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Section 2.6
                                  Implicit Differentiation

                                     V63.0121, Calculus I


                                     February 24/25, 2009



         Announcements
                  Midterm in class March 4/5
                  ALEKS due Friday, 11:59pm

         .
.
Image credit: Telstar Logistics
                                                            .   .   .   .   .   .
Outline



   The big idea, by example


   Examples
      Vertical and Horizontal Tangents
      Chemistry


   The power rule for rational powers




                                         .   .   .   .   .   .
y
                                              .
Motivating Example

Problem
Find the slope of the line which is
tangent to the curve
                                              .                   x
                                                                  .
              2    2
             x +y =1

at the point (3/5, −4/5).




                                      .   .       .   .   .   .
y
                                              .
Motivating Example

Problem
Find the slope of the line which is
tangent to the curve
                                              .                   x
                                                                  .
              2    2
             x +y =1

at the point (3/5, −4/5).




                                      .   .       .   .   .   .
y
                                              .
Motivating Example

Problem
Find the slope of the line which is
tangent to the curve
                                              .                       x
                                                                      .
              2    2
             x +y =1

at the point (3/5, −4/5).                                 .




                                      .   .       .   .       .   .
y
                                                           .
Motivating Example

Problem
Find the slope of the line which is
tangent to the curve
                                                           .                       x
                                                                                   .
              2    2
             x +y =1

at the point (3/5, −4/5).                                              .
   Solution (Explicit)
                                         √
         Isolate: y2 = 1 − x2 =⇒ y = −    1 − x2 . (Why the −?)




                                                  .    .       .   .       .   .
y
                                                        .
Motivating Example

Problem
Find the slope of the line which is
tangent to the curve
                                                        .                       x
                                                                                .
              2    2
             x +y =1

at the point (3/5, −4/5).                                           .
   Solution (Explicit)
                                        √
         Isolate: y2 = 1 − x2 =⇒ y = − 1 − x2 . (Why the −?)
                                 −2x
                        dy                   x
                           =− √         =√
         Differentiate:
                               2 1 − x2    1 − x2
                        dx




                                               .    .       .   .       .   .
y
                                                        .
Motivating Example

Problem
Find the slope of the line which is
tangent to the curve
                                                        .                       x
                                                                                .
              2    2
             x +y =1

at the point (3/5, −4/5).                                           .
   Solution (Explicit)
                                        √
         Isolate: y2 = 1 − x2 =⇒ y = − 1 − x2 . (Why the −?)
                                 −2x
                        dy                    x
                           =− √         =√
         Differentiate:
                               2 1 − x2     1 − x2
                        dx
                     dy            3/5         3/5  3
                              =√            =      =.
         Evaluate:
                                 1 − (3/5)
                     dx x=3/5                  4/5  4
                                          2



                                               .    .       .   .       .   .
y
                                                        .
Motivating Example

Problem
Find the slope of the line which is
tangent to the curve
                                                        .                       x
                                                                                .
              2    2
             x +y =1

at the point (3/5, −4/5).                                           .
   Solution (Explicit)
                                        √
         Isolate: y2 = 1 − x2 =⇒ y = − 1 − x2 . (Why the −?)
                                 −2x
                        dy                    x
                           =− √         =√
         Differentiate:
                               2 1 − x2     1 − x2
                        dx
                     dy            3/5         3/5  3
                              =√            =      =.
         Evaluate:
                                 1 − (3/5)
                     dx x=3/5                  4/5  4
                                          2



                                               .    .       .   .       .   .
We know that x2 + y2 = 1 does not define y as a function of x, but
suppose it did.
    Suppose we had y = f(x), so that

                            x2 + (f(x))2 = 1

    We could differentiate this equation to get

                          2x + 2f(x) · f′ (x) = 0

    We could then solve to get
                                            x
                             f′ (x) = −
                                          f(x)




                                                 .   .   .   .   .   .
The beautiful fact (i.e., deep theorem) is that this works!
                                                         y
                                                         .
   “Near” most points on
   the curve x2 + y2 = 1, the
   curve resembles the
   graph of a function.
   So f(x) is defined “locally”
                                                         .                       x
                                                                                 .
   and is differentiable
   The chain rule then
   applies for this local
                                                                     .
   choice.




                                                .    .       .   .       .   .
The beautiful fact (i.e., deep theorem) is that this works!
                                                         y
                                                         .
   “Near” most points on
   the curve x2 + y2 = 1, the
   curve resembles the
   graph of a function.
   So f(x) is defined “locally”
                                                         .                       x
                                                                                 .
   and is differentiable
   The chain rule then
   applies for this local
                                                                     .
   choice.




