SlideShare a Scribd company logo
1 of 39
Download to read offline
Lesson 24 (Sections 16.3, 16.7)
               Implicit Differentiation

                            Math 20


                     November 16, 2007

Announcements
   Problem Set 9 on the website. Due November 21.
   There will be class November 21 and homework due
   November 28.
   next OH: Monday 1-2pm, Tuesday 3-4pm
   Midterm II: Thursday, 12/6, 7-8:30pm in Hall A.
   Go Harvard! Beat Yale!
Outline

   Cleanup on Leibniz Rule

   Implicit Differentiation in two dimensions
      The Math 1a way
      Old school Implicit Differentation
      New school Implicit Differentation
      Compare

   Application

   More than two dimensions

   The second derivative
Last Time: the Chain Rule


   Theorem (The Chain Rule, General Version)
   Suppose that u is a differentiable function of the n variables
   x1 , x2 , . . . , xn , and each xi is a differentiable function of the m
   variables t1 , t2 , . . . , tm . Then u is a function of t1 , t2 , . . . , tm and
                  ∂u    ∂u ∂x1    ∂u ∂x2          ∂u ∂xn
                      =         +         + ··· +
                  ∂ti   ∂x1 ∂ti   ∂x2 ∂ti         ∂xn ∂ti
Last Time: the Chain Rule


   Theorem (The Chain Rule, General Version)
   Suppose that u is a differentiable function of the n variables
   x1 , x2 , . . . , xn , and each xi is a differentiable function of the m
   variables t1 , t2 , . . . , tm . Then u is a function of t1 , t2 , . . . , tm and
                  ∂u    ∂u ∂x1    ∂u ∂x2          ∂u ∂xn
                      =         +         + ··· +
                  ∂ti   ∂x1 ∂ti   ∂x2 ∂ti         ∂xn ∂ti

   In summation notation
                                           n
                                 ∂u             ∂u ∂xj
                                     =
                                 ∂ti            ∂xj ∂ti
                                          j=1
Leibniz’s Formula for Integrals
   Fact
   Suppose that f (, t, x), a(t), and b(t) are differentiable functions,
   and let
                                    b(t)
                         F (t) =           f (t, x) dx
                                   a(t)
Leibniz’s Formula for Integrals
   Fact
   Suppose that f (, t, x), a(t), and b(t) are differentiable functions,
   and let
                                    b(t)
                         F (t) =           f (t, x) dx
                                   a(t)

   Then
                                                          b(t)
                                                                 ∂f (t, x)
      F (t) = f (t, b(t))b (t) − f (t, a(t))a (t) +                        dx
                                                         a(t)       ∂t
Leibniz’s Formula for Integrals
   Fact
   Suppose that f (, t, x), a(t), and b(t) are differentiable functions,
   and let
                                    b(t)
                         F (t) =              f (t, x) dx
                                   a(t)

   Then
                                                                 b(t)
                                                                        ∂f (t, x)
      F (t) = f (t, b(t))b (t) − f (t, a(t))a (t) +                               dx
                                                                a(t)       ∂t


   Proof.
   Apply the chain rule to the function
                                              v
                        H(t, u, v ) =             f (t, x) dx
                                          u

   with u = a(t) and v = b(t).
Tree Diagram




                   H


               t   u   v


                   t   t
More about the proof

                                     v
                 H(t, u, v ) =           f (t, x) dx
                                 u
More about the proof

                                          v
                      H(t, u, v ) =           f (t, x) dx
                                      u
   Then by the Fundamental Theorem of Calculus (see Section 10.1)

                  ∂H                  ∂H
                     = f (t, v )         = −f (t, u)
                  ∂v                  ∂u
More about the proof

                                                 v
                       H(t, u, v ) =                 f (t, x) dx
                                             u
   Then by the Fundamental Theorem of Calculus (see Section 10.1)

