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Section	5.4
 The	Fundamental	Theorem	of	Calculus

                  V63.0121, Calculus	I



                     April	23, 2009



Announcements
   Quiz	6	next	week	on	§§5.1–5.2


                                         .   .   .   .   .   .
Outline

  Recall: The	Evaluation	Theorem	a/k/a	2FTC

  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

  Worksheet

  Summary


                                              .      .   .   .   .   .
The	definite	integral	as	a	limit




   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
                                   ∆x→0
                       a                  i=1




                                                 .    .    .    .   .      .
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




                                                  .    .   .   .   .   .
The	Integral	as	Total	Change


   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:




                                                       .    .   .   .   .   .
The	Integral	as	Total	Change


   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




                                                          .    .   .   .   .   .
The	Integral	as	Total	Change


   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



                                                       .    .   .   .   .   .
The	Integral	as	Total	Change


   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



                                                       .    .   .   .   .   .
My	first	table	of	integrals
    ∫                         ∫               ∫
         [f(x) + g(x)] dx =       f(x) dx +       g(x) dx
                                                     ∫                ∫
     ∫
                     xn+1
          xn dx =                                       cf(x) dx = c f(x) dx
                          + C (n ̸= −1)
                    n+1                                ∫
               ∫
                                                           1
                  ex dx = ex + C                             dx = ln |x| + C
                                                           x
                                                       ∫
           ∫
                                                                     ax
                                                           ax dx =       +C
              sin x dx = − cos x + C
                                                                    ln a
                                                    ∫
            ∫
                                                       csc2 x dx = − cot x + C
                cos x dx = sin x + C
                                                  ∫
           ∫
               sec2 x dx = tan x + C                 csc x cot x dx = − csc x + C
                                                  ∫
         ∫
                                                         1
                                                     √          dx = arcsin x + C
            sec x tan x dx = sec x + C
                                                       1 − x2
         ∫
                1
                     dx = arctan x + C
             1 + x2
                                                          .   .    .    .    .      .
Outline

  Recall: The	Evaluation	Theorem	a/k/a	2FTC

  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

  Worksheet

  Summary


                                              .      .   .   .   .   .
An	area	function
                                    ∫   x
               3
    Let f(t) = t and	define g(x) =           f(t) dt. Can	we	evaluate	the
                                    0
    integral	in g(x)?




    .
                        x
                        .
  0
  .




                                                      .   .    .   .       .   .
An	area	function
                                    ∫   x
               3
    Let f(t) = t and	define g(x) =           f(t) dt. Can	we	evaluate	the
                                    0
    integral	in g(x)?
                               Dividing	the	interval [0, x] into n pieces
                                           x                        ix
                               gives ∆x = and xi = 0 + i∆x = .
                                           n                        n
                               So
                                      x x3       x (2x)3           x (nx)3
                                         · 3 + · 3 + ··· + · 3
                               Rn =
                                      nn        n    n             n   n
                                        4(                           )
                                      x
                                    = 4 1 3 + 2 3 + 3 3 + · · · + n3
                                      n
                                      x4 [ 1         ]2
                                    = 4 2 n(n + 1)
    .
                                      n
                        x
                        .
  0
  .
                                      x4 n2 (n + 1)2    x4
                                                     →
                                    =
                                            4n4         4
                               as n → ∞.
                                                      .   .    .   .       .   .
An	area	function, continued




   So
                                x4
                       g(x) =      .
                                4




                                       .   .   .   .   .   .
An	area	function, continued




   So
                                x4
                       g(x) =      .
                                4
   This	means	that
                       g′ (x) = x3 .




                                       .   .   .   .   .   .
The	area	function



   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


       When	is g increasing?




                                                 .   .    .    .   .   .
The	area	function



   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


       When	is g increasing?
       When	is g decreasing?




                                                 .   .    .    .   .   .
The	area	function



   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


       When	is g increasing?
       When	is g decreasing?
       Over	a	small	interval, what’s	the	average	rate	of	change	of g?




                                                 .   .    .    .   .    .
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).




