In the equation, y=tan(kθ)y=tan(kθ), kk is a constant and has different effects on the graph of the function. The general shape of the graph of functions of this form is shown in Figure 7 for the function f(θ)=tan(2θ)f(θ)=tan(2θ).
On the same set of axes, plot the following graphs:
-
a
(
θ
)
=
tan
0
,
5
θ
a
(
θ
)
=
tan
0
,
5
θ
-
b
(
θ
)
=
tan
1
θ
b
(
θ
)
=
tan
1
θ
-
c
(
θ
)
=
tan
1
,
5
θ
c
(
θ
)
=
tan
1
,
5
θ
-
d
(
θ
)
=
tan
2
θ
d
(
θ
)
=
tan
2
θ
-
e
(
θ
)
=
tan
2
,
5
θ
e
(
θ
)
=
tan
2
,
5
θ
Use your results to deduce the effect of kk.
You should have found that, once again, the value of kk affects the periodicity (i.e. frequency) of the graph. As kk increases, the graph is more tightly packed. As kk decreases, the graph is more spread out. The period of the tan graph is given by 180∘k180∘k.
These different properties are summarised in Table 3.
Table 3: Table summarising general shapes and positions of graphs of functions of the form y=tan(kθ)y=tan(kθ).
|
k
>
0
k
>
0
|
k
<
0
k
<
0
|
|
|
|
For f(θ)=tan(kθ)f(θ)=tan(kθ), the domain of one branch is {θ:θ∈(-90∘k,90∘k)}{θ:θ∈(-90∘k,90∘k)} because the function is undefined for θ=-90∘kθ=-90∘k and θ=90∘kθ=90∘k.
The range of f(θ)=tan(kθ)f(θ)=tan(kθ) is {f(θ):f(θ)∈(-∞,∞)}{f(θ):f(θ)∈(-∞,∞)}.
For functions of the form, y=tan(kθ)y=tan(kθ), the details of calculating the intercepts with the xx and yy axis are given.
There are many xx-intercepts; each one is halfway between the asymptotes.
The yy-intercept is calculated as follows:
y
=
tan
(
k
θ
)
y
i
n
t
=
tan
(
0
)
=
0
y
=
tan
(
k
θ
)
y
i
n
t
=
tan
(
0
)
=
0
(3)The graph of tankθtankθ has asymptotes because as kθkθ approaches 90∘90∘, tankθtankθ approaches infinity. In other words, there is no defined value of the function at the asymptote values.
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