This document contains lecture notes on the fundamental theorem of calculus from a Calculus I class. The notes discuss:
1) The first and second fundamental theorems of calculus, which relate differentiation and integration as inverse processes.
2) How to use the first fundamental theorem to differentiate functions defined by integrals.
3) Biographies of several mathematicians involved in the development of calculus, including Newton, Leibniz, Gregory and Barrow.
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Lesson 26: The Fundamental Theorem of Calculus (Section 041 handout)
1. V63.0121.041, Calculus I Section 5.4 : The Fundamental Theorem December 8, 2010
Section 5.4
Notes
The Fundamental Theorem of Calculus
V63.0121.041, Calculus I
New York University
December 8, 2010
Announcements
Today: Section 5.4
Monday, December 13: Section 5.5
”Monday,” December 15: Review and Movie Day!
Monday, December 20, 12:00–1:50pm: Final Exam (location still
TBD)
Announcements
Notes
Today: Section 5.4
Monday, December 13:
Section 5.5
”Monday,” December 15:
Review and Movie Day!
Monday, December 20,
12:00–1:50pm: Final Exam
(location still TBD)
V63.0121.041, Calculus I (NYU) Section 5.4 The Fundamental Theorem December 8, 2010 2 / 33
Objectives
Notes
State and explain the
Fundemental Theorems of
Calculus
Use the first fundamental
theorem of calculus to find
derivatives of functions
defined as integrals.
Compute the average value
of an integrable function
over a closed interval.
V63.0121.041, Calculus I (NYU) Section 5.4 The Fundamental Theorem December 8, 2010 3 / 33
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2. V63.0121.041, Calculus I Section 5.4 : The Fundamental Theorem December 8, 2010
Outline
Notes
Recall: The Evaluation Theorem a/k/a 2nd FTC
The First Fundamental Theorem of Calculus
The Area Function
Statement and proof of 1FTC
Biographies
Differentiation of functions defined by integrals
“Contrived” examples
Erf
Other applications
V63.0121.041, Calculus I (NYU) Section 5.4 The Fundamental Theorem December 8, 2010 4 / 33
The definite integral as a limit
Notes
Definition
If f is a function defined on [a, b], the definite integral of f from a to b
is the number
b n
f (x) dx = lim f (ci ) ∆x
a ∆x→0
i=1
V63.0121.041, Calculus I (NYU) Section 5.4 The Fundamental Theorem December 8, 2010 5 / 33
Big time Theorem
Notes
Theorem (The Second Fundamental Theorem of Calculus)
Suppose f is integrable on [a, b] and f = F for another function F , then
b
f (x) dx = F (b) − F (a).
a
V63.0121.041, Calculus I (NYU) Section 5.4 The Fundamental Theorem December 8, 2010 6 / 33
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3. V63.0121.041, Calculus I Section 5.4 : The Fundamental Theorem December 8, 2010
The Integral as Total Change
Notes
Another way to state this theorem is:
b
F (x) dx = F (b) − F (a),
a
or the integral of a derivative along an interval is the total change between
the sides of that interval. This has many ramifications:
Theorem
If v (t) represents the velocity of a particle moving rectilinearly, then
t1
v (t) dt = s(t1 ) − s(t0 ).
t0
V63.0121.041, Calculus I (NYU) Section 5.4 The Fundamental Theorem December 8, 2010 7 / 33
The Integral as Total Change
Notes
Another way to state this theorem is:
b
F (x) dx = F (b) − F (a),
a
or the integral of a derivative along an interval is the total change between
the sides of that interval. This has many ramifications:
Theorem
If MC (x) represents the marginal cost of making x units of a product, then
x
C (x) = C (0) + MC (q) dq.
0
V63.0121.041, Calculus I (NYU) Section 5.4 The Fundamental Theorem December 8, 2010 7 / 33
The Integral as Total Change
Notes
Another way to state this theorem is:
b
F (x) dx = F (b) − F (a),
a
or the integral of a derivative along an interval is the total change between
the sides of that interval. This has many ramifications:
Theorem
If ρ(x) represents the density of a thin rod at a distance of x from its end,
then the mass of the rod up to x is
x
m(x) = ρ(s) ds.