                   ∂H                        ∂H
                      = f (t, v )               = −f (t, u)
                   ∂v                        ∂u
   Also,
                                        v
                         ∂H                 ∂f
                            =                  (t, x) dx
                         ∂t         u       ∂x
   since t and x are independent variables.
Since F (t) = H(t, a(t), b(t)),

      dF   ∂H     ∂H du ∂H dv
         =      +         +
      dt   ∂t      ∂u dt     ∂v dt
             b(t)
                  ∂f
         =           (t, x) + f (t, b(t))b (t) − f (t, a(t))a (t)
            a(t) ∂x
Application
   Example (Example 16.8 with better notation)
   Let the profit of a firm be π(t). The present value of the future
   profit π(τ ) where τ > t is

                                π(τ )e −r (τ −t) ,

   where r is the discount rate. On a time interval [0, T ], the present
   value of all future profit is
                                      T
                      V (t) =             π(τ )e −r (τ −t) dt.
                                  t

   Find V (t).
Application
   Example (Example 16.8 with better notation)
   Let the profit of a firm be π(t). The present value of the future
   profit π(τ ) where τ > t is

                                π(τ )e −r (τ −t) ,

   where r is the discount rate. On a time interval [0, T ], the present
   value of all future profit is
                                      T
                      V (t) =             π(τ )e −r (τ −t) dt.
                                  t

   Find V (t).

   Answer.

                          V (t) = rV (t) − π(t)
Solution
Since the upper limit is a constant, the only boundary term comes
from the lower limit:
                                               T
                                                   ∂
           V (t) = −π(t)e −r (t−t) +                  π(τ )e −r τ e rt dτ
                                           t       ∂t
                                   T
                 = −π(t) + r           π(τ )e −r τ e rt dτ
                               t
                 = rV (t) − π(t).

This means that
                               π(t) + V (t)
                          r=
                                   V (t)
So if the fraction on the right is less than the rate of return for
another, “safer” investment like bonds, it would be worth more to
sell the business and buy the bonds.
Outline

   Cleanup on Leibniz Rule

   Implicit Differentiation in two dimensions
      The Math 1a way
      Old school Implicit Differentation
      New school Implicit Differentation
      Compare

   Application

   More than two dimensions

   The second derivative
An example

                    4
 Consider the
 utility function
             1 1    3
 u(x, y ) = − −
             x y
 What is the
                    2
 slope of the
 tangent line
 along the
 indifference        1


 curve
 u(x, y ) = −1?
                        1   2   3   4
The Math 1a way


  Solve for y in terms of x and differentiate:
                     1  1              1
                       + = 1 =⇒ y =
                     x  y           1 − 1/x

  So
                    dy      −1          1
                       =      1/x )2
                    dx   (1 −           x2
                              −1              −1
                       = 2       1/x )2
                                        =
                         x (1 −            (x − 1)2
Old school Implicit Differentation




   Differentiate the equation remembering that y is presumed to be a
   function of x:
                              1    1 dy
                           − 2− 2       =0
                             x    y dx
   So
                        dy   y2    y        2
                           =− 2 =−
                        dx   x     x
New school Implicit Differentation

   This is a formalized version of old school: If

                                  F (x, y ) = c

   Then by differentiating the equation and treating y as a function
   of x, we get
                        ∂F     ∂F    dy
                            +              =0
                        ∂x     ∂y    dx F
   So
                             dy              ∂F /∂x
                                        =−
                             dx     F        ∂F /∂x
   The (·)F notation reminds us that y is not explicitly a function of
   x, but if F is held constant we can treat it implicitly so.
Tree diagram



                         F


                   x              y


                                  x

               ∂F   ∂F       dy
                  +                       =0
               ∂x   ∂y       dx       F
The big idea




   Fact
   Along the level curve F (x, y ) = c, the slope of the tangent line is
   given by
                dy       dy           ∂F /∂x       F (x, y )
                    =            =−           =− 1
                dx       dx F         ∂F /∂x       F2 (x, y )
Compare



     Explicitly solving for y is tedious, and sometimes impossible.
     Either implicit method brings out more clearly the important
     fact that (in our example) dy
                                 dx    depends only on the ratio
                                      u
     y/x .