                                                .    .       .   .       .   .
The beautiful fact (i.e., deep theorem) is that this works!
                                                         y
                                                         .
   “Near” most points on
   the curve x2 + y2 = 1, the
   curve resembles the
   graph of a function.
   So f(x) is defined “locally”
                                                           .                       x
                                                                                   .
   and is differentiable
   The chain rule then
   applies for this local
                                                                       .
   choice.
                                                         l
                                                         .ooks like a function



                                                .    .         .   .       .   .
The beautiful fact (i.e., deep theorem) is that this works!
                                                         y
                                                         .
   “Near” most points on
   the curve x2 + y2 = 1, the                                        .
   curve resembles the
   graph of a function.
   So f(x) is defined “locally”
                                                         .                       x
                                                                                 .
   and is differentiable
   The chain rule then
   applies for this local
   choice.




                                                .    .       .   .       .   .
The beautiful fact (i.e., deep theorem) is that this works!
                                                         y
                                                         .
   “Near” most points on
   the curve x2 + y2 = 1, the                                        .
   curve resembles the
   graph of a function.
   So f(x) is defined “locally”
                                                         .                       x
                                                                                 .
   and is differentiable
   The chain rule then
   applies for this local
   choice.




                                                .    .       .   .       .   .
The beautiful fact (i.e., deep theorem) is that this works!
                                                         y
                                                         .
   “Near” most points on
   the curve x2 + y2 = 1, the                                     .
   curve resembles the
   graph of a function.                                l
                                                       .ooks like a function
   So f(x) is defined “locally”
                                                         .                   x
                                                                             .
   and is differentiable
   The chain rule then
   applies for this local
   choice.




                                                .    .       .   .   .   .
The beautiful fact (i.e., deep theorem) is that this works!
                                                         y
                                                         .
   “Near” most points on
   the curve x2 + y2 = 1, the
   curve resembles the
   graph of a function.
   So f(x) is defined “locally”
                                            .            .                   x
                                                                             .
   and is differentiable
   The chain rule then
   applies for this local
   choice.




                                                .    .       .   .   .   .
The beautiful fact (i.e., deep theorem) is that this works!
                                                         y
                                                         .
   “Near” most points on
   the curve x2 + y2 = 1, the
   curve resembles the
   graph of a function.
   So f(x) is defined “locally”
                                            .            .                   x
                                                                             .
   and is differentiable
   The chain rule then
   applies for this local
   choice.




                                                .    .       .   .   .   .
The beautiful fact (i.e., deep theorem) is that this works!
                                                         y
                                                         .
   “Near” most points on
   the curve x2 + y2 = 1, the
   curve resembles the
   graph of a function.
   So f(x) is defined “locally”
                                               .             .                   x
                                                                                 .
   and is differentiable
                                 .
   The chain rule then               does not look like a
   applies for this local             function, but that’s
   choice.                           OK—there are only
                                     two points like this




                                                    .   .        .   .   .   .
Problem
Find the slope of the line which is tangent to the curve x2 + y2 = 1 at the
point (3/5, −4/5).

Solution (Implicit, with Leibniz notation)
     Differentiate. Remember y is assumed to be a function of x:

                                          dy
                                2x + 2y      = 0,
                                          dx
               dy
     Isolate      :
               dx
                                   dy   x
                                      =− .
                                   dx   y
     Evaluate:
                            dy             3/5  3
                                         =     =.
                            dx ( 3 ,− 4 ) 4/5   4
                                 5    5



                                                    .   .    .     .   .      .
Summary

                                           y
                                           .
If a relation is given between x and
y,
     “Most of the time” “at most
     places” y can be assumed to                               .
     be a function of x
                                           .
     we may differentiate the
     relation as is
                  dy
     Solving for     does give the
                  dx
     slope of the tangent line to
     the curve at a point on the
     curve.



                                       .       .   .   .   .       .
Mnemonic

                      Explicit    Implicit
                      y = f(x)   F(x, y) = k




                                                       .


.
Image credit: Walsh
                                    .    .     .   .       .   .
Outline



   The big idea, by example


   Examples
      Vertical and Horizontal Tangents
      Chemistry


   The power rule for rational powers




                                         .   .   .   .   .   .
Example
Find the equation of the line
tangent to the curve
                                .
   y2 = x2 (x + 1) = x3 + x2

at the point (3, −6).
                                                    .