0
V63.0121.041, Calculus I (NYU) Section 5.4 The Fundamental Theorem December 8, 2010 7 / 33
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4. V63.0121.041, Calculus I Section 5.4 : The Fundamental Theorem December 8, 2010
My first table of integrals
Notes
[f (x) + g (x)] dx = f (x) dx + g (x) dx
x n+1
x n dx = + C (n = −1) cf (x) dx = c f (x) dx
n+1
1
e x dx = e x + C dx = ln |x| + C
x
x ax
sin x dx = − cos x + C a dx = +C
ln a
cos x dx = sin x + C csc2 x dx = − cot x + C
sec2 x dx = tan x + C csc x cot x dx = − csc x + C
1
sec x tan x dx = sec x + C √ dx = arcsin x + C
1 − x2
1
dx = arctan x + C
1 + x2
V63.0121.041, Calculus I (NYU) Section 5.4 The Fundamental Theorem December 8, 2010 8 / 33
Outline
Notes
Recall: The Evaluation Theorem a/k/a 2nd FTC
The First Fundamental Theorem of Calculus
The Area Function
Statement and proof of 1FTC
Biographies
Differentiation of functions defined by integrals
“Contrived” examples
Erf
Other applications
V63.0121.041, Calculus I (NYU) Section 5.4 The Fundamental Theorem December 8, 2010 9 / 33
An area function
Notes
x
3
Let f (t) = t and define g (x) = f (t) dt. Can we evaluate the integral
0
in g (x)?
Dividing the interval [0, x] into n pieces
x ix
gives ∆t = and ti = 0 + i∆t = . So
n n
x x 3 x (2x)3 x (nx)3
Rn = · + · + ··· + ·
n n3 n n3 n n3
x4 3
= 4 1 + 23 + 33 + · · · + n 3
n
x4 1 2
= 4 2 n(n + 1)
n
0 x
x 4 n2 (n + 1)2 x4
= 4
→
4n 4
as n → ∞.
V63.0121.041, Calculus I (NYU) Section 5.4 The Fundamental Theorem December 8, 2010 10 / 33
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5. V63.0121.041, Calculus I Section 5.4 : The Fundamental Theorem December 8, 2010
An area function, continued
Notes
So
x4
g (x) = .
4
This means that
g (x) = x 3 .
V63.0121.041, Calculus I (NYU) Section 5.4 The Fundamental Theorem December 8, 2010 11 / 33
The area function
Notes
Let f be a function which is integrable (i.e., continuous or with finitely
many jump discontinuities) on [a, b]. Define
x
g (x) = f (t) dt.
a
The variable is x; t is a “dummy” variable that’s integrated over.
Picture changing x and taking more of less of the region under the
curve.
Question: What does f tell you about g ?
V63.0121.041, Calculus I (NYU) Section 5.4 The Fundamental Theorem December 8, 2010 12 / 33
Envisioning the area function
Notes
Example
Suppose f (t) is the function graphed below:
y
g
x
2 4 6 8 10f
x
Let g (x) = f (t) dt. What can you say about g ?
0
V63.0121.041, Calculus I (NYU) Section 5.4 The Fundamental Theorem December 8, 2010 13 / 33
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6. V63.0121.041, Calculus I Section 5.4 : The Fundamental Theorem December 8, 2010
features of g from f
Notes
y
Interval sign monotonicity monotonicity concavity
of f of g of f of g
g
[0, 2] +
x
2 4 6 8 10f [2, 4.5] +
[4.5, 6] −
[6, 8] −
[8, 10] − → none
We see that g is behaving a lot like an antiderivative of f .
V63.0121.041, Calculus I (NYU) Section 5.4 The Fundamental Theorem December 8, 2010 14 / 33
Another Big Time Theorem
Notes
Theorem (The First Fundamental Theorem of Calculus)
Let f be an integrable function on [a, b] and define
x
g (x) = f (t) dt.
a
If f is continuous at x in (a, b), then g is differentiable at x and
g (x) = f (x).
V63.0121.041, Calculus I (NYU) Section 5.4 The Fundamental Theorem December 8, 2010 15 / 33
Proving the Fundamental Theorem
Notes
Proof.
