Tangents of Parametric Curves

Jim Lambers
MAT 169
Fall Semester 2009-10
Lecture 32 Notes
These notes correspond to Section 9.2 in the text.
Tangents of Parametric Curves
When a curve is described by an equation of the form 𝑦 = 𝑓 (π‘₯), we know that the slope of the
tangent line of the curve at the point (π‘₯0 , 𝑦0 ) = (π‘₯0 , 𝑓 (π‘₯0 )) is given by
𝑑𝑦
= 𝑓 β€² (π‘₯).
𝑑π‘₯
However, if the curve is defined by parametric equations
π‘₯ = 𝑓 (𝑑),
𝑦 = 𝑔(𝑑),
then we may not have a description of the curve as a function of π‘₯ in order to compute the slope
of the tangent line in this way. Instead, we apply the Chain Rule to obtain
𝑑𝑦
𝑑𝑦 𝑑π‘₯
=
.
𝑑𝑑
𝑑π‘₯ 𝑑𝑑
Solving for 𝑑𝑦/𝑑π‘₯ yields
𝑑𝑦
=
𝑑π‘₯
𝑑𝑦
𝑑𝑑
𝑑π‘₯
𝑑𝑑
.
This allows us to express 𝑑𝑦/𝑑π‘₯ as a function of the parameter 𝑑.
Example The slope of the tangent to the spiraling curve defined by
π‘₯ = 𝑑 sin 𝑑,
𝑦 = 𝑑 cos 𝑑,
which is shown in the Lecture 31 notes, is given by
𝑑𝑦
=
𝑑π‘₯
𝑑𝑦
𝑑𝑑
𝑑π‘₯
𝑑𝑑
=
cos 𝑑 βˆ’ 𝑑 sin 𝑑
.
sin 𝑑 + 𝑑 cos 𝑑
At the point (πœ‹/2, 0), which corresponds to 𝑑 = πœ‹/2, the slope of the tangent is
π‘š=
cos πœ‹2 βˆ’ πœ‹2 sin πœ‹2
0βˆ’
πœ‹
πœ‹
πœ‹ =
sin 2 + 2 cos 2
1+
1
πœ‹
2
πœ‹
2
β‹…1
πœ‹
=βˆ’ .
β‹…0
2
From the point-slope form of the equation of a line, we see the equation of the tangent line of the
curve at this point is given by
πœ‹(
πœ‹)
π‘¦βˆ’0=βˆ’
π‘₯βˆ’
.
2
2
β–‘
We know that a curve defined by the equation 𝑦 = 𝑓 (π‘₯) has a horizontal tangent if 𝑑𝑦/𝑑π‘₯ = 0,
and a vertical tangent if 𝑓 β€² (π‘₯) has a vertical asymptote. For parametric curves, we also can identify
a horizontal tangent by determining where 𝑑𝑦/𝑑π‘₯ = 0. This is the case whenever 𝑑𝑦/𝑑𝑑 = 0,
provided that 𝑑π‘₯/𝑑𝑑 = 0, thus excluding the case where 𝑑𝑦/𝑑π‘₯ is the indeterminate form 0/0.
Similarly, the tangent line is vertical whenever 𝑑π‘₯/𝑑𝑑 = 0, but 𝑑𝑦/𝑑𝑑 βˆ•= 0.
Example Consider the unit circle, which can be parametrized by the equations
π‘₯ = cos 𝑑,
𝑦 = sin 𝑑,
0 ≀ 𝑑 < 2πœ‹.
The slope of the tangent at any point on the circle is given by
𝑑𝑦
=
𝑑π‘₯
𝑑𝑦
𝑑𝑑
𝑑π‘₯
𝑑𝑑
=
cos 𝑑
= βˆ’ cot 𝑑.
