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7.3 similar triangles.notebook
7.3 similar triangles.notebook

Chapter 5 - Angelfire
Chapter 5 - Angelfire

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studentproofs

... It is given that angle 2 is congruent to angle 6. We want to prove that angle 1 is congruent to angle 5, angle 7 is congruent to angle 3, and angle 8 is congruent to angle 4. Proof: By the problem on vertical angles (16(b)), angle 2 is congruent to angle 3 and angle 6 is congruent to angle 7. Theref ...
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... At first, I assumed that we are having hamburgers because today is Tuesday, and Tuesday is usually hamburger day. There is always ketchup on the table when we have hamburgers, so I looked for the ketchup, but I didn’t see any. So, my assumption that we are having hamburgers must be false. The studen ...
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a. Angles NMQ and MNP are consecutive angles. b. Angles MQP

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... While the congruence postulates and theorems apply for all triangles, we have postulates and theorems that apply specifically for right triangles. HL Postulate If the hypotenuse and leg of one right triangle are congruent to the hypotenuse and leg of another right triangle, then the triangles are co ...
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Chapter 4: Parallels - New Lexington City Schools

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Trigonometric Functions of Acute Right Triangles Lesson Plan

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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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