
If two sides and the included angle of one triangle are congruent to
... • We need to discover which cases turn out to be congruence shortcuts and which do not. ...
... • We need to discover which cases turn out to be congruence shortcuts and which do not. ...
ROCKY FORD CURRICULUM GUIDE SUBJECT: Geometry GRADE
... Derive the formula for the area of a sector. I d. Understand similarity in terms of similarity transformations. i. Verify experimentally the properties of dilations given by a center and a scale factor. 1. Show that a dilation takes a line not passing through the center of the dilation to a parallel ...
... Derive the formula for the area of a sector. I d. Understand similarity in terms of similarity transformations. i. Verify experimentally the properties of dilations given by a center and a scale factor. 1. Show that a dilation takes a line not passing through the center of the dilation to a parallel ...
Chapter 13
... §13.1 – Trigonometric Ratios • Trigonometric ratios – Relationship between an acute angle of a right triangle and the lengths of its sides • sin A = side opposite A hypotenuse • cos A = side adjacent to A hypotenuse • tan A = side opposite A side adjacent to A ...
... §13.1 – Trigonometric Ratios • Trigonometric ratios – Relationship between an acute angle of a right triangle and the lengths of its sides • sin A = side opposite A hypotenuse • cos A = side adjacent to A hypotenuse • tan A = side opposite A side adjacent to A ...
Activity 5.2.2b Proof of the Perpendicular Bisector Theorem
... Activity 5.2.2b Proof of the Perpendicular Bisector Theorem The Perpendicular Bisector Theorems says that the locus of points that are equidistant from the endpoints of a segment is the perpendicular bisector of the segment. To prove this theorem we need to prove two things: (1) If a point lies on t ...
... Activity 5.2.2b Proof of the Perpendicular Bisector Theorem The Perpendicular Bisector Theorems says that the locus of points that are equidistant from the endpoints of a segment is the perpendicular bisector of the segment. To prove this theorem we need to prove two things: (1) If a point lies on t ...
Curriculum Units - Township of Union Public Schools
... CCSS.Math.Content.HSG-CO.B.6 Use geometric descriptions of rigid motions to transform figures and to predict the effect of a given rigid motion on a given figure; given two figures, use the definition of congruence in terms of rigid motions to decide if they are ...
... CCSS.Math.Content.HSG-CO.B.6 Use geometric descriptions of rigid motions to transform figures and to predict the effect of a given rigid motion on a given figure; given two figures, use the definition of congruence in terms of rigid motions to decide if they are ...
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.