1. Trigonometric Fundamentals 51 circle centered at C with radius CA; that is, ω denotes the boundary of the base of the candle. Let B be the foot of the perpendicular line segment from D to the circle ω, and assume that ̸ OCB = θ. Because circle ω has radius 1, |ÔB|, the length of arc OB,is θ. (This is why we use radian measure for θ.) Then B 1 = (θ, 0) and D 1 = (θ, y) with y = BD. Let F be the foot of the perpendicular line segment from B to segment AC. Then CF = cos θ, and AF = 1 + cos θ. Note that A, Q, C, F , and O are coplanar, and ̸ OAQ = 45 ◦ . Point E is on segment AQ such that EF ⊥ AO. Consequently, ̸ AEF = ̸ OAQ = 45 ◦ and ̸ AFE = 90 ◦ , implying that the right triangle AEF is isosceles, with AF = EF. It is not difficult to see that BDEF is a rectangle. Hence BD = EF = AF = 1 + cos θ. We conclude that D 1 = (θ, 1 + cos θ); that is, D 1 lies on the curve y = 1 + cos x. Q1 2 1.5 D1 1 0.5 A1 -3 -2 -1 1 2 3 O1 -0.5 B1 A2 Figure 1.50. Finally, had we not cut off the bottom of the candle, the equation of the curve would have been y = 2 + cos x. Three Dimensional Coordinate Systems We view Earth as a sphere, with radius 3960 miles. We will set up two kinds of 3-D coordinate systems to describe the positions of places on Earth.
52 <strong>103</strong> <strong>Trigonometry</strong> <strong>Problems</strong> z x F B E A G C Figure 1.51. D H y The first system is the 3-D rectangular coordinate system (or Cartesian system). This is a simple generalization of the regular rectangular coordinate system in the plane (or more precisely, the xy plane). We add in the third coordinate z to describe the directed distance from a point to the xy plane. Figure 1.51 shows a rectangular box ABCDEF GH . Note that A = (0, 0, 0), and B,D, and E are on the coordinate axes. Given G = (6, 3, 2), wehaveB = (6, 0, 0), C = (6, 3, 0), D = (0, 3, 0), E = (0, 0, 2), F = (6, 0, 2), and H = (0, 3, 2). It is not difficult to see that the distance from G to the xy, yz, zx planes, x, y, z axes, and the origin are |GC| =2, |GH |=6, |GF |=3, |GB| = √ 13, |GD| =2 √ 10, |GE| =3 √ 5, and |GA| =7. It is not difficult to visualize this coordinate system. Just place yourself in a regular room, choose a corner on the floor (if you are good at seeing the world upside down, you might want to try a corner on the ceiling) as the origin, and assign the three edges going out of the chosen corner as the three axes. In general, for a point P = (x,y,z), x denotes the directed distance from P to the yzplane, y denotes the directed distance from P to the zx plane, and z denotes the directed distance from P to the xy plane. It is not difficult to see that √ x 2 + y 2 , √ y 2 + z 2 , and √ z 2 + x 2 are the respective distances from P to the z axis, x axis, and y axis. It is also not difficult to see that the distance between two points P 1 = (x 1 ,y 1 ,z 1 ) and P 2 = (x 2 ,y 2 ,z 2 ) is √ (x1 − x 2 ) 2 + (y 1 − y 2 ) 2 + (z 1 − z 2 ) 2 . Based on this generalization, we can talk about vectors in 3-D space and their lengths, and the angles formed by them when they are placed tail to tail. (Note that we cannot talk about the standard angle any more.) Hence we can easily generalize the definition of the dot product of threedimensional vectors u =[a,b,c] and v =[m, n, p] as u · v = am + bn + cp, and it is routine to check that all the properties of the dot product discussed earlier hold. Let O be the center of Earth. We set the plane containing the equator as the xy plane (or equatorial plane), and let the North Pole lie on the positive z axis. However,