βˆ’ sin 𝑑
A horizontal tangent occurs whenever cos 𝑑 = 0, and sin 𝑑 βˆ•= 0. This is the case whenever 𝑑 = πœ‹/2
or 𝑑 = 3πœ‹/2. Substituting these parameter values into the parametric equations, we see that the
circle has two horizontal tangents, at the points (0, 1) and (0, βˆ’1).
A vertical tangent occurs whenever sin 𝑑 = 0, and cos 𝑑 βˆ•= 0. This is the case whenever 𝑑 = 0 or
𝑑 = πœ‹. Substituting these parameter values into the parametric equations, we see that the circle
has two vertical tangents, at the points (1, 0) and (βˆ’1, 0). β–‘
It is important to note that unlike a curve defined by 𝑦 = 𝑓 (π‘₯), a point on the curve may have
more than one tangent line, because a parametric curve is allowed to intersect itself.
Example Consider the curve defined by the parametric equations
π‘₯ = 𝑑2 ,
𝑦 = (𝑑2 βˆ’ 4) sin 𝑑.
This curve has two tangents at the point (πœ‹ 2 , 0). To see this, we first note that π‘₯ = 𝑑2 = πœ‹ when
√
𝑑 = ± πœ‹. Substituting these values into the equation for 𝑦, we obtain 𝑦 = 0, since sin 𝑑 = 0 when
𝑑 = ±πœ‹. Therefore, there are two distinct parameter values corresponding to this point on the
curve.
Next, we must compute 𝑑𝑦/𝑑π‘₯ for both values of 𝑑. We have
𝑑𝑦
=
𝑑π‘₯
𝑑𝑦
𝑑𝑑
𝑑π‘₯
𝑑𝑑
=
𝑑2 βˆ’ 4
(𝑑2 βˆ’ 4) cos 𝑑 + 2𝑑 sin 𝑑
= sin 𝑑 +
cos 𝑑.
2𝑑
𝑑
2
Substituting 𝑑 = βˆ’πœ‹ yields
𝑑𝑦
(βˆ’πœ‹)2 βˆ’ 4
πœ‹2 βˆ’ 4
= sin(βˆ’πœ‹) +
cos(βˆ’πœ‹) =
β‰ˆ 1.8684.
𝑑π‘₯
βˆ’πœ‹
πœ‹
On the other hand, substituting 𝑑 = πœ‹ yields
𝑑𝑦
πœ‹2 βˆ’ 4
πœ‹2 βˆ’ 4
= sin πœ‹ +
cos πœ‹ = βˆ’
β‰ˆ βˆ’1.8684.
𝑑π‘₯
πœ‹
πœ‹
The curve is illustrated in Figure 1. β–‘
Figure 1: Graph of the parametric curve π‘₯ = 𝑑2 , 𝑦 = (𝑑2 βˆ’ 4) sin 𝑑.
In order to graph curves, it is helpful to know where the curve is concave up or concave down. For
a curve defined by 𝑦 = 𝑓 (π‘₯), this is determined by computing its second derivative 𝑑2 𝑦/𝑑π‘₯2 = 𝑓 β€²β€² (π‘₯)
and checking its sign. For a parametric curve, we can compute 𝑑2 𝑦/𝑑π‘₯2 in the same way as 𝑑𝑦/𝑑π‘₯,
by using the Chain Rule. First, we note that
( )
𝑑2 𝑦
𝑑 𝑑𝑦
=
.
𝑑π‘₯2
𝑑π‘₯ 𝑑π‘₯
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Then, from the Chain Rule,
𝑑
𝑑𝑑
(
𝑑𝑦
𝑑π‘₯
)
𝑑
=
𝑑π‘₯
(
𝑑𝑦
𝑑π‘₯
)
𝑑π‘₯
𝑑2 𝑦 𝑑π‘₯
= 2 .
𝑑𝑑
𝑑π‘₯ 𝑑𝑑
Solving for 𝑑2 𝑦/𝑑π‘₯2 yields
𝑑2 𝑦
𝑑π‘₯2
=
𝑑
𝑑π‘₯
(
𝑑𝑦
𝑑π‘₯
𝑑π‘₯
𝑑𝑑
)
.
