Multivariate Calculus - Bruce E. Shapiro

Multivariate Calculus - Bruce E. Shapiro Multivariate Calculus - Bruce E. Shapiro

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28 LECTURE 3. THE CROSS PRODUCT Example 3.6 Find the equation of the plane through (2, −3, 2) and parallel to the plane containing the vectors v = 4i + 3j − k, w = 2i − 5j + 6k. Solution.The normal to the desired plane will also be perpendicular to the plane containing v and w. Since the cross product of any two vectors is by definition perpendicular to the plane containing both vectors, then one such normal vector is i j k n = v × w = 4 3 −1 ∣2 −5 6 ∣ = i ∣ 3 −1 ∣ ∣ ∣∣∣ −5 6 ∣ − j 4 −1 ∣∣∣ 2 6 ∣ + k 4 3 2 −5∣ = 13i − 26j − 26k Since a point on the plane is (2,-3,2), the equation of the plane is n · (x, y, z) = n · P (13, −26, −26) · (x, y, z) = (13, −26, −26) · (2, −3, 2) 13x − 26y − 26z = 52 Dividing the last equation through by 13 gives x − 2y − 2z = 4 as the equation of the desired plane. Revised December 6, 2006. Math 250, Fall 2006

Lecture 4 Lines and Curves in 3D We can parameterize a curve in three dimensions in the same way that we did in two dimensions, associating a function with each of the three coordinates, x = f(t), y = g(t), z = h(t) (4.1) where t is allowed to vary over some interval that we will call I. It is useful to envision yourself as moving along the curve from one end to the other. At any time t, you are at a point (x, y, z) on the curve. We think of the parameter t as time and then x = f(t) is your x-coordinate at time t y = g(t)is your y-coordinate at time t z = h(t) is your z-coordinate at time t. Figure 4.1: A path can be parameterized by its coordinates. We define our position vector r(t) at any time t as the vector pointing from the origin to our position (x, y, z) at the time t. This vector is then a function of t and is given by r(t) = (x(t), y(t), z(t)) = f(t)i + g(t)j + h(t)k (4.2) Suppose that we walk along a straight line, as illustrated in figure 4.3, starting at the point P 0 , at a time t = 0, and arrive at the point P at time t, moving with a 29

Lecture 4<br />

Lines and Curves in 3D<br />

We can parameterize a curve in three dimensions in the same way that we did in<br />

two dimensions, associating a function with each of the three coordinates,<br />

x = f(t), y = g(t), z = h(t) (4.1)<br />

where t is allowed to vary over some interval that we will call I. It is useful to<br />

envision yourself as moving along the curve from one end to the other. At any time<br />

t, you are at a point (x, y, z) on the curve. We think of the parameter t as time and<br />

then<br />

x = f(t) is your x-coordinate at time t<br />

y = g(t)is your y-coordinate at time t<br />

z = h(t) is your z-coordinate at time t.<br />

Figure 4.1: A path can be parameterized by its coordinates.<br />

We define our position vector r(t) at any time t as the vector pointing from<br />

the origin to our position (x, y, z) at the time t. This vector is then a function of t<br />

and is given by<br />

r(t) = (x(t), y(t), z(t)) = f(t)i + g(t)j + h(t)k (4.2)<br />

Suppose that we walk along a straight line, as illustrated in figure 4.3, starting at<br />

the point P 0 , at a time t = 0, and arrive at the point P at time t, moving with a<br />

29

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