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Math 11 Final Fall 2010
Math 11 Final Fall 2010

... 10. Definition: A function is a rule or a set of rules that pairs each number in a set called the domain with exactly one number in a set called the range. (2) 11. Domain of f = {x : 2x  10  0 and x 2  8x  7  ( x  7)( x  1)  0} = {x : x  5 and x  7} . (4) 12. f (g(x ))  f (3x  2)  2(3x ...
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... a. It’s the steepness of a road or a mountain side OR A LINE. b. It’s the ratio of change between 2 y-coordinates and 2 xcoordinates. c. In formulas and graphs, it’s the variable ‘m’. You need 2 points first. Then you can choose 1 of 2 methods: ...
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... If two angles and a non-included side of one triangle are congruent to two angles and the corresponding non-included side of another triangle then the triangles are congruent Theorem 4-3 (Isosceles Triangle Theorem) If two sides of a triangle are congruent then the angles opposite those sides are co ...
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... weight, smell, and taste. The attraction of such a viewpoint faded dramatically with the advent of non-Euclidean geometry. Toward the end of the nineteenth century, an alternative conception of what mathematicians were doing became prominent. Mathematics isn’t “about” anything. What mathematicians d ...
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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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