To use this formula, one first computes 𝑑𝑦/𝑑π‘₯ in terms of 𝑑𝑦/𝑑𝑑 and 𝑑π‘₯/𝑑𝑑, as described above.
Then, 𝑑𝑦/𝑑π‘₯ is a function of 𝑑, which can be differentiated with respect to 𝑑 in the usual way, before
being divided by 𝑑π‘₯/𝑑𝑑 to obtain 𝑑2 𝑦/𝑑π‘₯2 .
It is possible to obtain a formula for 𝑑2 𝑦/𝑑π‘₯2 that uses only derivatives of π‘₯ and 𝑦 with respect
to 𝑑. By applying the Quotient Rule to differentiate 𝑑𝑦/𝑑π‘₯ with respect to 𝑑, we obtain
𝑑2 𝑦
=
𝑑π‘₯2
𝑑π‘₯ 𝑑2 𝑦
𝑑𝑑 𝑑𝑑2
2
𝑑 π‘₯
βˆ’ 𝑑𝑦
𝑑𝑑 𝑑𝑑2
,
( 𝑑π‘₯ )3
𝑑𝑑
although the first formula may be easier to remember.
Example Consider the astroid, illustrated in the Lecture defined by the parametric equations
π‘₯ = cos3 𝑑,
𝑦 = sin3 𝑑,
0 ≀ 𝑑 < 2πœ‹.
This curve is illustrated in Figure 2. To determine where the curve is concave up or concave down,
we first compute 𝑑𝑦/𝑑π‘₯ as a function of 𝑑:
𝑑𝑦
=
𝑑π‘₯
𝑑𝑦
𝑑𝑑
𝑑π‘₯
𝑑𝑑
=
3 sin2 𝑑 cos 𝑑
= βˆ’ tan 𝑑.
βˆ’3 cos2 𝑑 sin 𝑑
Next, we use this to compute 𝑑2 𝑦/𝑑π‘₯2 :
( )
𝑑𝑦
𝑑
2
𝑑𝑑 𝑑π‘₯
𝑑 𝑦
βˆ’ sec2 𝑑
1
=
=
=
.
2
2
4
𝑑π‘₯
𝑑π‘₯
βˆ’3 cos 𝑑 sin 𝑑
3 cos 𝑑 sin 𝑑
𝑑𝑑
We conclude that the astroid is concave up whenever sin 𝑑 > 0, which is the case when 𝑦 > 0. It is
concave down whenever sin 𝑑 < 0, which is the case whenever 𝑦 < 0. β–‘
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Figure 2: Graph of the astroid π‘₯ = cos3 𝑑, 𝑦 = sin3 𝑑, for 0 ≀ 𝑑 < 2πœ‹.
Areas Under Parametric Curves
Recall that the area 𝐴 of the region bounded by the curve 𝑦 = 𝐹 (π‘₯), the vertical lines π‘₯ = π‘Ž and
π‘₯ = 𝑏, and the π‘₯-axis is given by the integral
∫
𝐴=
𝑏
𝐹 (π‘₯) 𝑑π‘₯.
π‘Ž
Now, suppose that the curve 𝑦 = 𝐹 (π‘₯) is also defined by the parametric equations π‘₯ = 𝑓 (𝑑),
𝑦 = 𝑔(𝑑), for 𝛼 ≀ 𝑑 ≀ 𝛽. Furthermore, suppose that 𝑓 (𝛼) = π‘Ž and 𝑓 (𝛼) = 𝑏. If the curve is
traversed only once as 𝑑 increases from 𝛼 to 𝛽, then the area can also be computed by integrating
with respect to 𝑑 as follows:
∫
𝐴=
𝑏
∫
𝛽
𝐹 (π‘₯) 𝑑π‘₯ =
π‘Ž
𝛼
5
𝑔(𝑑)𝑓 β€² (𝑑) 𝑑𝑑.