     Old-school implicit differentiation is familiar but (IMO)
     contrived.
     New-school implicit differentiation is systematic and
     generalizable.
Outline

   Cleanup on Leibniz Rule

   Implicit Differentiation in two dimensions
      The Math 1a way
      Old school Implicit Differentation
      New school Implicit Differentation
      Compare

   Application

   More than two dimensions

   The second derivative
Application




   If u(x, y ) is a utility function of two goods, then u(x, y ) = c is a
   indifference curve, and the slope represents the marginal rate of
   substitution:
                                 dy           ux   MUx
                     Ryx = −              =      =
                                 dx   u       uy   MUy
Outline

   Cleanup on Leibniz Rule

   Implicit Differentiation in two dimensions
      The Math 1a way
      Old school Implicit Differentation
      New school Implicit Differentation
      Compare

   Application

   More than two dimensions

   The second derivative
More than two dimensions
   The basic idea is to close your eyes and use the chain rule:
   Example
   Suppose a surface is given by F (x, y , z) = c. If this defines z as a
   function of x and y , find zx and zy .
More than two dimensions
   The basic idea is to close your eyes and use the chain rule:
   Example
   Suppose a surface is given by F (x, y , z) = c. If this defines z as a
   function of x and y , find zx and zy .

   Solution
   Setting F (x, y , z) = c and remembering z is implicitly a function
   of x and y , we get

              ∂F   ∂F      ∂z                  ∂z          Fx
                 +                  = 0 =⇒              =−
              ∂x   ∂z      ∂x   F              ∂x   F      Fz
              ∂F   ∂F      ∂z                  ∂z          Fy
                 +                  = 0 =⇒              =−
              ∂y   ∂z      ∂y   F              ∂y   F      Fz
Tree diagram



                              F


                    x         y       z


                                      x

          ∂F   ∂F   ∂z                ∂z            Fx
             +               = 0 =⇒            =−
          ∂x   ∂z   ∂x   F            ∂x   F        Fz
Example
Suppose production is given by a Cobb-Douglas function

                      P(A, K , L) = AK a Lb

where K is capital, L is labor, and A is technology. Compute the
changes in technology or capital needed to sustain production if
labor decreases.
Example
Suppose production is given by a Cobb-Douglas function

                       P(A, K , L) = AK a Lb

where K is capital, L is labor, and A is technology. Compute the
changes in technology or capital needed to sustain production if
labor decreases.

Solution

             ∂K            PL    AK a bLb−1    b K
                      =−      =−      a−1 Lb
                                             =− ·
             ∂L   P        PK    AaK           a L
             ∂A            PL    AK a bLb−1    bA
                      =−      =−      a Lb
                                            =−
             ∂L   P        PA      K            L

                                                 b       K
So if labor decreases by 1 unit we need either   a   ·   L   more capital or
bA
 L more tech to sustain production.
Outline

   Cleanup on Leibniz Rule

   Implicit Differentiation in two dimensions
      The Math 1a way
      Old school Implicit Differentation
      New school Implicit Differentation
      Compare

   Application

   More than two dimensions

   The second derivative
The second derivative: Derivation
   What is the concavity of an indifference curve? We know

                         dy            Fx    G
                                  =−      =−
                         dx   F        Fy    H

   Then
                                  HG − GH
                         y =−
                                     H2
   Now
                        d ∂F      ∂2F     ∂ 2 F dy
                   G =         =       +
                        dx ∂x     ∂x 2   ∂y ∂x dx
                        ∂ 2F    ∂ 2F    ∂F /∂x
                      =      −
                        ∂x 2   ∂y ∂x ∂F /∂y

   So
                   ∂F ∂ 2 F    ∂ 2 F ∂F
            HG =            −           = Fy Fxx − Fyx Fx
                   ∂y ∂x 2    ∂y ∂x ∂x
Also
          d ∂F       ∂F    ∂ 2 F dy
       H =      =       +
          dx ∂y   ∂x ∂y    ∂y 2 dx
           ∂2F    ∂ 2 F ∂F /∂x
        =       −
          ∂x ∂y   ∂y 2 ∂F /∂y

