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MAT01B1: Calculus with parametric curves
Dr Craig
16 October 2018
My details:
I Consulting hours:
Any time Wed, Thu or Fri except
08h30 – 11h30 Thu, 13h00 – 15h30 Thu,
10h30 – 12h30 Friday.
I Office C-Ring 508
https://andrewcraigmaths.wordpress.com/
(Or, just google ‘Andrew Craig maths’.)
Semester Test 2
I Saturday 20 October
I 09h00 B-LES 100/B-LES 101
I Scope:
4.5, 4.7, 3.9
6.1, 6.2, 6.3, 6.5
(including proof of MVT for Integrals)
8.1, 8.2
9.3, 9.5
10.1, 10.2 (up to Example 2)
Recap: last week we learned to work with
curves defined in the following way:
x = f (t) y = g(t)
These curves contain more information than
just the set of points (x, y) = (f (t), g(t)).
The additional information is the fact that a
curve is at a particular point (x′, y′) at a
particular value of t. Also, parametric curves
have direction.
Recap: sometimes we can rewrite the
equations x = f (t) and y = g(t) without
using t.
(For example: x = r cos t, y = r sin t gives
us r2 = x2 + y2.) This can sometimes make
it easier to sketch the curve.
There will also sometimes be limits on the
values of t (and hence x and y). These will
either be implicitly imposed by the domain of
f (t) and/or g(t), or explicitly stated (e.g.
0 6 t 6 2π).
Derivatives of parametric curves
The derivative of a curve
dy
dx=
dy
dtdx
dt
is defined wheneverdx
dt6= 0
Horizontal tangent whendy
dt= 0.
Vertical tangent whendx
dt= 0 and
dy
dt6= 0
Second derivatives
To get the second derivative of a
parametric curve, we differentiate the first
derivative with respect to x:
d2y
dx2=
d
dx
(dy
dx
)=
d
dt
(dy
dx
)dx
dtWe can use the second derivative to explore
the concavity of a parametric curve.
Example: consider the curve defined by
x = f (t) = t2 y = g(t) = t3 − 3t
(a) Show that the curve has two tangents at
the point (3, 0) and find their equations.
(b) Find the points (x, y) on the curve where
the tangent is horizontal or vertical.
(c) Determine where the curve is concave
upward or downward.
(d) Sketch the curve.
x = f (t) = t2 y = g(t) = t3 − 3t
Example: consider the cycloid
x = r(θ − sin θ) y = r(1− cos θ)
(a) Find the tangent at the point where
θ = π/3.
(b) At what points is the tangent horizontal?
(Give (x, y) coordinates of the points.)
(c) At what points is the tangent vertical?
Vertical tangents of the cycloid
We get vertical tangents at t = k.2π (or
x = k.2πr) for all k ∈ Z. We can see this by
calculating
limθ→k.2π+
dy
dx=∞ and lim
θ→k.2π−dy
dx= −∞
Area under a parametric curve
We are used to the following situation:
A =
∫ b
a
y dx
However, now y is no longer a function of x (it is afunction of t) so we aren’t able to find theantiderivative.
We use the fact that dxdt = f ′(t) and hence
dx = f ′(t) dt. We change the x-bounds to t-boundsby solving a = f(α) and b = f(β). Finally we have
A =
∫ β
α
g(t)f ′(t) dt
Example
Find the area under one arch of the cycloid
x = r(θ − sin θ) y = r(1− cos θ)
A = 3πr2
Example:
Find the area between the x-axis and the
parametric curve
x = 1 + et y = t− t2
Solution:
A = 3− e
Arc length from Chapter 8
If y = h(x) and a 6 x 6 b and h′(x) is
continuous, then
L =
∫ b
a
√1 +
(dy
dx
)2
dx
Now when f (α) = a and f (β) = b we have
L =
∫ β
α
√1 +
(dy
dx
)2dx
dtdt
and therefore
L =
∫ β
α
√(dx
dt
)2
+
(dy
dt
)2
dt
Theorem: If C is described by x = f (t),
y = g(t), α 6 t 6 β and f ′(t) and g′(t)
are continuous on [α, β], and C is
traversed exactly once as t increases from
α to β, then the length of C is
L =
∫ β
α
√(dx
dt
)2
+
(dy
dt
)2
dt
Arc length examples:
Find the arc length of the two curves from
last time.
(a) x = cos t, y = sin t, 0 6 t 6 2π
(b) x = sin 2t, y = cos 2t, 0 6 t 6 2π
Arc length example:
Find the length of one arch of the cycloid
x = r(θ − sin θ) y = r(1− cos θ)
Surface area
Previously, if we have y = f (x) and we
rotated a piece of that function (a 6 x 6 b)
around the x-axis, we would calculate the
surface area as follows:∫ b
a
2πf (x)√
1 + [f ′(x)]2 dx
Now suppose that we rotate a parametric
curve about the x-axis.
Surface area: for x = f (t), y = g(t),
α 6 t 6 β rotated about the x-axis (with f ′
and g′ continuous and g(t) > 0) we have
S =
∫ β
α
2πy
√(dx
dt
)2
+
(dy
dt
)2
dt
Note that we will use y = g(t) so that we
can integrate with respect to t:
S = 2π
∫ β
α
g(t)
√(dx
dt
)2
+
(dy
dt
)2
dt
Surface area
If we rotate x = f (t), y = g(t), α 6 t 6 β
about the y-axis (with f ′ and g′ continuous
and f (t) > 0) we have
S =
∫ β
α
2πf (t)
√(dx
dt
)2
+
(dy
dt
)2
dt
Example: show that the surface area of a
sphere of radius r is 4πr2. (This can be done
by rotating a semicircle either around the
x-axis or around the y-axis.)