                                    .   .   .   .       .   .
Example
Find the equation of the line
tangent to the curve
                                                     .
   y2 = x2 (x + 1) = x3 + x2

at the point (3, −6).
                                                                         .
 Solution
 Differentiating the expression implicitly with respect to x gives
                               3x2 + 2x
    dy                   dy
 2y = 3x2 + 2x, so          =             , and
    dx                  dx        2y

                                       3 · 32 + 2 · 3
                     dy                                 11
                                                      =− .
                                   =
                     dx                    2(−6)         4
                          (3,−6)




                                                         .   .   .   .       .   .
Example
Find the equation of the line
tangent to the curve
                                                     .
   y2 = x2 (x + 1) = x3 + x2

at the point (3, −6).
                                                                               .
 Solution
 Differentiating the expression implicitly with respect to x gives
                               3x2 + 2x
    dy                   dy
 2y = 3x2 + 2x, so          =             , and
    dx                  dx        2y

                                       3 · 32 + 2 · 3
                     dy                                 11
                                                      =− .
                                   =
                     dx                    2(−6)         4
                          (3,−6)

                                                             11
 Thus the equation of the tangent line is y + 6 = −             (x − 3).
                                                              4
                                                         .      .    .     .       .   .
Example
Find the horizontal tangent lines to the same curve: y2 = x3 + x2




                                              .    .    .    .      .   .
Example
Find the horizontal tangent lines to the same curve: y2 = x3 + x2

Solution




                                              .    .    .    .      .   .
Example
Find the horizontal tangent lines to the same curve: y2 = x3 + x2

Solution
    We solve for dy/dx = 0:

           3x2 + 2x
                    = 0 =⇒ 3x2 + 2x = 0 =⇒ x(3x + 2) = 0
              2y




                                              .    .    .    .      .   .
Example
Find the horizontal tangent lines to the same curve: y2 = x3 + x2

Solution
    We solve for dy/dx = 0:

           3x2 + 2x
                    = 0 =⇒ 3x2 + 2x = 0 =⇒ x(3x + 2) = 0
              2y


    The possible solution x = 0 leads to y = 0, which is not a smooth
    point of the function (the denominator in dy/dx becomes 0).




                                                .    .    .    .    .   .
Example
Find the horizontal tangent lines to the same curve: y2 = x3 + x2

Solution
    We solve for dy/dx = 0:

           3x2 + 2x
                    = 0 =⇒ 3x2 + 2x = 0 =⇒ x(3x + 2) = 0
              2y


    The possible solution x = 0 leads to y = 0, which is not a smooth
    point of the function (the denominator in dy/dx becomes 0).
    The possible solution x = − 2 yields y = ± 3√3 .
                                                2
                                3




                                                 .     .   .   .    .   .
Example
Find the vertical tangent lines to the same curve: y2 = x3 + x2




                                               .    .    .    .   .   .
Example
Find the vertical tangent lines to the same curve: y2 = x3 + x2

Solution
                                        dx
                                           = 0.
     Tangent lines are vertical when
                                        dy
     Differentiating x implicitly as a function of y gives
               dx        dx
     2y = 3x2 + 2x , so
               dy        dy

                                  dx     2y
                                     =2
                                      3x + 2x
                                  dy




                                                     .       .   .   .   .   .
Example
Find the vertical tangent lines to the same curve: y2 = x3 + x2

Solution
                                        dx
                                           = 0.
     Tangent lines are vertical when
                                        dy
     Differentiating x implicitly as a function of y gives
               dx        dx
     2y = 3x2 + 2x , so
               dy        dy

                                  dx     2y
                                     =2
                                      3x + 2x
                                  dy


     This is 0 only when y = 0.



                                                     .       .   .   .   .   .
Example
Find the vertical tangent lines to the same curve: y2 = x3 + x2

Solution
                                        dx
                                           = 0.
     Tangent lines are vertical when
                                        dy
     Differentiating x implicitly as a function of y gives
               dx        dx
     2y = 3x2 + 2x , so
               dy        dy

                                  dx     2y
                                     =2
                                      3x + 2x
                                  dy


     This is 0 only when y = 0.
     We get the false solution x = 0 and the real solution x = −1.


                                                     .       .   .   .   .   .
Ideal gases




     The ideal gas law relates
     temperature, pressure, and
     volume of a gas:

                         PV = nRT

     (R is a constant, n is the
     amount of gas in moles)



                                                                 .
.
Image credit: Scott Beale / Laughing Squid
                                             .   .   .   .   .   .
.