So
                          Fyy (Fx )2
        GH = Fx Fxy −
                             Fy
                 Fx Fxy Fy − Fyy (Fx )2
             =
                           Fy
Putting this all together we get

                                         Fx Fxy Fy − Fyy (Fx )2
                Fy Fxx − Fyx Fx −
                                                   Fy
        y =−
                                     (Fy )2
                  1
           =−          F (F )2 − 2Fxy Fx Fy + Fyy (Fx )2
                (Fy )3 xx y
                    0     Fx       Fy
               1
           =        Fx    Fxx      Fxy
             (Fy )3
                    Fy    Fxy      Fyy
Example
Along the indifference curve
                              1  1
                                + =c
                              x  y
                                           d
compute (y )u . What does this say about   dx Ryx ?
Example
Along the indifference curve
                                 1  1
                                   + =c
                                 x  y
                                                  d
compute (y )u . What does this say about          dx Ryx ?

Solution
                     1     1
We have u(x, y ) =   x   + y , so

                                          0      −1/x 2 −1/y 2
             d 2y                1
                         =              −1/x 2   2/x 3   0
             dx 2    u       (−1/y 2 )3 −1/y 2    0     −2/y 3
Solution (continued)


                                     0          −1/x 2 −1/y 2
  d 2y                1
             =                     −1/x 2       2/x 3   0
  dx 2   u       (−1/y 2 )3 −1/y 2               0     −2/y 3
                                   −1           −1       2             −1     2    −1
             = −y 6 −                                             −
                                   x2           x2       y3            y2     x3   y2
                               1            1
             = 2y 6                 +
                          x 4y 3         y 4x 3
                    y      3       1   1                 y    3
             =2                      +            = 2c
                    x              x   y                 x

                                                         dy
This is positive, and since Ryx = −                      dx       , we have
                                                              u

                                   d            y             3
                                      Ryx = −2u                   <0
                                   dx           x
So the MRS diminishes with increasing consumption of x.
Bonus: Elasticity of substitution
See Section 16.4



    The elasticity of substitution is the elasticity of the MRS with
    respect to the ratio y/x :

                                               ∂Ryx y/x
                        σyx = εRyx ,(y/x ) =          ·
                                               ∂(y/x ) Ryx

    In our case, Ryx = (y/x )2 , so
                                               y/x
                           σyx = 2 (y/x )              =2
                                            (y/x )2
                                               1       1
    which is why the function u(x, y ) =       x   +   y   is called a constant
    elasticity of substitution function.

More Related Content

What's hot

Stuff You Must Know Cold for the AP Calculus BC Exam!
Stuff You Must Know Cold for the AP Calculus BC Exam!Stuff You Must Know Cold for the AP Calculus BC Exam!
Stuff You Must Know Cold for the AP Calculus BC Exam!
A Jorge Garcia
 
Quantum modes - Ion Cotaescu
Quantum modes - Ion CotaescuQuantum modes - Ion Cotaescu
Quantum modes - Ion Cotaescu
SEENET-MTP
 
Calculus cheat sheet_integrals
Calculus cheat sheet_integralsCalculus cheat sheet_integrals
Calculus cheat sheet_integrals
UrbanX4
 
Euler lagrange equation
Euler lagrange equationEuler lagrange equation
Euler lagrange equation
mufti195
 
Lesson 28: The Fundamental Theorem of Calculus
Lesson 28: The Fundamental Theorem of CalculusLesson 28: The Fundamental Theorem of Calculus
Lesson 28: The Fundamental Theorem of Calculus
Matthew Leingang
 

What's hot (19)

Lesson 24: Implicit Differentiation
Lesson 24: Implicit DifferentiationLesson 24: Implicit Differentiation
Lesson 24: Implicit Differentiation
 
Chapter 5 (maths 3)
Chapter 5 (maths 3)Chapter 5 (maths 3)
Chapter 5 (maths 3)
 