                                                 .    .    .    .      .   .
Proof.
Let h > 0 be	given	so	that x + h < b. We	have

                g(x + h) − g(x)
                                =
                       h




                                          .     .   .   .   .   .
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




                                                 .     .   .   .   .   .
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 mh the
minimum	value	of f on [x, x + h]. From	§5.2	we	have
                          ∫    x+h
                                     f(t) dt
                           x




                                                      .     .   .   .   .   .
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 mh the
minimum	value	of f on [x, x + h]. From	§5.2	we	have
                          ∫    x+h
                                     f(t) dt ≤ Mh · h
                           x




                                                     .     .   .   .   .   .
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 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




                                                      .     .   .   .   .   .
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 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



                                                      .     .   .   .   .   .
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 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). Zappa-dappa.


                                                      .     .   .   .   .   .
Meet	the	Mathematician: James	Gregory


     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



                                 .   .   .   .   .   .
Meet	the	Mathematician: Isaac	Barrow




     English, 1630-1677
     Professor	of	Greek,
     theology, and
     mathematics	at
     Cambridge
     Had	a	famous	student




                                  .    .   .   .   .   .
Meet	the	Mathematician: Isaac	Newton




     English, 1643–1727
     Professor	at	Cambridge
     (England)
     Philosophiae	Naturalis
     Principia	Mathematica
     published	1687




                                 .     .   .   .   .   .
Meet	the	Mathematician: Gottfried	Leibniz




     German, 1646–1716
     Eminent	philosopher	as
     well	as	mathematician
     Contemporarily
     disgraced	by	the
     calculus	priority	dispute




                                   .   .    .   .   .   .
Differentiation	and	Integration	as	reverse	processes



   Putting	together	1FTC and	2FTC,	we	get	a	beautiful	relationship
   between	the	two	fundamental	concepts	in	calculus.
                                 ∫   x
                            d
                                         f(t) dt = f(x)
                            dx   a




                                                      .   .   .   .   .   .
Differentiation	and	Integration	as	reverse	processes



   Putting	together	1FTC and	2FTC,	we	get	a	beautiful	relationship
   between	the	two	fundamental	concepts	in	calculus.
                                      ∫   x
                                 d
                                              f(t) dt = f(x)
                                 dx   a


                        ∫    b
                                 F′ (x) dx = F(b) − F(a).
                         a




                                                           .   .   .   .   .   .
Outline

  Recall: The	Evaluation	Theorem	a/k/a	2FTC

  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

  Worksheet

  Summary


                                              .      .   .   .   .   .
Differentiation	of	area	functions

   Example ∫
                    x
                        t3 dt. We	know g′ (x) = x3 . What	if	instead	we	had
   Let g(x) =
                0
                                           ∫   3x
                                                    t3 dt.
                                  h(x) =
                                           0

   What	is h′ (x)?




                                                             .   .   .   .   .   .
Differentiation	of	area	functions

   Example ∫
                    x
                        t3 dt. We	know g′ (x) = x3 . What	if	instead	we	had
   Let g(x) =
                0
                                           ∫   3x
                                                    t3 dt.
                                  h(x) =
                                           0

   What	is h′ (x)?

   Solution                                                              ∫       u
                                                                                     t3 dt
   We	can	think	of h as	the	composition g k, where g(u) =
                                                        ◦
                                                                             0
   and k(x) = 3x. Then

           h′ (x) = g′ (k(x))k′ (x) = 3(k(x))3 = 3(3x)3 = 81x3 .


                                                             .   .   .   .            .      .
Example
             ∫   sin2 x
                          (17t2 + 4t − 4) dt. What	is h′ (x)?
Let h(x) =
             0




                                                      .    .    .   .   .   .
Example
             ∫       sin2 x
                              (17t2 + 4t − 4) dt. What	is h′ (x)?
Let h(x) =
                 0

Solution
We	have
             ∫   sin2 x
       d
                          (17t2 + 4t − 4) dt
       dx    0
                               (                            )d
                              = 17(sin2 x)2 + 4(sin2 x) − 4 ·       sin2 x
                                                                dx
                               (                        )
                              = 17 sin4 x + 4 sin2 x − 4 · 2 sin x cos x




                                                          .    .    .    .   .   .
Erf
      Here’s	a	function	with	a	funny	name	but	an	important	role:
                                       ∫x
                                     2       2
                                          e−t dt.
                                    √
                           erf(x) =
                                      π0




                                                 .   .    .   .    .   .
Erf
      Here’s	a	function	with	a	funny	name	but	an	important	role:
                                       ∫x
                                     2       2
                                          e−t dt.
                                    √
                           erf(x) =
                                      π0
      It	turns	out erf is	the	shape	of	the	bell	curve.