Let h > 0 be given so that x + h < b. We have
x+h
g (x + h) − g (x) 1
= f (t) dt.
h h x
Let Mh be the maximum value of f on [x, x + h], and let mh the minimum
value of f on [x, x + h]. From §5.2 we have
x+h
mh · h ≤ f (t) dt ≤ Mh · h
x
So
g (x + h) − g (x)
mh ≤ ≤ Mh .
h
As h → 0, both mh and Mh tend to f (x).
V63.0121.041, Calculus I (NYU) Section 5.4 The Fundamental Theorem December 8, 2010 16 / 33
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7. V63.0121.041, Calculus I Section 5.4 : The Fundamental Theorem December 8, 2010
Meet the Mathematician: James Gregory
Notes
Scottish, 1638-1675
Astronomer and Geometer
Conceived transcendental
numbers and found evidence
that π was transcendental
Proved a geometric version
of 1FTC as a lemma but
didn’t take it further
V63.0121.041, Calculus I (NYU) Section 5.4 The Fundamental Theorem December 8, 2010 17 / 33
Meet the Mathematician: Isaac Barrow
Notes
English, 1630-1677
Professor of Greek, theology,
and mathematics at
Cambridge
Had a famous student
V63.0121.041, Calculus I (NYU) Section 5.4 The Fundamental Theorem December 8, 2010 18 / 33
Meet the Mathematician: Isaac Newton
Notes
English, 1643–1727
Professor at Cambridge
(England)
Philosophiae Naturalis
Principia Mathematica
published 1687
V63.0121.041, Calculus I (NYU) Section 5.4 The Fundamental Theorem December 8, 2010 19 / 33
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8. V63.0121.041, Calculus I Section 5.4 : The Fundamental Theorem December 8, 2010
Meet the Mathematician: Gottfried Leibniz
Notes
German, 1646–1716
Eminent philosopher as well
as mathematician
Contemporarily disgraced by
the calculus priority dispute
V63.0121.041, Calculus I (NYU) Section 5.4 The Fundamental Theorem December 8, 2010 20 / 33
Differentiation and Integration as reverse processes
Notes
Putting together 1FTC and 2FTC, we get a beautiful relationship between
the two fundamental concepts in calculus.
Theorem (The Fundamental Theorem(s) of Calculus)
I. If f is a continuous function, then
x
d
f (t) dt = f (x)
dx a
So the derivative of the integral is the original function.
II. If f is a differentiable function, then
b
f (x) dx = f (b) − f (a).
a
So the integral of the derivative of is (an evaluation of) the original
function.
V63.0121.041, Calculus I (NYU) Section 5.4 The Fundamental Theorem December 8, 2010 21 / 33
Outline
Notes
Recall: The Evaluation Theorem a/k/a 2nd FTC
The First Fundamental Theorem of Calculus
The Area Function
Statement and proof of 1FTC
Biographies
Differentiation of functions defined by integrals
“Contrived” examples
Erf
Other applications
V63.0121.041, Calculus I (NYU) Section 5.4 The Fundamental Theorem December 8, 2010 22 / 33
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9. V63.0121.041, Calculus I Section 5.4 : The Fundamental Theorem December 8, 2010
Differentiation of area functions
Notes
Example
3x
Let h(x) = t 3 dt. What is h (x)?
0
Solution (Using 2FTC)
3x
t4 1
h(x) = = (3x)4 = 1
4 · 81x 4 , so h (x) = 81x 3 .
4 0 4
Solution (Using 1FTC)
u
We can think of h as the composition g ◦ k, where g (u) = t 3 dt and
0
k(x) = 3x. Then h (x) = g (u) · k (x), or
h (x) = g (k(x)) · k (x) = (k(x))3 · 3 = (3x)3 · 3 = 81x 3 .