Lesson 20: Derivatives and the Shapes of Curves (slides)
Lesson 20: Derivatives and the Shapes of Curves (slides)Lesson 20: Derivatives and the Shapes of Curves (slides)
Lesson 20: Derivatives and the Shapes of Curves (slides)
 
Lesson 8: Basic Differentation Rules (slides)
Lesson 8: Basic Differentation Rules (slides)Lesson 8: Basic Differentation Rules (slides)
Lesson 8: Basic Differentation Rules (slides)
 
Stuff You Must Know Cold for the AP Calculus BC Exam!
Stuff You Must Know Cold for the AP Calculus BC Exam!Stuff You Must Know Cold for the AP Calculus BC Exam!
Stuff You Must Know Cold for the AP Calculus BC Exam!
 
ON OPTIMALITY OF THE INDEX OF SUM, PRODUCT, MAXIMUM, AND MINIMUM OF FINITE BA...
ON OPTIMALITY OF THE INDEX OF SUM, PRODUCT, MAXIMUM, AND MINIMUM OF FINITE BA...ON OPTIMALITY OF THE INDEX OF SUM, PRODUCT, MAXIMUM, AND MINIMUM OF FINITE BA...
ON OPTIMALITY OF THE INDEX OF SUM, PRODUCT, MAXIMUM, AND MINIMUM OF FINITE BA...
 
Harmonic Analysis and Deep Learning
Harmonic Analysis and Deep LearningHarmonic Analysis and Deep Learning
Harmonic Analysis and Deep Learning
 
Quantum modes - Ion Cotaescu
Quantum modes - Ion CotaescuQuantum modes - Ion Cotaescu
Quantum modes - Ion Cotaescu
 
Lesson 18: Maximum and Minimum Values (slides)
Lesson 18: Maximum and Minimum Values (slides)Lesson 18: Maximum and Minimum Values (slides)
Lesson 18: Maximum and Minimum Values (slides)
 
Calculus cheat sheet_integrals
Calculus cheat sheet_integralsCalculus cheat sheet_integrals
Calculus cheat sheet_integrals
 
Chapter 4 (maths 3)
Chapter 4 (maths 3)Chapter 4 (maths 3)
Chapter 4 (maths 3)
 
Fourier series
Fourier seriesFourier series
Fourier series
 
Euler lagrange equation
Euler lagrange equationEuler lagrange equation
Euler lagrange equation
 
Lesson 31: Evaluating Definite Integrals
Lesson 31: Evaluating Definite IntegralsLesson 31: Evaluating Definite Integrals
Lesson 31: Evaluating Definite Integrals
 
Hw2 s
Hw2 sHw2 s
Hw2 s
 
Rao-Blackwellisation schemes for accelerating Metropolis-Hastings algorithms
Rao-Blackwellisation schemes for accelerating Metropolis-Hastings algorithmsRao-Blackwellisation schemes for accelerating Metropolis-Hastings algorithms
Rao-Blackwellisation schemes for accelerating Metropolis-Hastings algorithms
 
Common derivatives integrals_reduced
Common derivatives integrals_reducedCommon derivatives integrals_reduced
Common derivatives integrals_reduced
 
Chapter 2 (maths 3)
Chapter 2 (maths 3)Chapter 2 (maths 3)
Chapter 2 (maths 3)
 
Lesson 28: The Fundamental Theorem of Calculus
Lesson 28: The Fundamental Theorem of CalculusLesson 28: The Fundamental Theorem of Calculus
Lesson 28: The Fundamental Theorem of Calculus
 

Viewers also liked

Lesson20 Tangent Planes Slides+Notes
Lesson20   Tangent Planes Slides+NotesLesson20   Tangent Planes Slides+Notes
Lesson20 Tangent Planes Slides+Notes
Matthew Leingang
 
Lesson 16: Implicit Differentiation
Lesson 16: Implicit DifferentiationLesson 16: Implicit Differentiation
Lesson 16: Implicit Differentiation
Matthew Leingang
 

Viewers also liked (18)

Lesson 26: Optimization II: Data Fitting
Lesson 26: Optimization II: Data FittingLesson 26: Optimization II: Data Fitting
Lesson 26: Optimization II: Data Fitting
 