        Definition
        The isothermic compressibility of a fluid is defined by

                                             dV 1
                                      β=−
                                             dP V
        with temperature held constant.

.
Image credit: Neil Better
                                                        .       .   .   .   .       .
.

        Definition
        The isothermic compressibility of a fluid is defined by

                                             dV 1
                                      β=−
                                             dP V
        with temperature held constant.

        The smaller the β, the “harder” the fluid.
.
Image credit: Neil Better
                                                        .       .   .   .   .       .
Example
Find the isothermic compressibility of an ideal gas.




                                                .      .   .   .   .   .
Example
Find the isothermic compressibility of an ideal gas.

Solution
If PV = k (n is constant for our purposes, T is constant because of the
word isothermic, and R really is constant), then

                   dP        dV      dV    V
                      · V + P = 0 =⇒    =−
                   dP        dP      dP    P
So
                                   1 dV        1
                           β=− ·           =
                                   V dP        P
Compressibility and pressure are inversely related.




                                                      .   .   .   .       .   .
Nonideal gasses
Not that there’s anything wrong with that


   Example
   The van der Waals equation                                                 H
                                                                              ..
   makes fewer simplifications:
                                                                       O.
    (         )                                                        . xygen . .
                                                                               H
           n2
      P + a 2 (V − nb) = nRT,                                  .
           V                                          H
                                                      ..
                                            O.                     H
                                                                   . ydrogen bonds
                                            . xygen
   where P is the pressure, V the
                                                      H
                                                      ..
   volume, T the temperature, n                                .
   the number of moles of the
                                                                       O.
                                                                       . xygen . .
                                                                               H
   gas, R a constant, a is a
   measure of attraction between
                                                                              H
                                                                              ..
   particles of the gas, and b a
   measure of particle size.

                                                 .         .       .      .        .   .
Nonideal gasses
Not that there’s anything wrong with that



     Example
     The van der Waals equation
     makes fewer simplifications:
      (         )
             n2
        P + a 2 (V − nb) = nRT,
             V
     where P is the pressure, V the
     volume, T the temperature, n
     the number of moles of the
     gas, R a constant, a is a
     measure of attraction between
     particles of the gas, and b a
     measure of particle size.                                      .
.
Image credit: Wikimedia Commons
                                            .   .   .   .   .   .
Let’s find the compressibility of a van der Waals gas. Differentiating
the van der Waals equation by treating V as a function of P gives
           (       )                   (            )
                an2 dV                      2an2 dV
                          + (V − bn) 1 − 3
             P+ 2                                      = 0,
                      dP                     V dP
                 V




                                                .   .    .    .    .    .
Let’s find the compressibility of a van der Waals gas. Differentiating
the van der Waals equation by treating V as a function of P gives
           (       )                   (            )
                an2 dV                      2an2 dV
                          + (V − bn) 1 − 3
             P+ 2                                      = 0,
                      dP                     V dP
                 V
so
                                   V2 (V − nb)
                        1 dV
                 β=−         =
                               2abn3 − an2 V + PV3
                        V dP




                                                .   .    .    .    .    .
Let’s find the compressibility of a van der Waals gas. Differentiating
the van der Waals equation by treating V as a function of P gives
           (       )                   (            )
                an2 dV                      2an2 dV
                          + (V − bn) 1 − 3
             P+ 2                                      = 0,
                      dP                     V dP
                 V
so
                                     V2 (V − nb)
                          1 dV
                 β=−           =
                                 2abn3 − an2 V + PV3
                          V dP

     What if a = b = 0?




                                                .   .    .    .    .    .
Let’s find the compressibility of a van der Waals gas. Differentiating
the van der Waals equation by treating V as a function of P gives
           (       )                   (            )
                an2 dV                      2an2 dV
                          + (V − bn) 1 − 3
             P+ 2                                      = 0,
                      dP                     V dP
                 V
so
                                     V2 (V − nb)
                          1 dV
                 β=−           =
                                 2abn3 − an2 V + PV3
                          V dP

     What if a = b = 0?
                                                          dβ
     Without taking the derivative, what is the sign of      ?
                                                          db




                                                .   .      .     .   .   .
Let’s find the compressibility of a van der Waals gas. Differentiating
the van der Waals equation by treating V as a function of P gives
           (       )                   (            )
                an2 dV                      2an2 dV
                          + (V − bn) 1 − 3
             P+ 2                                      = 0,
                      dP                     V dP
                 V
so
                                     V2 (V − nb)
                          1 dV
                 β=−           =
                                 2abn3 − an2 V + PV3
                          V dP

