Solids David Newcomb Stanford University 03/09/12 Problem Describe the symmetry groups of the Platonic solids, with proofs, and with an emphasis on the icosahedron. Figure 1: The five Platonic solids. 1 Introduction The first group of people to carefully study Platonic solids were the ancient Greeks. Although they bear the namesake of Plato, the initial proofs and descriptions of such solids come from Theaetetus, a contemporary. Theaetetus provided the first known proof that there are only five Platonic solids, in addition to a mathematical description of each one. The five solids are the cube, the tetrahedron, the octahedron, the icosahedron, and the dodecahedron. Euclid, in his book Elements also offers a more thorough description of the construction and properties of each solid. Nearly 2000 years later, Kepler attempted a beautiful planetary model involving the use of the Platonic solids. Although the model proved to be incorrect, it helped Kepler discover fundamental laws of the universe. Still today, Platonic solids are useful tools in the natural sciences. Primarily, they are important tools for understanding the basic chemistry of molecules. Additionally, dodecahedral behavior has been found in the shape of the earth's crust as well as the structure of protons in nuclei. 1 The scope of this paper, however, is limited to the mathematical dissection of the sym- metry groups of such solids. Initially, necessary definitions will be provided along with important theorems. Next, the brief proof of Theaetetus will be discussed, followed by a discussion of the broad technique used to determine the symmetry groups of Platonic solids.
    [Show full text]
  • Transformation Geometry — Math 331 April 14, 2004 the Classification of Isometries of R3:III Proposition
    Transformation Geometry — Math 331 April 14, 2004 The Classification of Isometries of R3: III Proposition. If a rotation of R3 is composed with the translation by a vector that is perpendicular to the axis of the rotation, the resulting isometry is a rotation with axis parallel to the original axis. Proof. Since both rotations and translations are orientation-preserving, the composition is orientation-preserving, and the question of why it must be a rotation is that of why it must have a fixed point. Let Π be a plane that is perpendicular to the axis of the given rotation. The given rotation induces a rotation in Π, and, since the given vector may be viewed as a vector in Π, the effect of the composed isometry of R3 in the plane Π is an isometry of Π that is the composition of a rotation in Π and a translation in Π. Since in Π the composition of a rotation and a translation is a rotation, the point in Π that is the center of the latter rotation of Π is a fixed point of the composed isometry of R3, and, therefore, the composed isometry is a rotation. It is clear that the distance of this fixed point, i.e., the point of the axis of the new rotation in Π, from the axis of the given rotation is independent of which plane Π normal to the original axis is chosen and, therefore, that the axis of the new rotation is parallel to that of the original. Definition. The isometry that results from composing a non-identity rotation with a non-identity translation parallel to its axis is called a screw.
    [Show full text]
  • F-Vectors of 3-Polytopes Symmetric Under Rotations and Rotary Reflections
    f-vectors of 3-polytopes symmetric under rotations and rotary reflections Maren H. Ring,∗ Robert Sch¨ulery February 21, 2020 Abstract The f-vector of a polytope consists of the numbers of its i-dimensional faces. An open field of study is the characterization of all possible f- vectors. It has been solved in three dimensions by Steinitz in the early 19th century. We state a related question, i.e. to characterize f-vectors of three dimensional polytopes respecting a symmetry, given by a finite group of matrices. We give a full answer for all three dimensional polytopes that are symmetric with respect to a finite rotation or rotary reflection group. We solve these cases constructively by developing tools that generalize Steinitz's approach. 1 Introduction There are many studies of f-vectors in higher dimensions, for example see [Gr¨u03],[Bar71], [Bar72], [Bar73], [BB84], [Sta80], [Sta85] or [BB85]. The set of f-vectors of four dimensional polytopes has been studied in [BR73], [Bar74], [AS85], [Bay87], [EKZ03], [Zie02] and [BZ18]. Some insights about f-vectors of centrally symmetric polytopes are given in [BL82], [AN06], [Sta87] and [FHSZ13]. It is still an open question, even in three dimensions, what the f-vectors of symmetric polytopes are. This question will be partially answered in this paper. In particular, given a finite 3 × 3 matrix group G, we ask to determine the arXiv:2002.00355v2 [math.MG] 20 Feb 2020 set F (G) of vectors (f0; f2) 2 N × N such that there is a polytope P symmetric under G (i.e. A · P = P for all A 2 G) with f0 vertices and f2 facets (we omit the number of edges by the Euler-equation).
    [Show full text]
  • Isometries Come in Circles by George Baloglou
    Isometries come in circles by George Baloglou ([email protected]) Department of Mathematics, SUNY Oswego, NY 13126 In the study of geometry, one is constantly confronted with groups of transformations on various “spaces.” Many of these groups consist simply of the symmetries of those spaces with respect to suitably chosen properties. An obvious example is furnished by the symmetries of the cube. Geometrically speaking, these are the one-one transformations which preserve distances on the cube. They are known as “isometries,” and are 48 in number. [Birkhoff & MacLane, Survey of Modern Algebra (1941), p. 127] The goal of this note is a purely geometrical classification of isometries of the line, circle, plane, sphere and space. The main idea employed is that every isometry of Rn is essentially determined, for n = 2 and n = 3 at least, by its effect on one circle, where it is conveniently ‘trapped’. Moreover, we stress the affinity between isometries in R1, R2 and R3 and offer, with the exception of one lemma, what we view as a ’two-dimensional’ classification of isometries of R3. Our method differs substantially from the standard geometrical approach (as given, for example, in chapters 3 & 7 of [3] or 8 & 16 of [5]) and is, we hope, more constructive and intuitive. Before we begin, let us recall that every isometry of R1 is determined by its effect on 2 non-identical points, every isometry of R2 is determined by its effect on 3 non-collinear points, every isometry of R3 is determined by its effect on 4 non-coplanar points, and so on.
