Chapter 1 Topics in Analytic Geometry
Chapter 1 Topics in Analytic Geometry
Chapter 1 Topics in Analytic Geometry
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••••MA112 Section 750001: Prepared by Dr.Archara Pacheenburawana 65r 0t(r 1 −r 0 )rOr 1r = (1−t)r 0 +tr 1It is common to call (4.5) the two-po<strong>in</strong>t vector form of a l<strong>in</strong>e. It is understood<strong>in</strong> (4.5) that t varies from −∞ to +∞. However, if we restrict t to vary over the <strong>in</strong>terval0 ≤ t ≤ 1, then r will vary from r 0 to r 1 . Thus, the equationr = (1−t)r 0 +tr 1 (0 ≤ t ≤ 1) (4.6)represents the l<strong>in</strong>e segment <strong>in</strong> 2-space or 3-space that is traced from r 0 to r 1 .4.2 Calculus of Vector-Valued FunctionsIn this section we will def<strong>in</strong>e limits, derivative, and <strong>in</strong>tegral of vector-valued functions.Limits and Cont<strong>in</strong>uityOur first goal <strong>in</strong> this section is to develop a notion of what it means for a vector-valuedfunction r(t) <strong>in</strong> 2-space or 3-space to approach a limit<strong>in</strong>g vector ̷L ar t approaches a numbera. That is, we want to def<strong>in</strong>elimr(t) = ̷L (4.7)t→aDef<strong>in</strong>ition 4.1 Let r(t) be a vector-valued function that is def<strong>in</strong>ed for all t <strong>in</strong> some open<strong>in</strong>terval conta<strong>in</strong><strong>in</strong>g the number a, except that r(t) need not be def<strong>in</strong>ed at a. We will writelimr(t) = ̷Lt→aif and only ifTheorem 4.1lim‖r(t)− ̷L‖ = 0t→a(a) If r(t) = 〈x(t),y(t)〉 = x(t)i+y(t)j, thenlimr(t) =t→a〈limt→ax(t),limt→ay(t)〉= limt→ax(t)i+limt→ay(t)jprovided the limits of the component functions exist. Conversely, the limits of thecomponent functions exist provided r(t) approaches a limit<strong>in</strong>g vector as t approachesa.