     What if a = b = 0?
                                                        dβ
     Without taking the derivative, what is the sign of    ?
                                                        db
                                                        dβ
     Without taking the derivative, what is the sign of    ?
                                                        da



                                                .   .     .    .   .    .
Nasty derivatives




                (2abn3 − an2 V + PV3 )(nV2 ) − (nbV2 − V3 )(2an3 )
          dβ
             =−
                              (2abn3 − an2 V + PV3 )2
          db
                        (2         )
                    nV3 an + PV2
             = −(                     )2 < 0
                  PV3 + an2 (2bn − V)

                          n2 (bn − V)(2bn − V)V2
                      dβ
                         =(                     )2 > 0
                      da    PV3 + an2 (2bn − V)
       (as long as V > 2nb, and it’s probably true that V ≫ 2nb).



                                                 .    .    .    .    .   .
Outline



   The big idea, by example


   Examples
      Vertical and Horizontal Tangents
      Chemistry


   The power rule for rational powers




                                         .   .   .   .   .   .
Using implicit differentiation to find derivatives



   Example
                   √
          dy
             if y = x.
   Find
          dx




                                        .   .   .   .   .   .
Using implicit differentiation to find derivatives



   Example
                   √
          dy
             if y = x.
   Find
          dx
   Solution
         √
   If y =   x, then
                                  y2 = x,
   so
                           dy        dy   1    1
                                             = √.
                              = 1 =⇒    =
                      2y
                           dx        dx   2y  2x




                                             .   .   .   .   .   .
The power rule for rational numbers

   Example
          dy
             if y = xp/q , where p and q are integers.
   Find
          dx




                                                     .   .   .   .   .   .
The power rule for rational numbers

   Example
          dy
             if y = xp/q , where p and q are integers.
   Find
          dx
   Solution
   We have
                                                    p xp−1
                                  dy            dy
                                                   = · q−1
             yq = xp =⇒ qyq−1        = pxp−1 =⇒
                                  dx            dx  qy




                                                     .   .   .   .   .   .
The power rule for rational numbers

   Example
          dy
             if y = xp/q , where p and q are integers.
   Find
          dx
   Solution
   We have
                                                    p xp−1
                                  dy            dy
                                                   = · q−1
             yq = xp =⇒ qyq−1        = pxp−1 =⇒
                                  dx            dx  qy

   Now yq−1 = xp(q−1)/q = xp−p/q so

                         xp−1
                              = xp−1−(p−p/q) = xp/q−1
                         yq−1



                                                     .   .   .   .   .   .

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Lesson 12: Implicit Differentiation