    [Show full text]
  • Symmetry of Molecules and Point Groups
    Symmetry of Molecules and Point Groups What does symmetry mean? Symmetry (Greek = harmony, regularity) means the repetition of a motif and thus the agreement of parts of an ensemble (Fig. 1). Precession pattern of LiAlSiO4 Ice crystal Rotation of ClH2C-CH2Cl (a*b* plane, symmetry 6mm) (symmetry ~6mm) (symmetry C2, C2v or C2h) Matrix for a vector rotation J.S. Bach, „Die Kunst der Fuge“ Anti-symmetry Radiolarian shell (Circogonia Normal modes of XeF4 3D object icodaedra) with icosaeder symmetry (symmetry group D4h) (csi.chemie.tu-darmstadt.de/ak/immel/) Fig.1 Examples of symmetric objects Symmetry can also mean harmony of proportions, or stability, order, and beauty. 1 Definition: An object is symmetric if it is left invariant by a transformation, i.e., cannot be distinguished before and after transformation. Symmetry transformations, operations, elements are: Symbol* Symmetry operation * Notation of symmetry elements after Schönflies (Sch for moleculs) Sch HM and International Notation after Hermann/Mauguin (HM for crystals) E (1) identity (E from “Einheit” = unity, an object is left unchanged) Cn (n) properrotation through an angle of 2π/n rad. improperrotation through an angle of 2π/n rad. Sn followed by a reflection in a plane perpendicular to the axis (rotation-reflection axis) improperrotation through an angle of 2π/n rad. n followed by a reflection through a point on the axis (rotation- inversion axis) inversion (point reflection) ( 1 ≡ S ) → i 2 1 (x, y, z →-x, -y, -z in Cartesian coordinates) σ m mirror plane (from “Spiegel”) horizontal reflection in a plane passing through the origin and σ h perpendicular to the axis with highest symmetry vertical reflection in a plane passing through the origin and the σ v axis with highest symmetry diagonal reflection in a plane as σv and bisecting the angle σd between the two-fold axis perpendicular to the axis of highest symmetry t translation t = n1⋅a+ n2⋅b + n3⋅c 1.
    [Show full text]
  • [Math.GR] 10 Feb 2000 Otnosbnr Operation Binary Continuous a X Od for Hold
    GLOBAL LEFT LOOP STRUCTURES ON SPHERES MICHAEL K. KINYON Abstract. On the unit sphere S in a real Hilbert space H, we derive a binary operation ⊙ such that (S, ⊙) is a power-associative Kikkawa left loop with two-sided identity e0, i.e., it has the left inverse, automorphic inverse, and Al properties. The operation ⊙ is compatible with the symmetric space structure of S. (S, ⊙) is not a loop, and the right translations which fail to be injective are easily characterized. (S, ⊙) satisfies the left power alternative and left Bol identities “almost everywhere” but not everywhere. Left translations are everywhere analytic; right translations are analytic except at −e0 where they have a nonremovable discontinuity. The orthogonal group O(H) is a semidirect product of (S, ⊙) with its automorphism group. The left loop structure of (S, ⊙) gives some insight into spherical geometry. 1. Introduction Let H be a real Hilbert space with inner product h·, ·i. Let (1.1) S = {x ∈ H : hx, xi =1} be the unit sphere in H. For x, y ∈ S, set (1.2) x ∗ y =2hx, yix − y. ([16], p.66). If x and y span a plane Π through the origin, then x ∗ y is a point lying in S ∩ Π which is obtained by reflecting y in Π about the line passing through x and the origin. Equivalently, thinking of S ∩ Π as the great circle passing through x and y, x ∗ y is the point on S ∩ Π whose angle with x is the same as the angle between x and y, but with the opposite orientation.
    [Show full text]
  • Chapter 6 Transformation and the Coordinate Plane
    14365C06.pgs 7/12/07 2:57 PM Page 209 CHAPTER 6 TRANSFORMATIONS AND THE COORDINATE CHAPTER PLANE TABLE OF CONTENTS 6-1 The Coordinates of a Point in a Plane In our study of mathematics, we are accustomed to representing an equation as a line or a curve. This 6-2 Line Reflections blending of geometry and algebra was not always famil- 6-3 Line Reflections in the Coordinate Plane iar to mathematicians. In the seventeenth century, René Descartes (1596–1650), a French philosopher 6-4 Point Reflections in the Coordinate Plane and mathematician, applied algebraic principles and 6-5 Translations in the methods to geometry. This blending of algebra and Coordinate Plane geometry is known as coordinate geometry or 6-6 Rotations in the Coordinate analytic geometry. Pierre de Fermat (1601–1665) Plane independently developed analytic geometry before 6-7 Glide Reflections Descartes but Descartes was the first to publish his 6-8 Dilations in the Coordinate work. Plane Descartes showed that a curve in a plane could be 6-9 Transformations as Functions completely determined if the distances of its points Chapter Summary from two fixed perpendicular lines were known. We Vocabulary call these distances the Cartesian coordinates of the points; thus giving Descartes’ name to the system Review Exercises that he developed. Cumulative Review 209 14365C06.pgs 7/12/07 2:57 PM Page 210 210 Transformations and the Coordinate Plane 6-1 THE COORDINATES OF A POINT IN A PLANE In this chapter, we will review what you know about the coordinate plane and y you will study transformations and symmetry, which are common elements in 3 nature, art, and architecture.
    [Show full text]