Tangents of Parametric Curves

advertisement
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 ′ (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 − 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 − πœ‹2 sin πœ‹2
0−
πœ‹
πœ‹
πœ‹ =
sin 2 + 2 cos 2
1+
1
πœ‹
2
πœ‹
2
⋅1
πœ‹
=− .
⋅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‹)
𝑦−0=−
π‘₯−
.
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 ′ (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
= − cot 𝑑.
− 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, −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 (−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 − 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 − 4
(𝑑2 − 4) cos 𝑑 + 2𝑑 sin 𝑑
= sin 𝑑 +
cos 𝑑.
2𝑑
𝑑
2
Substituting 𝑑 = −πœ‹ yields
𝑑𝑦
(−πœ‹)2 − 4
πœ‹2 − 4
= sin(−πœ‹) +
cos(−πœ‹) =
≈ 1.8684.
𝑑π‘₯
−πœ‹
πœ‹
On the other hand, substituting 𝑑 = πœ‹ yields
𝑑𝑦
πœ‹2 − 4
πœ‹2 − 4
= sin πœ‹ +
cos πœ‹ = −
≈ −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 − 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 ′′ (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‘₯
3
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‘₯
− 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
= − tan 𝑑.
−3 cos2 𝑑 sin 𝑑
Next, we use this to compute 𝑑2 𝑦/𝑑π‘₯2 :
( )
𝑑𝑦
𝑑
2
𝑑𝑑 𝑑π‘₯
𝑑 𝑦
− sec2 𝑑
1
=
=
=
.
2
2
4
𝑑π‘₯
𝑑π‘₯
−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–‘
4
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 ′ (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
𝑔(𝑑)𝑓 (𝑑) 𝑑𝑑 = −
𝐴=
𝑔(𝑑)𝑓 ′ (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 − cos 2𝑑
πœ‹
𝑑
sin 2𝑑 πœ‹
2
2
𝐴=
sin 𝑑(− sin 𝑑) 𝑑𝑑 =
− sin 𝑑 𝑑𝑑 =
sin 𝑑 𝑑𝑑 =
= ,
𝑑𝑑 = −
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 ′ (𝑑) 𝑑𝑑, provided that the curve is only traversed once as 𝑑 increases from 𝛼 to 𝛽.
7
Download