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 45Moreover, if we assume that the object moves along a l<strong>in</strong>e from po<strong>in</strong>t P to po<strong>in</strong>t Q, thend = ‖ −→ PQ‖, so that the work can be expressed entirely <strong>in</strong> vector form asW = ‖F‖‖ −→ PQ‖The vector −→ PQ is called the displacement vector for the object.In the case where a constant force F is not <strong>in</strong> the direction of motion, but rather makesan angle θ with the displacement vector, then we def<strong>in</strong>e the work W done by F to beW = (‖F‖cosθ)‖ −→ PQ‖ = F·−→ PQ (3.13)•P‖F‖FWork = ‖F‖‖ −→ PQ‖•Q•P‖F‖Fθ‖F‖cosθWork = (‖F‖cosθ)‖ −→ PQ‖•QExample 3.19 A force F = 8i + 5j <strong>in</strong> pound moves an object from P(1,0) to Q(7,1),distance measured <strong>in</strong> feet. How much work is done?Solution .........Example 3.20 A wagon is pulled horizontally by exert<strong>in</strong>g a constant force of 10lb on thehandle at an angle of 60 ◦ with the horizontal. How much work is done <strong>in</strong> mov<strong>in</strong>g the wagon50 ft?Solution .........3.4 Cross ProductDeterm<strong>in</strong>antsBefore we def<strong>in</strong>e the cross product, we need to def<strong>in</strong>e the notion of determ<strong>in</strong>ant.Def<strong>in</strong>ition 3.4 The determ<strong>in</strong>ant of a 2×2 matrix of real number is def<strong>in</strong>ed by∣ a ∣1 a 2∣∣∣= ab 1 b 1 b 2 −a 2 b 1 .2Def<strong>in</strong>ition 3.5 The determ<strong>in</strong>ant of a 3×3 matrix of real number is def<strong>in</strong>ed as a comb<strong>in</strong>ationof three 2×2 determ<strong>in</strong>ants, as follows:∣ a 1 a 2 a 3∣∣∣∣∣∣ ∣ ∣ ∣ ∣ ∣ ∣∣∣ b b 1 b 2 b 3 = a 2 b 3∣∣∣∣∣∣ b1 −a 1 b 3∣∣∣∣∣∣ b∣ cc 1 c 2 c 2 c 2 +a 1 b 2∣∣∣3 c 1 c 3 (3.14)3 c 1 c 23Note that Equation (3.14) is referred to as an expansion of the determ<strong>in</strong>ant alongthe first row.