Lesson 25: Unconstrained Optimization I
Lesson 25: Unconstrained Optimization ILesson 25: Unconstrained Optimization I
Lesson 25: Unconstrained Optimization I
 
Lesson 29: Areas
Lesson 29: AreasLesson 29: Areas
Lesson 29: Areas
 
Lesson20 Tangent Planes Slides+Notes
Lesson20   Tangent Planes Slides+NotesLesson20   Tangent Planes Slides+Notes
Lesson20 Tangent Planes Slides+Notes
 
Midterm II Review
Midterm II ReviewMidterm II Review
Midterm II Review
 
Lesson 28: Lagrange Multipliers II
Lesson 28: Lagrange  Multipliers IILesson 28: Lagrange  Multipliers II
Lesson 28: Lagrange Multipliers II
 
Lesson 32: The Fundamental Theorem Of Calculus
Lesson 32: The Fundamental Theorem Of CalculusLesson 32: The Fundamental Theorem Of Calculus
Lesson 32: The Fundamental Theorem Of Calculus
 
Lesson 25: Indeterminate Forms and L'Hôpital's Rule
Lesson 25: Indeterminate Forms and L'Hôpital's RuleLesson 25: Indeterminate Forms and L'Hôpital's Rule
Lesson 25: Indeterminate Forms and L'Hôpital's Rule
 
Lesson 22: Quadratic Forms
Lesson 22: Quadratic FormsLesson 22: Quadratic Forms
Lesson 22: Quadratic Forms
 
Lesson 23: The Chain Rule
Lesson 23: The Chain RuleLesson 23: The Chain Rule
Lesson 23: The Chain Rule
 
Lesson 27: Lagrange Multipliers I
Lesson 27: Lagrange Multipliers ILesson 27: Lagrange Multipliers I
Lesson 27: Lagrange Multipliers I
 
Midterm II Review Session Slides
Midterm II Review Session SlidesMidterm II Review Session Slides
Midterm II Review Session Slides
 
Lesson 30: The Definite Integral
Lesson 30: The  Definite  IntegralLesson 30: The  Definite  Integral
Lesson 30: The Definite Integral
 
Lesson 34: Introduction To Game Theory
Lesson 34: Introduction To Game TheoryLesson 34: Introduction To Game Theory
Lesson 34: Introduction To Game Theory
 
Lesson 19: Related Rates
Lesson 19: Related RatesLesson 19: Related Rates
Lesson 19: Related Rates
 
Lesson 16: Implicit Differentiation
Lesson 16: Implicit DifferentiationLesson 16: Implicit Differentiation
Lesson 16: Implicit Differentiation
 
Lesson 21: Partial Derivatives in Economics
Lesson 21: Partial Derivatives in EconomicsLesson 21: Partial Derivatives in Economics
Lesson 21: Partial Derivatives in Economics
 
Lesson 30: Duality In Linear Programming
Lesson 30: Duality In Linear ProgrammingLesson 30: Duality In Linear Programming
Lesson 30: Duality In Linear Programming
 

Similar to Lesson24 Implicit Differentiation Slides

3.7 applications of tangent lines
3.7 applications of tangent lines3.7 applications of tangent lines
3.7 applications of tangent lines
math265
 
Stochastic Control and Information Theoretic Dualities (Complete Version)
Stochastic Control and Information Theoretic Dualities (Complete Version)Stochastic Control and Information Theoretic Dualities (Complete Version)
Stochastic Control and Information Theoretic Dualities (Complete Version)
Haruki Nishimura
 
Stochastic Calculus, Summer 2014, July 22,Lecture 7Con.docx
Stochastic Calculus, Summer 2014, July 22,Lecture 7Con.docxStochastic Calculus, Summer 2014, July 22,Lecture 7Con.docx
Stochastic Calculus, Summer 2014, July 22,Lecture 7Con.docx
dessiechisomjj4
 
