page 328 - Blackboard
... the product of one secant segment and its external segment equals the product of the other secant segment and its external segment. ...
... the product of one secant segment and its external segment equals the product of the other secant segment and its external segment. ...
Definitions, Axioms, Postulates, Propositions, and Theorems from
... Note: Statements up to this point are from or form neutral geometry. Choosing Hilbert’s/Euclid’s Axiom (the two are logically equivalent) or the Hyperbolic Axiom will make the geometry Euclidean or Hyperbolic, respectively. Parallelism Axioms: Hilbert’s Parallelism Axiom for Euclidean Geometry: For ...
... Note: Statements up to this point are from or form neutral geometry. Choosing Hilbert’s/Euclid’s Axiom (the two are logically equivalent) or the Hyperbolic Axiom will make the geometry Euclidean or Hyperbolic, respectively. Parallelism Axioms: Hilbert’s Parallelism Axiom for Euclidean Geometry: For ...
Geometry Assessment Blueprint
... Use ratios of similar 3-dimensional figures to determine unknown values, such as angles, side lengths, perimeter or circumference of a face, area of a face, and volume. Models and Perspective (4.3) Create a model of a 3-dimensional figure from a 2-dimensional drawing and make a 2-dimensional represe ...
... Use ratios of similar 3-dimensional figures to determine unknown values, such as angles, side lengths, perimeter or circumference of a face, area of a face, and volume. Models and Perspective (4.3) Create a model of a 3-dimensional figure from a 2-dimensional drawing and make a 2-dimensional represe ...
MAT360 Lecture 10
... Let l be a line and let P be a point not on l. Let Q be the foot of the perpendicular from P to l. Then there are two unique rays PX and PX’ on opposite sides of PQ that do not meet l and such that a ray emanating from P intersects l if and only if it is between PX and PX’. Moreover,
... Let l be a line and let P be a point not on l. Let Q be the foot of the perpendicular from P to l. Then there are two unique rays PX and PX’ on opposite sides of PQ that do not meet l and such that a ray emanating from P intersects l if and only if it is between PX and PX’. Moreover,
Co-incidence Problems and Methods
... (1) A line is completely determined by any two points incident on it. Conversely, given any two points there is a unique line incident on both of them. (2) A point is completely determined by any two lines incident on it. The converse breaks down because of parallel lines, but is almost true – given ...
... (1) A line is completely determined by any two points incident on it. Conversely, given any two points there is a unique line incident on both of them. (2) A point is completely determined by any two lines incident on it. The converse breaks down because of parallel lines, but is almost true – given ...
Name________________________________
... 19. Write the conditional statement t s: ___________________________________________________________________________________________ 20. Write the converse of the statement in Exercise 19: ___________________________________________________________________________________________ 21. Write the bic ...
... 19. Write the conditional statement t s: ___________________________________________________________________________________________ 20. Write the converse of the statement in Exercise 19: ___________________________________________________________________________________________ 21. Write the bic ...
5 The hyperbolic plane
... of sheets. By counting vertices, edges and faces it is clear that χ(X̃) = kχ(X). Since χ(S) = 2, we must have k = 1 or 2, but if the latter χ(X) = 1 which is not of the allowable form 2 − 2g for an orientable surface and a Riemann surface is orientable. So it is only the Riemann sphere in this case. ...
... of sheets. By counting vertices, edges and faces it is clear that χ(X̃) = kχ(X). Since χ(S) = 2, we must have k = 1 or 2, but if the latter χ(X) = 1 which is not of the allowable form 2 − 2g for an orientable surface and a Riemann surface is orientable. So it is only the Riemann sphere in this case. ...
GEOMETRY--2013
... 3. To graph the ordered pairs, make sure all other graphs are turned off. To do this, hit the “y=” key on the first row and hit “clear” until all graphs have been cleared. Also, the stat plots must be turned off. To do this, hit “2nd” and “y=” and then scroll to number 4 “Plotsoff” and hit ENTER twi ...
... 3. To graph the ordered pairs, make sure all other graphs are turned off. To do this, hit the “y=” key on the first row and hit “clear” until all graphs have been cleared. Also, the stat plots must be turned off. To do this, hit “2nd” and “y=” and then scroll to number 4 “Plotsoff” and hit ENTER twi ...
Lie sphere geometry
Lie sphere geometry is a geometrical theory of planar or spatial geometry in which the fundamental concept is the circle or sphere. It was introduced by Sophus Lie in the nineteenth century. The main idea which leads to Lie sphere geometry is that lines (or planes) should be regarded as circles (or spheres) of infinite radius and that points in the plane (or space) should be regarded as circles (or spheres) of zero radius.The space of circles in the plane (or spheres in space), including points and lines (or planes) turns out to be a manifold known as the Lie quadric (a quadric hypersurface in projective space). Lie sphere geometry is the geometry of the Lie quadric and the Lie transformations which preserve it. This geometry can be difficult to visualize because Lie transformations do not preserve points in general: points can be transformed into circles (or spheres).To handle this, curves in the plane and surfaces in space are studied using their contact lifts, which are determined by their tangent spaces. This provides a natural realisation of the osculating circle to a curve, and the curvature spheres of a surface. It also allows for a natural treatment of Dupin cyclides and a conceptual solution of the problem of Apollonius.Lie sphere geometry can be defined in any dimension, but the case of the plane and 3-dimensional space are the most important. In the latter case, Lie noticed a remarkable similarity between the Lie quadric of spheres in 3-dimensions, and the space of lines in 3-dimensional projective space, which is also a quadric hypersurface in a 5-dimensional projective space, called the Plücker or Klein quadric. This similarity led Lie to his famous ""line-sphere correspondence"" between the space of lines and the space of spheres in 3-dimensional space.