Sections 10.3–4 Curves, Arc Length, and Acceleration Math 21a February 22, 2008 Announcements I Problem Sessions: I Monday, 8:30, SC 103b (Sophie) I Thursday, 7:30, SC 103b (Jeremy) I Office hours Tuesday, Wednesday 2–4pm SC 323.
Jul 02, 2015
Sections 10.3–4
Curves, Arc Length, and Acceleration
Math 21a
February 22, 2008
Announcements
I Problem Sessions:I Monday, 8:30, SC 103b (Sophie)I Thursday, 7:30, SC 103b (Jeremy)
I Office hours Tuesday, Wednesday 2–4pm SC 323.
Outline
Arc length
Velocity
Pythagorean length of a line segment
Given two points P1(x1, y1) and P2(x2, y2), we can use Pythagorasto find the distance between them:
x
y
P1
P2
x2 − x1
y2 − y1
|P1P2| =√
(x2 − x1)2 + (y2 − y1)2 =√
(∆x)2 + (∆y)2
Length of a curve
Break up the curve into pieces, and approximate the arc lengthwith the sum of the lengths of the pieces:
x
y
Length of a curve
Break up the curve into pieces, and approximate the arc lengthwith the sum of the lengths of the pieces:
x
y
Length of a curve
Break up the curve into pieces, and approximate the arc lengthwith the sum of the lengths of the pieces:
x
y
Length of a curve
Break up the curve into pieces, and approximate the arc lengthwith the sum of the lengths of the pieces:
x
y
Length of a curve
Break up the curve into pieces, and approximate the arc lengthwith the sum of the lengths of the pieces:
x
y
Length of a curve
Break up the curve into pieces, and approximate the arc lengthwith the sum of the lengths of the pieces:
x
y
L ≈n∑
i=1
√(∆xi )2 + (∆yi )2
Sum goes to integralIf 〈x , y〉 is given by a vector-valued function r(t) = 〈f (t), g(t), 〉with domain [a, b], we can approximate:
∆xi = f ′(ti )∆ti ∆xi = g ′(ti )∆ti
So
L ≈n∑
i=1
√(∆xi )2 + (∆yi )2 ≈
n∑i=1
√[f ′(ti )∆ti ]
2 + [g ′(ti )∆ti ]2
=n∑
i=1
√[f ′(ti )]2 + [g ′(ti )]2 ∆ti
As n→∞, this converges to
L =
∫ b
a
√[f ′(t)]2 + [g ′(t)]2 dt
In 3D, r(t) = 〈f (t), g(t), h(t)〉, and
L =
∫ b
a
√[f ′(t)]2 + [g ′(t)]2 + [h′(t)]2 dt
Sum goes to integralIf 〈x , y〉 is given by a vector-valued function r(t) = 〈f (t), g(t), 〉with domain [a, b], we can approximate:
∆xi = f ′(ti )∆ti ∆xi = g ′(ti )∆ti
So
L ≈n∑
i=1
√(∆xi )2 + (∆yi )2 ≈
n∑i=1
√[f ′(ti )∆ti ]
2 + [g ′(ti )∆ti ]2
=n∑
i=1
√[f ′(ti )]2 + [g ′(ti )]2 ∆ti
As n→∞, this converges to
L =
∫ b
a
√[f ′(t)]2 + [g ′(t)]2 dt
In 3D, r(t) = 〈f (t), g(t), h(t)〉, and
L =
∫ b
a
√[f ′(t)]2 + [g ′(t)]2 + [h′(t)]2 dt
Example
Example
Find the length of the parabola y = x2 from x = 0 to x = 1.
SolutionLet r(t) =
⟨t, t2
⟩. Then
L =
∫ 1
0
√1 + (2t)2 =
√5
2+
1
4ln∣∣∣2 +
√5∣∣∣
Example
Example
Find the length of the parabola y = x2 from x = 0 to x = 1.
SolutionLet r(t) =
⟨t, t2
⟩. Then
L =
∫ 1
0
√1 + (2t)2 =
√5
2+
1
4ln∣∣∣2 +
√5∣∣∣
Example
Find the length of the curve
r(t) = 〈2 sin t, 5t, 2 cos t〉
for −10 ≤ t ≤ 10.
AnswerL = 20
√29
Example
Find the length of the curve
r(t) = 〈2 sin t, 5t, 2 cos t〉
for −10 ≤ t ≤ 10.
AnswerL = 20
√29
Outline
Arc length
Velocity
Velocity and Acceleration
DefinitionLet r(t) be a vector-valued function.
I The velocity v(t) is the derivative r′(t)
I The speed is the length of the derivative |r′(t)|I The acceleration is the second derivative r′′(t).
Example
Find the velocity, acceleration, and speed of a particle withposition function
r(t) = 〈2 sin t, 5t, 2 cos t〉
Answer
I r′(t) = 〈2 cos(t), 5,−2 sin(t)〉I∣∣r′(t)
∣∣ =√
29
I r′′(t) = 〈−2 sin(t), 0,−2 cos(t)〉
Example
Find the velocity, acceleration, and speed of a particle withposition function
r(t) = 〈2 sin t, 5t, 2 cos t〉
Answer
I r′(t) = 〈2 cos(t), 5,−2 sin(t)〉I∣∣r′(t)
∣∣ =√
29
I r′′(t) = 〈−2 sin(t), 0,−2 cos(t)〉
Example
The position function of a particle is given by
r(t) =⟨t2, 5t, t2 − 16t
⟩When is the speed a minimum?
SolutionThe square of the speed is
(2t)2 + 52 + (2t − 16)2
which is minimized when
0 = 8t + 4(2t − 16) =⇒ t = 4
Example
The position function of a particle is given by
r(t) =⟨t2, 5t, t2 − 16t
⟩When is the speed a minimum?
SolutionThe square of the speed is
(2t)2 + 52 + (2t − 16)2
which is minimized when
0 = 8t + 4(2t − 16) =⇒ t = 4
Example
A batter hits a baseball 3 ft above the ground towards the GreenMonster in Fenway Park, which is 37 ft high and 310 ft from homeplate (down the left field foul line). The ball leaves with a speed of115 ft/s and at an angle of 50◦ above the horizontal. Is the ball ahome run, a wallball double, or is it caught by the left fielder?
SolutionThe position function is given by
r(t) =⟨115 cos(50◦)t, 3 + 115 sin(50◦)t − 16t2
⟩The question is: what is g(t) when f (t) = 310? The equation
f (t) = 310 gives t∗ =310
115 cos(50◦), so
g(t∗) = 3 + 115 sin(50◦)
(310
115 cos(50◦)
)2
− 16
(310
115 cos(50◦)
)2
≈ 91.051 ft
Home run!
SolutionThe position function is given by
r(t) =⟨115 cos(50◦)t, 3 + 115 sin(50◦)t − 16t2
⟩The question is: what is g(t) when f (t) = 310? The equation
f (t) = 310 gives t∗ =310
115 cos(50◦), so
g(t∗) = 3 + 115 sin(50◦)
(310
115 cos(50◦)
)2
− 16
(310
115 cos(50◦)
)2
≈ 91.051 ft
Home run!