11.[104 111]analytical solution for telegraph equation by modified of sumudu ...
11.[104 111]analytical solution for telegraph equation by modified of sumudu ...11.[104 111]analytical solution for telegraph equation by modified of sumudu ...
11.[104 111]analytical solution for telegraph equation by modified of sumudu ...
Alexander Decker
 
11.solution of linear and nonlinear partial differential equations using mixt...
11.solution of linear and nonlinear partial differential equations using mixt...11.solution of linear and nonlinear partial differential equations using mixt...
11.solution of linear and nonlinear partial differential equations using mixt...
Alexander Decker
 

Similar to Lesson24 Implicit Differentiation Slides (20)

Desktop
DesktopDesktop
Desktop
 
Desktop
DesktopDesktop
Desktop
 
3.7 applications of tangent lines
3.7 applications of tangent lines3.7 applications of tangent lines
3.7 applications of tangent lines
 
Lesson 7: Vector-valued functions
Lesson 7: Vector-valued functionsLesson 7: Vector-valued functions
Lesson 7: Vector-valued functions
 
160511 hasegawa lab_seminar
160511 hasegawa lab_seminar160511 hasegawa lab_seminar
160511 hasegawa lab_seminar
 
On Twisted Paraproducts and some other Multilinear Singular Integrals
On Twisted Paraproducts and some other Multilinear Singular IntegralsOn Twisted Paraproducts and some other Multilinear Singular Integrals
On Twisted Paraproducts and some other Multilinear Singular Integrals
 
research paper publication
research paper publicationresearch paper publication
research paper publication
 
Stochastic Control and Information Theoretic Dualities (Complete Version)
Stochastic Control and Information Theoretic Dualities (Complete Version)Stochastic Control and Information Theoretic Dualities (Complete Version)
Stochastic Control and Information Theoretic Dualities (Complete Version)
 
Coincidence points for mappings under generalized contraction
Coincidence points for mappings under generalized contractionCoincidence points for mappings under generalized contraction
Coincidence points for mappings under generalized contraction
 
Congrès SMAI 2019
Congrès SMAI 2019Congrès SMAI 2019
Congrès SMAI 2019
 
Lesson 26: The Fundamental Theorem of Calculus (slides)
Lesson 26: The Fundamental Theorem of Calculus (slides)Lesson 26: The Fundamental Theorem of Calculus (slides)
Lesson 26: The Fundamental Theorem of Calculus (slides)
 
Lesson 26: The Fundamental Theorem of Calculus (slides)
Lesson 26: The Fundamental Theorem of Calculus (slides)Lesson 26: The Fundamental Theorem of Calculus (slides)
Lesson 26: The Fundamental Theorem of Calculus (slides)
 
AJMS_403_22.pdf
AJMS_403_22.pdfAJMS_403_22.pdf
AJMS_403_22.pdf
 
Chain rule
Chain ruleChain rule
Chain rule
 
Btech admission in india
Btech admission in indiaBtech admission in india
Btech admission in india
 
Stochastic Calculus, Summer 2014, July 22,Lecture 7Con.docx
Stochastic Calculus, Summer 2014, July 22,Lecture 7Con.docxStochastic Calculus, Summer 2014, July 22,Lecture 7Con.docx
Stochastic Calculus, Summer 2014, July 22,Lecture 7Con.docx
 
11.[104 111]analytical solution for telegraph equation by modified of sumudu ...
11.[104 111]analytical solution for telegraph equation by modified of sumudu ...11.[104 111]analytical solution for telegraph equation by modified of sumudu ...
11.[104 111]analytical solution for telegraph equation by modified of sumudu ...
 
11.solution of linear and nonlinear partial differential equations using mixt...
11.solution of linear and nonlinear partial differential equations using mixt...11.solution of linear and nonlinear partial differential equations using mixt...
11.solution of linear and nonlinear partial differential equations using mixt...
 
Solution of linear and nonlinear partial differential equations using mixture...
Solution of linear and nonlinear partial differential equations using mixture...Solution of linear and nonlinear partial differential equations using mixture...
Solution of linear and nonlinear partial differential equations using mixture...
 