  • 1. Section 2.6 Implicit Differentiation V63.0121, Calculus I February 24/25, 2009 Announcements Midterm in class March 4/5 ALEKS due Friday, 11:59pm . . Image credit: Telstar Logistics . . . . . .
  • 2. Outline The big idea, by example Examples Vertical and Horizontal Tangents Chemistry The power rule for rational powers . . . . . .
  • 3. y . Motivating Example Problem Find the slope of the line which is tangent to the curve . x . 2 2 x +y =1 at the point (3/5, −4/5). . . . . . .
  • 4. y . Motivating Example Problem Find the slope of the line which is tangent to the curve . x . 2 2 x +y =1 at the point (3/5, −4/5). . . . . . .
  • 5. y . Motivating Example Problem Find the slope of the line which is tangent to the curve . x . 2 2 x +y =1 at the point (3/5, −4/5). . . . . . . .
  • 6. y . Motivating Example Problem Find the slope of the line which is tangent to the curve . x . 2 2 x +y =1 at the point (3/5, −4/5). . Solution (Explicit) √ Isolate: y2 = 1 − x2 =⇒ y = − 1 − x2 . (Why the −?) . . . . . .
  • 7. y . Motivating Example Problem Find the slope of the line which is tangent to the curve . x . 2 2 x +y =1 at the point (3/5, −4/5). . Solution (Explicit) √ Isolate: y2 = 1 − x2 =⇒ y = − 1 − x2 . (Why the −?) −2x dy x =− √ =√ Differentiate: 2 1 − x2 1 − x2 dx . . . . . .
  • 8. y . Motivating Example Problem Find the slope of the line which is tangent to the curve . x . 2 2 x +y =1 at the point (3/5, −4/5). . Solution (Explicit) √ Isolate: y2 = 1 − x2 =⇒ y = − 1 − x2 . (Why the −?) −2x dy x =− √ =√ Differentiate: 2 1 − x2 1 − x2 dx dy 3/5 3/5 3 =√ = =. Evaluate: 1 − (3/5) dx x=3/5 4/5 4 2 . . . . . .
  • 9. y . Motivating Example Problem Find the slope of the line which is tangent to the curve . x . 2 2 x +y =1 at the point (3/5, −4/5). . Solution (Explicit) √ Isolate: y2 = 1 − x2 =⇒ y = − 1 − x2 . (Why the −?) −2x dy x =− √ =√ Differentiate: 2 1 − x2 1 − x2 dx dy 3/5 3/5 3 =√ = =. Evaluate: 1 − (3/5) dx x=3/5 4/5 4 2 . . . . . .
  • 10. We know that x2 + y2 = 1 does not define y as a function of x, but suppose it did. Suppose we had y = f(x), so that x2 + (f(x))2 = 1 We could differentiate this equation to get 2x + 2f(x) · f′ (x) = 0 We could then solve to get x f′ (x) = − f(x) . . . . . .
  • 11. The beautiful fact (i.e., deep theorem) is that this works! y . “Near” most points on the curve x2 + y2 = 1, the curve resembles the graph of a function. So f(x) is defined “locally” . x . and is differentiable The chain rule then applies for this local . choice. . . . . . .
  • 12. The beautiful fact (i.e., deep theorem) is that this works! y . “Near” most points on the curve x2 + y2 = 1, the curve resembles the graph of a function. So f(x) is defined “locally” . x . and is differentiable The chain rule then applies for this local . choice. . . . . . .
  • 13. The beautiful fact (i.e., deep theorem) is that this works! y . “Near” most points on the curve x2 + y2 = 1, the curve resembles the graph of a function. So f(x) is defined “locally” . x . and is differentiable The chain rule then applies for this local . choice. l .ooks like a function . . . . . .
  • 14. The beautiful fact (i.e., deep theorem) is that this works! y . “Near” most points on the curve x2 + y2 = 1, the . curve resembles the graph of a function. So f(x) is defined “locally” . x . and is differentiable The chain rule then applies for this local choice. . . . . . .
  • 15. The beautiful fact (i.e., deep theorem) is that this works! y . “Near” most points on the curve x2 + y2 = 1, the . curve resembles the graph of a function. So f(x) is defined “locally” . x . and is differentiable The chain rule then applies for this local choice. . . . . . .
  • 16. The beautiful fact (i.e., deep theorem) is that this works! y . “Near” most points on the curve x2 + y2 = 1, the . curve resembles the graph of a function. l .ooks like a function So f(x) is defined “locally” . x . and is differentiable The chain rule then applies for this local choice. . . . . . .
  • 17. The beautiful fact (i.e., deep theorem) is that this works! y . “Near” most points on the curve x2 + y2 = 1, the curve resembles the graph of a function. So f(x) is defined “locally” . . x . and is differentiable The chain rule then applies for this local choice. . . . . . .