V63.0121.041, Calculus I (NYU) Section 5.4 The Fundamental Theorem December 8, 2010 23 / 33
Differentiation of area functions, in general
Notes
by 1FTC
k(x)
d
f (t) dt = f (k(x))k (x)
dx a
by reversing the order of integration:
b h(x)
d d
f (t) dt = − f (t) dt = −f (h(x))h (x)
dx h(x) dx b
by combining the two above:
k(x) k(x) 0
d d
f (t) dt = f (t) dt + f (t) dt
dx h(x) dx 0 h(x)
= f (k(x))k (x) − f (h(x))h (x)
V63.0121.041, Calculus I (NYU) Section 5.4 The Fundamental Theorem December 8, 2010 24 / 33
Another Example
Notes
Example
sin2 x
Let h(x) = (17t 2 + 4t − 4) dt. What is h (x)?
0
Solution
V63.0121.041, Calculus I (NYU) Section 5.4 The Fundamental Theorem December 8, 2010 25 / 33
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10. V63.0121.041, Calculus I Section 5.4 : The Fundamental Theorem December 8, 2010
A Similar Example
Notes
Example
sin2 x
Let h(x) = (17t 2 + 4t − 4) dt. What is h (x)?
3
Solution
V63.0121.041, Calculus I (NYU) Section 5.4 The Fundamental Theorem December 8, 2010 26 / 33
Compare
Notes
Question
Why is
sin2 x sin2 x
d d
(17t 2 + 4t − 4) dt = (17t 2 + 4t − 4) dt?
dx 0 dx 3
Or, why doesn’t the lower limit appear in the derivative?
Answer
Because
sin2 x 3 sin2 x
(17t 2 + 4t − 4) dt = (17t 2 + 4t − 4) dt + (17t 2 + 4t − 4) dt
0 0 3
So the two functions differ by a constant.
V63.0121.041, Calculus I (NYU) Section 5.4 The Fundamental Theorem December 8, 2010 27 / 33
The Full Nasty
Notes
Example
ex
Find the derivative of F (x) = sin4 t dt.
x3
Solution
Notice here it’s much easier than finding an antiderivative for sin4 .
V63.0121.041, Calculus I (NYU) Section 5.4 The Fundamental Theorem December 8, 2010 28 / 33
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11. V63.0121.041, Calculus I Section 5.4 : The Fundamental Theorem December 8, 2010
Why use 1FTC?
Notes
Question
Why would we use 1FTC to find the derivative of an integral? It seems
like confusion for its own sake.
Answer
Some functions are difficult or impossible to integrate in elementary
terms.
Some functions are naturally defined in terms of other integrals.
V63.0121.041, Calculus I (NYU) Section 5.4 The Fundamental Theorem December 8, 2010 29 / 33
Erf
Notes
Here’s a function with a funny name but an important role:
x
2 2
erf(x) = √ e −t dt.
π 0
It turns out erf is the shape of the bell curve. We can’t find erf(x),
2 2
explicitly, but we do know its derivative: erf (x) = √ e −x .
π
Example
d
Find erf(x 2 ).
dx
Solution
V63.0121.041, Calculus I (NYU) Section 5.4 The Fundamental Theorem December 8, 2010 30 / 33
Other functions defined by integrals
Notes
The future value of an asset:
∞
FV (t) = π(s)e −rs ds
t
where π(s) is the profitability at time s and r is the discount rate.
The consumer surplus of a good:
q∗
CS(q ∗ ) = (f (q) − p ∗ ) dq
0
where f (q) is the demand function and p ∗ and q ∗ the equilibrium
price and quantity.
V63.0121.041, Calculus I (NYU) Section 5.4 The Fundamental Theorem December 8, 2010 31 / 33
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12. V63.0121.041, Calculus I Section 5.4 : The Fundamental Theorem December 8, 2010
Surplus by picture
Notes
consumer surplus
price (p)
producer surplus
supply
p∗ equilibrium
market revenue
demand f (q)
q∗ quantity (q)
V63.0121.041, Calculus I (NYU) Section 5.4 The Fundamental Theorem December 8, 2010 32 / 33
Summary
Notes
Functions defined as integrals can be differentiated using the first
FTC: x
d
f (t) dt = f (x)
dx a
The two FTCs link the two major processes in calculus: differentiation
and integration
F (x) dx = F (x) + C
Follow the calculus wars on twitter: #calcwars
V63.0121.041, Calculus I (NYU) Section 5.4 The Fundamental Theorem December 8, 2010 33 / 33
Notes
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