
MA4-17MG Properties of geometrical figures 1
... opposite, isosceles, protractor, transversal, equilateral, acute, alternate, quadrilateral, convex quadrilateral, non-convex quadrilateral, line symmetry, rotational symmetry, axis, axes, square, rectangle, kite, rhombus, parallelogram, trapezium, interior, exterior, interval, complement, supplement ...
... opposite, isosceles, protractor, transversal, equilateral, acute, alternate, quadrilateral, convex quadrilateral, non-convex quadrilateral, line symmetry, rotational symmetry, axis, axes, square, rectangle, kite, rhombus, parallelogram, trapezium, interior, exterior, interval, complement, supplement ...
Study Guide - Village Christian School
... To find linear pairs, look for adjacent angles whose non-common sides are opposite rays. <1 and < 2 are a linear pair. < 2 and < 3 are also a linear pair. < 3 and < 4 are also a linear pair. < 1 and < 4 are also a linear pair. To find vertical angles, look for angles formed by intersecting lines. < ...
... To find linear pairs, look for adjacent angles whose non-common sides are opposite rays. <1 and < 2 are a linear pair. < 2 and < 3 are also a linear pair. < 3 and < 4 are also a linear pair. < 1 and < 4 are also a linear pair. To find vertical angles, look for angles formed by intersecting lines. < ...
Triangle Sum Proof
... The student’s proof reveals some evidence of an overall strategy, but the student fails to establish major conditio Examples of Student Work at this Level The student’s proof establishes the congruence of the alternate interior angles but goes no further. ...
... The student’s proof reveals some evidence of an overall strategy, but the student fails to establish major conditio Examples of Student Work at this Level The student’s proof establishes the congruence of the alternate interior angles but goes no further. ...
Deductive Proof in Geometry
... right angles are equal. This may seem obvious, but it actually assumes that space is the same in all directions - by this we mean that a figure will be independent of the position in space in which it is placed. This idea is central to most spatial concepts in physics. When I taught physics, we spen ...
... right angles are equal. This may seem obvious, but it actually assumes that space is the same in all directions - by this we mean that a figure will be independent of the position in space in which it is placed. This idea is central to most spatial concepts in physics. When I taught physics, we spen ...
Template for Navigation to PowerPoint Presentation Title: Module 4
... 1. Develop your power point presentation as normal with engaging graphics, interesting text, and designed just how you like. 2. Place the presentation in the zip file. The presentation will be placed in the new template which will allow students to view additional navigation options of the topics pr ...
... 1. Develop your power point presentation as normal with engaging graphics, interesting text, and designed just how you like. 2. Place the presentation in the zip file. The presentation will be placed in the new template which will allow students to view additional navigation options of the topics pr ...
Euler angles
The Euler angles are three angles introduced by Leonhard Euler to describe the orientation of a rigid body. To describe such an orientation in 3-dimensional Euclidean space three parameters are required. They can be given in several ways, Euler angles being one of them; see charts on SO(3) for others. Euler angles are also used to describe the orientation of a frame of reference (typically, a coordinate system or basis) relative to another. They are typically denoted as α, β, γ, or φ, θ, ψ.Euler angles represent a sequence of three elemental rotations, i.e. rotations about the axes of a coordinate system. For instance, a first rotation about z by an angle α, a second rotation about x by an angle β, and a last rotation again about z, by an angle γ. These rotations start from a known standard orientation. In physics, this standard initial orientation is typically represented by a motionless (fixed, global, or world) coordinate system; in linear algebra, by a standard basis.Any orientation can be achieved by composing three elemental rotations. The elemental rotations can either occur about the axes of the fixed coordinate system (extrinsic rotations) or about the axes of a rotating coordinate system, which is initially aligned with the fixed one, and modifies its orientation after each elemental rotation (intrinsic rotations). The rotating coordinate system may be imagined to be rigidly attached to a rigid body. In this case, it is sometimes called a local coordinate system. Without considering the possibility of using two different conventions for the definition of the rotation axes (intrinsic or extrinsic), there exist twelve possible sequences of rotation axes, divided in two groups: Proper Euler angles (z-x-z, x-y-x, y-z-y, z-y-z, x-z-x, y-x-y) Tait–Bryan angles (x-y-z, y-z-x, z-x-y, x-z-y, z-y-x, y-x-z). Tait–Bryan angles are also called Cardan angles; nautical angles; heading, elevation, and bank; or yaw, pitch, and roll. Sometimes, both kinds of sequences are called ""Euler angles"". In that case, the sequences of the first group are called proper or classic Euler angles.