  • 18. The beautiful fact (i.e., deep theorem) is that this works! y . “Near” most points on the curve x2 + y2 = 1, the curve resembles the graph of a function. So f(x) is defined “locally” . . x . and is differentiable The chain rule then applies for this local choice. . . . . . .
  • 19. The beautiful fact (i.e., deep theorem) is that this works! y . “Near” most points on the curve x2 + y2 = 1, the curve resembles the graph of a function. So f(x) is defined “locally” . . x . and is differentiable . The chain rule then does not look like a applies for this local function, but that’s choice. OK—there are only two points like this . . . . . .
  • 20. Problem Find the slope of the line which is tangent to the curve x2 + y2 = 1 at the point (3/5, −4/5). Solution (Implicit, with Leibniz notation) Differentiate. Remember y is assumed to be a function of x: dy 2x + 2y = 0, dx dy Isolate : dx dy x =− . dx y Evaluate: dy 3/5 3 = =. dx ( 3 ,− 4 ) 4/5 4 5 5 . . . . . .
  • 21. Summary y . If a relation is given between x and y, “Most of the time” “at most places” y can be assumed to . be a function of x . we may differentiate the relation as is dy Solving for does give the dx slope of the tangent line to the curve at a point on the curve. . . . . . .
  • 22. Mnemonic Explicit Implicit y = f(x) F(x, y) = k . . Image credit: Walsh . . . . . .
  • 23. Outline The big idea, by example Examples Vertical and Horizontal Tangents Chemistry The power rule for rational powers . . . . . .
  • 24. Example Find the equation of the line tangent to the curve . y2 = x2 (x + 1) = x3 + x2 at the point (3, −6). . . . . . . .
  • 25. Example Find the equation of the line tangent to the curve . y2 = x2 (x + 1) = x3 + x2 at the point (3, −6). . Solution Differentiating the expression implicitly with respect to x gives 3x2 + 2x dy dy 2y = 3x2 + 2x, so = , and dx dx 2y 3 · 32 + 2 · 3 dy 11 =− . = dx 2(−6) 4 (3,−6) . . . . . .
  • 26. Example Find the equation of the line tangent to the curve . y2 = x2 (x + 1) = x3 + x2 at the point (3, −6). . Solution Differentiating the expression implicitly with respect to x gives 3x2 + 2x dy dy 2y = 3x2 + 2x, so = , and dx dx 2y 3 · 32 + 2 · 3 dy 11 =− . = dx 2(−6) 4 (3,−6) 11 Thus the equation of the tangent line is y + 6 = − (x − 3). 4 . . . . . .
  • 27. Example Find the horizontal tangent lines to the same curve: y2 = x3 + x2 . . . . . .
  • 28. Example Find the horizontal tangent lines to the same curve: y2 = x3 + x2 Solution . . . . . .
  • 29. Example Find the horizontal tangent lines to the same curve: y2 = x3 + x2 Solution We solve for dy/dx = 0: 3x2 + 2x = 0 =⇒ 3x2 + 2x = 0 =⇒ x(3x + 2) = 0 2y . . . . . .
  • 30. Example Find the horizontal tangent lines to the same curve: y2 = x3 + x2 Solution We solve for dy/dx = 0: 3x2 + 2x = 0 =⇒ 3x2 + 2x = 0 =⇒ x(3x + 2) = 0 2y The possible solution x = 0 leads to y = 0, which is not a smooth point of the function (the denominator in dy/dx becomes 0). . . . . . .
  • 31. Example Find the horizontal tangent lines to the same curve: y2 = x3 + x2 Solution We solve for dy/dx = 0: 3x2 + 2x = 0 =⇒ 3x2 + 2x = 0 =⇒ x(3x + 2) = 0 2y The possible solution x = 0 leads to y = 0, which is not a smooth point of the function (the denominator in dy/dx becomes 0). The possible solution x = − 2 yields y = ± 3√3 . 2 3 . . . . . .
  • 32. Example Find the vertical tangent lines to the same curve: y2 = x3 + x2 . . . . . .
  • 33. Example Find the vertical tangent lines to the same curve: y2 = x3 + x2 Solution dx = 0. Tangent lines are vertical when dy Differentiating x implicitly as a function of y gives dx dx 2y = 3x2 + 2x , so dy dy dx 2y =2 3x + 2x dy . . . . . .
  • 34. Example Find the vertical tangent lines to the same curve: y2 = x3 + x2 Solution dx = 0. Tangent lines are vertical when dy Differentiating x implicitly as a function of y gives dx dx 2y = 3x2 + 2x , so dy dy dx 2y =2 3x + 2x dy This is 0 only when y = 0. . . . . . .
  • 35. Example Find the vertical tangent lines to the same curve: y2 = x3 + x2 Solution dx = 0. Tangent lines are vertical when dy Differentiating x implicitly as a function of y gives dx dx 2y = 3x2 + 2x , so dy dy dx 2y =2 3x + 2x dy This is 0 only when y = 0. We get the false solution x = 0 and the real solution x = −1. . . . . . .
  • 36. Ideal gases The ideal gas law relates temperature, pressure, and volume of a gas: PV = nRT (R is a constant, n is the amount of gas in moles) . . Image credit: Scott Beale / Laughing Squid . . . . . .