                                                         .   .   .   .   .   .
Erf
      Here’s	a	function	with	a	funny	name	but	an	important	role:
                                       ∫x
                                     2       2
                                          e−t dt.
                                    √
                           erf(x) =
                                      π0
      It	turns	out erf is	the	shape	of	the	bell	curve. We	can’t	find erf(x),
      explicitly, but	we	do	know	its	derivative.

                               erf′ (x) =




                                                    .    .    .    .   .      .
Erf
      Here’s	a	function	with	a	funny	name	but	an	important	role:
                                       ∫x
                                     2       2
                                          e−t dt.
                                    √
                           erf(x) =
                                      π0
      It	turns	out erf is	the	shape	of	the	bell	curve. We	can’t	find erf(x),
      explicitly, but	we	do	know	its	derivative.
                                           2   2
                               erf′ (x) = √ e−x .
                                            π




                                                    .    .    .    .   .      .
Erf
      Here’s	a	function	with	a	funny	name	but	an	important	role:
                                       ∫x
                                     2       2
                                          e−t dt.
                                    √
                           erf(x) =
                                      π0
      It	turns	out erf is	the	shape	of	the	bell	curve. We	can’t	find erf(x),
      explicitly, but	we	do	know	its	derivative.
                                           2   2
                               erf′ (x) = √ e−x .
                                            π

      Example
             d
                erf(x2 ).
      Find
             dx




                                                    .    .    .    .   .      .
Erf
      Here’s	a	function	with	a	funny	name	but	an	important	role:
                                       ∫x
                                     2       2
                                          e−t dt.
                                    √
                           erf(x) =
                                      π0
      It	turns	out erf is	the	shape	of	the	bell	curve. We	can’t	find erf(x),
      explicitly, but	we	do	know	its	derivative.
                                           2   2
                               erf′ (x) = √ e−x .
                                            π

      Example
             d
                erf(x2 ).
      Find
             dx
      Solution
      By	the	chain	rule	we	have

              d                       d      2             4
                                                  22            4
                 erf(x2 ) = erf′ (x2 ) x2 = √ e−(x ) 2x = √ xe−x .
              dx                      dx      π             π
                                                    .    .    .    .   .      .
Other	functions	defined	by	integrals

      The	future	value	of	an	asset:
                                 ∫∞
                                    π(τ )e−rτ dτ
                        FV(t) =
                                       t

      where π(τ ) is	the	profitability	at	time τ 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.


                                                         .    .   .   .   .   .
Outline

  Recall: The	Evaluation	Theorem	a/k/a	2FTC

  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

  Worksheet

  Summary


                                              .      .   .   .   .   .
Worksheet
        .




.
Image: Erick	Cifuentes
                                     .   .   .   .   .   .
Outline

  Recall: The	Evaluation	Theorem	a/k/a	2FTC

  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

  Worksheet

  Summary


                                              .      .   .   .   .   .
Summary




     FTC links	integration	and	differentiation
     When	differentiating	integral	functions, do	not	forget	the
     chain	rule
     Facts	about	the	integral	function	can	be	gleaned	from	the
     integrand




                                             .    .   .    .      .   .

