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Glossary Terms * Chapter 3
Glossary Terms * Chapter 3

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... Students will understand: Proving triangles congruent using SSS, SAS, ASA and AAS. They will write proofs as 2 column, and possible flow and coordinate proofs. They will classify triangles according to angles or sides and apply the Angle Sum Theorem and the Exterior Angle Theorem. Students will use ...
student objectives (competencies/outcomes)
student objectives (competencies/outcomes)

... Students will understand: Proving triangles congruent using SSS, SAS, ASA and AAS. They will write proofs as 2 column, and possible flow and coordinate proofs. They will classify triangles according to angles or sides and apply the Angle Sum Theorem and the Exterior Angle Theorem. Students will use ...
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... If there is a line and a point not on the line, then there is exactly one line through the point parallel to the given line. Perpendicular Postulate If there is a line and a point not on the line, then there is exactly one line through the point perpendicular to the given line. Corresponding Angles ...
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... charge is at z ¼ 0 and at z ¼ 1.6 In other words, if we interpret U as a function of the charge’s position z, then Uð0Þ ¼ Uð1Þ. The existence of a repulsive regime follows immediately from the equality Uð0Þ ¼ Uð1Þ: UðzÞ must vary nonmonotonically between z ¼ 0 and z ¼ 1 and in particular must be dec ...
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... By the end of this lesson, you should be able to 1. Recognize and apply relationships between sides and angles in a triangle. 2. Apply the Triangle Inequality Theorem We learned previously that if sides in a triangle were congruent, then the angles opposite those sides are also congruent (and vice-v ...
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Noether's theorem



Noether's (first) theorem states that every differentiable symmetry of the action of a physical system has a corresponding conservation law. The theorem was proven by German mathematician Emmy Noether in 1915 and published in 1918. The action of a physical system is the integral over time of a Lagrangian function (which may or may not be an integral over space of a Lagrangian density function), from which the system's behavior can be determined by the principle of least action.Noether's theorem has become a fundamental tool of modern theoretical physics and the calculus of variations. A generalization of the seminal formulations on constants of motion in Lagrangian and Hamiltonian mechanics (developed in 1788 and 1833, respectively), it does not apply to systems that cannot be modeled with a Lagrangian alone (e.g. systems with a Rayleigh dissipation function). In particular, dissipative systems with continuous symmetries need not have a corresponding conservation law.
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