
Geometry Fall 2011 Lesson 29 _Proving lines parallel
... Aim: How do we prove lines are parallel? Objectives: 1) Students will be able to prove lines parallel. Note: From Lesson 27 recall the theorem - The measure of an exterior angle of a triangle is greater than the measure of either non adjacent interior angle. Do Now: Examine this proof by contradicti ...
... Aim: How do we prove lines are parallel? Objectives: 1) Students will be able to prove lines parallel. Note: From Lesson 27 recall the theorem - The measure of an exterior angle of a triangle is greater than the measure of either non adjacent interior angle. Do Now: Examine this proof by contradicti ...
Geometry Fall 2014 Lesson 030 _Proving lines parallel
... congruent, then the two lines are parallel Theorem: If two lines are perpendicular to the same line, then they are parallel. Summary of ways to prove lines parallel 1) A pair of alternate interior angles congruent 2) A pair of corresponding angles congruent 3) A pair of interior angles on the same s ...
... congruent, then the two lines are parallel Theorem: If two lines are perpendicular to the same line, then they are parallel. Summary of ways to prove lines parallel 1) A pair of alternate interior angles congruent 2) A pair of corresponding angles congruent 3) A pair of interior angles on the same s ...
Geometry Course Syllabus Cindy Kroon Course description The
... 14.1 Inscribed angles 14.2 Tangents to a circle 14.3 Secant angles 14.4 Secant-tangent angles 14.5 Segment measure 14.6 Equations of circles Instructional Philosophy: All students can and should learn geometry. A mathematical way of thinking and problem solving is important for everyone. Geometry co ...
... 14.1 Inscribed angles 14.2 Tangents to a circle 14.3 Secant angles 14.4 Secant-tangent angles 14.5 Segment measure 14.6 Equations of circles Instructional Philosophy: All students can and should learn geometry. A mathematical way of thinking and problem solving is important for everyone. Geometry co ...
1-5 Exploring Angle Pairs
... Section 1.5 – Exploring Angle Pairs AN ANGLE BISECTOR IS A RAY THAT DIVIDES AN ANGLE INTO TWO CONGRUENT ANGLES. ITS ENDPOINT IS A THE ANGLE VERTEX. WITHIN THE RAY, A SEGMENT WITH THE SAME ENDPOINT IS ALSO AN ANGLE BISECTOR. THE RAY OR SEGMENT BISECTS THE ANGLE. IN THE DIAGRAM, RAY AY IS THE ANGLE B ...
... Section 1.5 – Exploring Angle Pairs AN ANGLE BISECTOR IS A RAY THAT DIVIDES AN ANGLE INTO TWO CONGRUENT ANGLES. ITS ENDPOINT IS A THE ANGLE VERTEX. WITHIN THE RAY, A SEGMENT WITH THE SAME ENDPOINT IS ALSO AN ANGLE BISECTOR. THE RAY OR SEGMENT BISECTS THE ANGLE. IN THE DIAGRAM, RAY AY IS THE ANGLE B ...
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.