  • 37. . Definition The isothermic compressibility of a fluid is defined by dV 1 β=− dP V with temperature held constant. . Image credit: Neil Better . . . . . .
  • 38. . Definition The isothermic compressibility of a fluid is defined by dV 1 β=− dP V with temperature held constant. The smaller the β, the “harder” the fluid. . Image credit: Neil Better . . . . . .
  • 39. Example Find the isothermic compressibility of an ideal gas. . . . . . .
  • 40. Example Find the isothermic compressibility of an ideal gas. Solution If PV = k (n is constant for our purposes, T is constant because of the word isothermic, and R really is constant), then dP dV dV V · V + P = 0 =⇒ =− dP dP dP P So 1 dV 1 β=− · = V dP P Compressibility and pressure are inversely related. . . . . . .
  • 41. Nonideal gasses Not that there’s anything wrong with that Example The van der Waals equation H .. makes fewer simplifications: O. ( ) . xygen . . H n2 P + a 2 (V − nb) = nRT, . V H .. O. H . ydrogen bonds . xygen where P is the pressure, V the H .. volume, T the temperature, n . the number of moles of the O. . xygen . . H gas, R a constant, a is a measure of attraction between H .. particles of the gas, and b a measure of particle size. . . . . . .
  • 42. Nonideal gasses Not that there’s anything wrong with that Example The van der Waals equation makes fewer simplifications: ( ) n2 P + a 2 (V − nb) = nRT, V where P is the pressure, V the volume, T the temperature, n the number of moles of the gas, R a constant, a is a measure of attraction between particles of the gas, and b a measure of particle size. . . Image credit: Wikimedia Commons . . . . . .
  • 43. Let’s find the compressibility of a van der Waals gas. Differentiating the van der Waals equation by treating V as a function of P gives ( ) ( ) an2 dV 2an2 dV + (V − bn) 1 − 3 P+ 2 = 0, dP V dP V . . . . . .
  • 44. Let’s find the compressibility of a van der Waals gas. Differentiating the van der Waals equation by treating V as a function of P gives ( ) ( ) an2 dV 2an2 dV + (V − bn) 1 − 3 P+ 2 = 0, dP V dP V so V2 (V − nb) 1 dV β=− = 2abn3 − an2 V + PV3 V dP . . . . . .
  • 45. Let’s find the compressibility of a van der Waals gas. Differentiating the van der Waals equation by treating V as a function of P gives ( ) ( ) an2 dV 2an2 dV + (V − bn) 1 − 3 P+ 2 = 0, dP V dP V so V2 (V − nb) 1 dV β=− = 2abn3 − an2 V + PV3 V dP What if a = b = 0? . . . . . .
  • 46. Let’s find the compressibility of a van der Waals gas. Differentiating the van der Waals equation by treating V as a function of P gives ( ) ( ) an2 dV 2an2 dV + (V − bn) 1 − 3 P+ 2 = 0, dP V dP V so V2 (V − nb) 1 dV β=− = 2abn3 − an2 V + PV3 V dP What if a = b = 0? dβ Without taking the derivative, what is the sign of ? db . . . . . .
  • 47. Let’s find the compressibility of a van der Waals gas. Differentiating the van der Waals equation by treating V as a function of P gives ( ) ( ) an2 dV 2an2 dV + (V − bn) 1 − 3 P+ 2 = 0, dP V dP V so V2 (V − nb) 1 dV β=− = 2abn3 − an2 V + PV3 V dP What if a = b = 0? dβ Without taking the derivative, what is the sign of ? db dβ Without taking the derivative, what is the sign of ? da . . . . . .
  • 48. Nasty derivatives (2abn3 − an2 V + PV3 )(nV2 ) − (nbV2 − V3 )(2an3 ) dβ =− (2abn3 − an2 V + PV3 )2 db (2 ) nV3 an + PV2 = −( )2 < 0 PV3 + an2 (2bn − V) n2 (bn − V)(2bn − V)V2 dβ =( )2 > 0 da PV3 + an2 (2bn − V) (as long as V > 2nb, and it’s probably true that V ≫ 2nb). . . . . . .
  • 49. Outline The big idea, by example Examples Vertical and Horizontal Tangents Chemistry The power rule for rational powers . . . . . .
  • 50. Using implicit differentiation to find derivatives Example √ dy if y = x. Find dx . . . . . .
  • 51. Using implicit differentiation to find derivatives Example √ dy if y = x. Find dx Solution √ If y = x, then y2 = x, so dy dy 1 1 = √. = 1 =⇒ = 2y dx dx 2y 2x . . . . . .
  • 52. The power rule for rational numbers Example dy if y = xp/q , where p and q are integers. Find dx . . . . . .
  • 53. The power rule for rational numbers Example dy if y = xp/q , where p and q are integers. Find dx Solution We have p xp−1 dy dy = · q−1 yq = xp =⇒ qyq−1 = pxp−1 =⇒ dx dx qy . . . . . .
  • 54. The power rule for rational numbers Example dy if y = xp/q , where p and q are integers. Find dx Solution We have p xp−1 dy dy = · q−1 yq = xp =⇒ qyq−1 = pxp−1 =⇒ dx dx qy Now yq−1 = xp(q−1)/q = xp−p/q so xp−1 = xp−1−(p−p/q) = xp/q−1 yq−1 . . . . . .