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Lesson 26: The Fundamental Theorem of Calculus (Section 4 version)

  • 1. Section 5.4 The Fundamental Theorem of Calculus V63.0121, Calculus I April 23, 2009 Announcements Quiz 6 next week on §§5.1–5.2 . . . . . .
  • 2. Outline Recall: The Evaluation Theorem a/k/a 2FTC 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 Worksheet Summary . . . . . .
  • 3. The definite integral as a limit 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 ∆x→0 a i=1 . . . . . .
  • 4. 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 . . . . . .
  • 5. The Integral as Total Change 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: . . . . . .
  • 6. The Integral as Total Change 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 . . . . . .
  • 7. The Integral as Total Change 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 . . . . . .
  • 8. The Integral as Total Change 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 . . . . . .
  • 9. My first table of integrals ∫ ∫ ∫ [f(x) + g(x)] dx = f(x) dx + g(x) dx ∫ ∫ ∫ xn+1 xn dx = cf(x) dx = c f(x) dx + C (n ̸= −1) n+1 ∫ ∫ 1 ex dx = ex + C dx = ln |x| + C x ∫ ∫ ax ax dx = +C sin x dx = − cos x + C ln a ∫ ∫ csc2 x dx = − cot x + C cos x dx = sin x + C ∫ ∫ sec2 x dx = tan x + C csc x cot x dx = − csc x + C ∫ ∫ 1 √ dx = arcsin x + C sec x tan x dx = sec x + C 1 − x2 ∫ 1 dx = arctan x + C 1 + x2 . . . . . .
  • 10. Outline Recall: The Evaluation Theorem a/k/a 2FTC 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 Worksheet Summary . . . . . .
  • 11. An area function ∫ x 3 Let f(t) = t and define g(x) = f(t) dt. Can we evaluate the 0 integral in g(x)? . x . 0 . . . . . . .
  • 12. An area function ∫ x 3 Let f(t) = t and define g(x) = f(t) dt. Can we evaluate the 0 integral in g(x)? Dividing the interval [0, x] into n pieces x ix gives ∆x = and xi = 0 + i∆x = . n n So x x3 x (2x)3 x (nx)3 · 3 + · 3 + ··· + · 3 Rn = nn n n n n 4( ) x = 4 1 3 + 2 3 + 3 3 + · · · + n3 n x4 [ 1 ]2 = 4 2 n(n + 1) . n x . 0 . x4 n2 (n + 1)2 x4 → = 4n4 4 as n → ∞. . . . . . .
  • 13. An area function, continued So x4 g(x) = . 4 . . . . . .
  • 14. An area function, continued So x4 g(x) = . 4 This means that g′ (x) = x3 . . . . . . .
  • 15. The area function 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 When is g increasing? . . . . . .
  • 16. The area function 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 When is g increasing? When is g decreasing? . . . . . .
  • 17. The area function 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 When is g increasing? When is g decreasing? Over a small interval, what’s the average rate of change of g? . . . . . .
  • 18. 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). . . . . . .
  • 19. Proof. Let h > 0 be given so that x + h < b. We have g(x + h) − g(x) = h . . . . . .
  • 20. 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 . . . . . .
  • 21. 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 mh the minimum value of f on [x, x + h]. From §5.2 we have ∫ x+h f(t) dt x . . . . . .
  • 22. 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 mh the minimum value of f on [x, x + h]. From §5.2 we have ∫ x+h f(t) dt ≤ Mh · h x . . . . . .
  • 23. 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 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 . . . . . .
  • 24. 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 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 . . . . . .
  • 25. 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 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). Zappa-dappa. . . . . . .
  • 26. Meet the Mathematician: James Gregory 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 . . . . . .
  • 27. Meet the Mathematician: Isaac Barrow English, 1630-1677 Professor of Greek, theology, and mathematics at Cambridge Had a famous student . . . . . .
