Chapter 10 Trigonometric functions - Ugrad.math.ubc.ca
Chapter 10 Trigonometric functions - Ugrad.math.ubc.ca
Chapter 10 Trigonometric functions - Ugrad.math.ubc.ca
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Math <strong>10</strong>2 Notes <strong>Chapter</strong> <strong>10</strong><br />
1<br />
y=sin (t)<br />
0<br />
−1<br />
π/2 π 3π/2 2π 5π/2<br />
3π<br />
t<br />
period, T<br />
y=cos (t)<br />
1<br />
0<br />
π/2 π 3π/2 2π 5π/2 3π<br />
t<br />
−1<br />
period, T<br />
Figure <strong>10</strong>.5: Periodicity of the sine and cosine. Note that the two curves are just shifted versions<br />
of one another.<br />
<strong>10</strong>.4 Phase, amplitude, and frequency<br />
We have already learned how the appearance of <strong>functions</strong> changes when we shift their graph in<br />
one direction or another, s<strong>ca</strong>le one of the axes, and so on. Thus it will be easy to follow the basic<br />
changes in shape of a typi<strong>ca</strong>l trigonometric function.<br />
A function of the form<br />
y = f(t) = A sin(ωt)<br />
has both its t and y axes s<strong>ca</strong>led. The constant A, referred to as the amplitude of the graph, s<strong>ca</strong>les<br />
the y axis so that the oscillation swings between a low value of −A and a high value of A. The<br />
constant ω, <strong>ca</strong>lled the frequency, s<strong>ca</strong>les the t axis. This results in crowding together of the peaks<br />
and valleys (if ω > 1) or stretching them out (if ω < 1). One full cycle is completed when<br />
ωt = 2π<br />
and this occurs at time<br />
t = 2π ω .<br />
We will use the symbol T, to denote this special time, and we refer to T as the period. We note the<br />
connection between frequency and period:<br />
ω = 2π<br />
T ,<br />
T = 2π ω .<br />
v.2005.1 - September 4, 2009 6