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Chapter 1 Topics in Analytic Geometry

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MA112 Section 750001: Prepared by Dr.Archara Pacheenburawana 32• If k < 0, the equation is not satisfied by any values of x, y, and z, so it has no graph.Theorem 3.1 An equation of the formx 2 +y 2 +z 2 +Gx+Hy +Iz +J = 0represents a sphere, a po<strong>in</strong>t, or has no graph.Cyl<strong>in</strong>drical SurfacesTheorem 3.2 An equation that conta<strong>in</strong>s only two of the variables x, y, and z represents acyl<strong>in</strong>drical surface <strong>in</strong> an xyz-coord<strong>in</strong>ate system. The surface can be obta<strong>in</strong>ed by graph<strong>in</strong>gthe equation <strong>in</strong> the coord<strong>in</strong>ate plane of the two variables that appear <strong>in</strong> the equation andthen translat<strong>in</strong>g that graph parallel to the axis of the miss<strong>in</strong>g variable.Example 3.3 Sketch the graph of x 2 +z 2 = 1 <strong>in</strong> 3-space.Solution .........Example 3.4 Sketch the graph of z = s<strong>in</strong>y <strong>in</strong>3-space.Solution .........3.2 VectorsMany physical quantities such as area, length, mass, and temperature are completely describedonce the magnitude of the quantity is given. Such quantities are called scalar.Other physical quantities, called vectors are not completely determ<strong>in</strong>ed until both magnitudeand a direction are specified.Vectors can be represented geometrically by arrows <strong>in</strong> 2-space or 3-space: the directionof the arrow specifies the direction of the vector and the length of the arrow describes itsmagnitude. The tail of the arrow is called the the <strong>in</strong>itial po<strong>in</strong>t of the vector, and the tipof the arrow the term<strong>in</strong>al po<strong>in</strong>t.We will denote vectors with lowercase boldface type such as a, k, v, w, and x. Whendiscuss<strong>in</strong>g vectors, we will refer to real numbers as scalars. Scalar will be denoted bylowercase italic type such as a, k, w, and x.Two vectors, v and w, are considered to be equal (also called equivalent) if theyhave the same length and same direction, <strong>in</strong> which case we write v = w. Geometrically,two vectors are equal if they are translations of one another; thus, the three vectors <strong>in</strong> thefollow<strong>in</strong>g figure are equal, even though they are <strong>in</strong> different positions.

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