  • 28. Meet the Mathematician: Isaac Newton English, 1643–1727 Professor at Cambridge (England) Philosophiae Naturalis Principia Mathematica published 1687 . . . . . .
  • 29. Meet the Mathematician: Gottfried Leibniz German, 1646–1716 Eminent philosopher as well as mathematician Contemporarily disgraced by the calculus priority dispute . . . . . .
  • 30. Differentiation and Integration as reverse processes Putting together 1FTC and 2FTC, we get a beautiful relationship between the two fundamental concepts in calculus. ∫ x d f(t) dt = f(x) dx a . . . . . .
  • 31. Differentiation and Integration as reverse processes Putting together 1FTC and 2FTC, we get a beautiful relationship between the two fundamental concepts in calculus. ∫ x d f(t) dt = f(x) dx a ∫ b F′ (x) dx = F(b) − F(a). a . . . . . .
  • 32. Outline Recall: The Evaluation Theorem a/k/a 2FTC 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 Worksheet Summary . . . . . .
  • 33. Differentiation of area functions Example ∫ x t3 dt. We know g′ (x) = x3 . What if instead we had Let g(x) = 0 ∫ 3x t3 dt. h(x) = 0 What is h′ (x)? . . . . . .
  • 34. Differentiation of area functions Example ∫ x t3 dt. We know g′ (x) = x3 . What if instead we had Let g(x) = 0 ∫ 3x t3 dt. h(x) = 0 What is h′ (x)? Solution ∫ u t3 dt We can think of h as the composition g k, where g(u) = ◦ 0 and k(x) = 3x. Then h′ (x) = g′ (k(x))k′ (x) = 3(k(x))3 = 3(3x)3 = 81x3 . . . . . . .
  • 35. Example ∫ sin2 x (17t2 + 4t − 4) dt. What is h′ (x)? Let h(x) = 0 . . . . . .
  • 36. Example ∫ sin2 x (17t2 + 4t − 4) dt. What is h′ (x)? Let h(x) = 0 Solution We have ∫ sin2 x d (17t2 + 4t − 4) dt dx 0 ( )d = 17(sin2 x)2 + 4(sin2 x) − 4 · sin2 x dx ( ) = 17 sin4 x + 4 sin2 x − 4 · 2 sin x cos x . . . . . .
  • 37. Erf Here’s a function with a funny name but an important role: ∫x 2 2 e−t dt. √ erf(x) = π0 . . . . . .
  • 38. Erf Here’s a function with a funny name but an important role: ∫x 2 2 e−t dt. √ erf(x) = π0 It turns out erf is the shape of the bell curve. . . . . . .
  • 39. Erf Here’s a function with a funny name but an important role: ∫x 2 2 e−t dt. √ erf(x) = π0 It turns out erf is the shape of the bell curve. We can’t find erf(x), explicitly, but we do know its derivative. erf′ (x) = . . . . . .
  • 40. Erf Here’s a function with a funny name but an important role: ∫x 2 2 e−t dt. √ erf(x) = π0 It turns out erf is the shape of the bell curve. We can’t find erf(x), explicitly, but we do know its derivative. 2 2 erf′ (x) = √ e−x . π . . . . . .
  • 41. Erf Here’s a function with a funny name but an important role: ∫x 2 2 e−t dt. √ erf(x) = π0 It turns out erf is the shape of the bell curve. We can’t find erf(x), explicitly, but we do know its derivative. 2 2 erf′ (x) = √ e−x . π Example d erf(x2 ). Find dx . . . . . .
  • 42. Erf Here’s a function with a funny name but an important role: ∫x 2 2 e−t dt. √ erf(x) = π0 It turns out erf is the shape of the bell curve. We can’t find erf(x), explicitly, but we do know its derivative. 2 2 erf′ (x) = √ e−x . π Example d erf(x2 ). Find dx Solution By the chain rule we have d d 2 4 22 4 erf(x2 ) = erf′ (x2 ) x2 = √ e−(x ) 2x = √ xe−x . dx dx π π . . . . . .
  • 43. Other functions defined by integrals The future value of an asset: ∫∞ π(τ )e−rτ dτ FV(t) = t where π(τ ) is the profitability at time τ 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. . . . . . .
  • 44. Outline Recall: The Evaluation Theorem a/k/a 2FTC 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 Worksheet Summary . . . . . .
  • 45. Worksheet . . Image: Erick Cifuentes . . . . . .
  • 46. Outline Recall: The Evaluation Theorem a/k/a 2FTC 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 Worksheet Summary . . . . . .
  • 47. Summary FTC links integration and differentiation When differentiating integral functions, do not forget the chain rule Facts about the integral function can be gleaned from the integrand . . . . . .