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A p p e n d i x A : U s e f u l M a t h 719<br />

tanα = a b<br />

or a = b tanβ (A.4.3e)<br />

tanβ = b a<br />

or b = a tanβ (A.4.3f)<br />

Substituting in Eqs. (A.4.1), (A.4.3a), and (A.4.3.c), we can say:<br />

h 2 = a 2 + b 2 = h 2 sin<br />

2 α + h<br />

2 cos<br />

2 α<br />

(A.4.4)<br />

or<br />

2 2<br />

1 = sin α + cos α (A.4.5)<br />

Suppose we draw a circle to represent the rotation of a chair on a Ferris wheel. Inside<br />

that circle we draw a right triangle whose hypotenuse is equal to the radius of the<br />

circle and is connected to the chair at one end, as shown in Fig. A.4.3. As the chair travels<br />

the circumference of the circle, the right triangle we draw at each instant is a different<br />

shape but we can always draw a right triangle. Because h, the hypotenuse, is equal<br />

to the radius of the circle traversed by the chair, it is always constant. But sides a and b<br />

are always changing. As an example: When the chair reaches the top of the Ferris wheel,<br />

side b of the right triangle goes to 0 and side a is the same length as the hypotenuse h.<br />

At that point, sin a = 0 and cos a = 1, agreeing with Eq. (A.4.5).<br />

h'<br />

a'<br />

a''<br />

b''<br />

h''<br />

b'<br />

h<br />

b<br />

a<br />

Figure A.4.3 Circular motion and the right triangle.

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