On the other hand, if 𝑑 = 𝛼 corresponds to the right endpoint of the curve, and 𝑑 = 𝛽 corresponds
to the left endpoint, then limits of integration must be reversed:
∫
𝛼
∫
β€²
𝛽
𝑔(𝑑)𝑓 (𝑑) 𝑑𝑑 = βˆ’
𝐴=
𝑔(𝑑)𝑓 β€² (𝑑) 𝑑𝑑.
𝛼
𝛽
Example The upper half-circle with center (0, 0) and radius 1 can be defined by the parametric
equations π‘₯ = cos 𝑑, 𝑦 = sin 𝑑, for 0 ≀ 𝑑 ≀ πœ‹. Because 𝑑 = 0 corresponds to the right endpoint of
this curve, and 𝑑 = πœ‹ corresponds to the left endpoint, the area bounded by the upper half-circle
and the π‘₯-axis is given by
∫ 0
∫ 0
∫ πœ‹
∫ πœ‹
1 βˆ’ cos 2𝑑
πœ‹
𝑑
sin 2𝑑 πœ‹
2
2
𝐴=
sin 𝑑(βˆ’ sin 𝑑) 𝑑𝑑 =
βˆ’ sin 𝑑 𝑑𝑑 =
sin 𝑑 𝑑𝑑 =
= ,
𝑑𝑑 = βˆ’
2
2
4 0
2
πœ‹
πœ‹
0
0
which, as expected, is half of the area of the circle. β–‘
6
Summary
βˆ™ The slope of the tangent line of a parametric curve defined by parametric equations π‘₯ = 𝑓 (𝑑),
𝑦 = 𝑔(𝑑) is given by 𝑑𝑦/𝑑π‘₯ = (𝑑𝑦/𝑑𝑑)/(𝑑π‘₯/𝑑𝑑).
βˆ™ A parametric curve has a horizontal tangent wherever 𝑑𝑦/𝑑𝑑 = 0 and 𝑑π‘₯/𝑑𝑑 βˆ•= 0. It has a
vertical tangent wherever 𝑑π‘₯/𝑑𝑑 = 0 and 𝑑𝑦/𝑑𝑑 βˆ•= 0.
βˆ™ The concavity of a parametric curve at a point can be determined by computing 𝑑2 𝑦/𝑑π‘₯2 =
𝑑(𝑑𝑦/𝑑π‘₯)/𝑑𝑑/(𝑑π‘₯/𝑑𝑑), where 𝑑𝑦/𝑑𝑑 is best represented as a function of 𝑑, not π‘₯. The curve is
concave up when 𝑑2 𝑦/𝑑π‘₯2 is positive, and concave down if it is negative.
βˆ™ A parametric curve π‘₯ = 𝑓 (𝑑), 𝑦 = 𝑔(𝑑) can have two tangents at a point (π‘₯0 , 𝑦0 ) on its graph,
if there are two distinct values of the parameter 𝑑, 𝑑1 and 𝑑2 , such that 𝑓 (𝑑1 ) = 𝑓 (𝑑2 ) = π‘₯0
and 𝑔(𝑑1 ) = 𝑔(𝑑2 ) = 𝑦0 .
βˆ™ The area of the region bounded by the parametric curve π‘₯ = 𝑓 (𝑑), 𝑦 = 𝑔(𝑑), the π‘₯-axis, the
line π‘₯ = π‘Ž, and the line π‘₯ = 𝑏, where 𝑓 (𝛼) = π‘Ž and 𝑔(𝛽) = 𝑏, is the integral from 𝛼 to 𝛽 of
𝑔(𝑑)𝑓 β€² (𝑑) 𝑑𝑑, provided that the curve is only traversed once as 𝑑 increases from 𝛼 to 𝛽.
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