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Chapter 3 Student Notes
Chapter 3 Student Notes

03. Euclid
03. Euclid

1st Semester Final Review Packet
1st Semester Final Review Packet

... 8. Specify a series of transformations that map PDM onto EJS. You may use descriptions, function rules, and/or coordinate rules as long as they are complete. ...
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Parallel Lines Intersected by a Transversal Parallel Lines

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For each REGULAR polygon, find the SUM of the interior angles
For each REGULAR polygon, find the SUM of the interior angles

UNIT 7 – TRIGONOMETRY IN ACUTE TRIANGLES (Lesson 1
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Angles and Parallel Lines
Angles and Parallel Lines

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RHOMBUS

... b) According to the reflexive property, RO = ? c) Why is HM = MH? d) What triangle congruence conditions justifies ∆HRM ≅ ∆ MOH? e) What other two triangles are congruent by Side-Side-Side? f) Why is ∠4≅∠8? g) What other two angles are congruent by CPCTC? h) Name two other pairs of congruent angles. ...
Chapter Audio Summary for McDougal Littell
Chapter Audio Summary for McDougal Littell

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Similar Polygons (notes)
Similar Polygons (notes)

Geometry Fall 2011 Lesson 17 (S.A.S. Postulate)
Geometry Fall 2011 Lesson 17 (S.A.S. Postulate)

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geometry - SchoolRack

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End of Module Study Guide: Concepts of Congruence Rigid Motions

... Alternate Interior Angles:  Angles  on  opposite  sides  of  the  transversal  on  the   inside  of  the  parallel  lines.    Alternate  interior  angles  are  congruent  because  you  can   map  one  to  another  by  rotating  180°  arou ...
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4.2 Multiplying Matrices & 4.3a Determinants of Matrices

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Notes 4.1

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Propositions 11

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Math 8 Lesson Plan 69E Complementary Angles class outline for

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Pg. 19 #5, 6

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Geometry

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6.2 Similar Triangle Theorems

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Geometry Lesson 11-3 Inscribed Angles.notebook

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... Geometry Section 1.4 ...
< 1 ... 466 467 468 469 470 471 472 473 474 ... 552 >

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.
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