Geometric and viscosity solutions for the Cauchy problem of first order
Geometric and viscosity solutions for the Cauchy problem of first orderGeometric and viscosity solutions for the Cauchy problem of first order
Geometric and viscosity solutions for the Cauchy problem of first order
 

More from Matthew Leingang

More from Matthew Leingang (20)

Making Lesson Plans
Making Lesson PlansMaking Lesson Plans
Making Lesson Plans
 
Streamlining assessment, feedback, and archival with auto-multiple-choice
Streamlining assessment, feedback, and archival with auto-multiple-choiceStreamlining assessment, feedback, and archival with auto-multiple-choice
Streamlining assessment, feedback, and archival with auto-multiple-choice
 
Electronic Grading of Paper Assessments
Electronic Grading of Paper AssessmentsElectronic Grading of Paper Assessments
Electronic Grading of Paper Assessments
 
Lesson 27: Integration by Substitution (handout)
Lesson 27: Integration by Substitution (handout)Lesson 27: Integration by Substitution (handout)
Lesson 27: Integration by Substitution (handout)
 
Lesson 26: The Fundamental Theorem of Calculus (handout)
Lesson 26: The Fundamental Theorem of Calculus (handout)Lesson 26: The Fundamental Theorem of Calculus (handout)
Lesson 26: The Fundamental Theorem of Calculus (handout)
 
Lesson 25: Evaluating Definite Integrals (slides)
Lesson 25: Evaluating Definite Integrals (slides)Lesson 25: Evaluating Definite Integrals (slides)
Lesson 25: Evaluating Definite Integrals (slides)
 
Lesson 25: Evaluating Definite Integrals (handout)
Lesson 25: Evaluating Definite Integrals (handout)Lesson 25: Evaluating Definite Integrals (handout)
Lesson 25: Evaluating Definite Integrals (handout)
 
Lesson 24: Areas and Distances, The Definite Integral (handout)
Lesson 24: Areas and Distances, The Definite Integral (handout)Lesson 24: Areas and Distances, The Definite Integral (handout)
Lesson 24: Areas and Distances, The Definite Integral (handout)
 
Lesson 24: Areas and Distances, The Definite Integral (slides)
Lesson 24: Areas and Distances, The Definite Integral (slides)Lesson 24: Areas and Distances, The Definite Integral (slides)
Lesson 24: Areas and Distances, The Definite Integral (slides)
 
Lesson 23: Antiderivatives (slides)
Lesson 23: Antiderivatives (slides)Lesson 23: Antiderivatives (slides)
Lesson 23: Antiderivatives (slides)
 
Lesson 22: Optimization Problems (slides)
Lesson 22: Optimization Problems (slides)Lesson 22: Optimization Problems (slides)
Lesson 22: Optimization Problems (slides)
 
Lesson 22: Optimization Problems (handout)
Lesson 22: Optimization Problems (handout)Lesson 22: Optimization Problems (handout)
Lesson 22: Optimization Problems (handout)
 
Lesson 21: Curve Sketching (slides)
Lesson 21: Curve Sketching (slides)Lesson 21: Curve Sketching (slides)
Lesson 21: Curve Sketching (slides)
 
Lesson 21: Curve Sketching (handout)
Lesson 21: Curve Sketching (handout)Lesson 21: Curve Sketching (handout)
Lesson 21: Curve Sketching (handout)
 
Lesson 20: Derivatives and the Shapes of Curves (handout)
Lesson 20: Derivatives and the Shapes of Curves (handout)Lesson 20: Derivatives and the Shapes of Curves (handout)
Lesson 20: Derivatives and the Shapes of Curves (handout)
 
Lesson 19: The Mean Value Theorem (slides)
Lesson 19: The Mean Value Theorem (slides)Lesson 19: The Mean Value Theorem (slides)
Lesson 19: The Mean Value Theorem (slides)
 
Lesson 17: Indeterminate forms and l'Hôpital's Rule (slides)
Lesson 17: Indeterminate forms and l'Hôpital's Rule (slides)Lesson 17: Indeterminate forms and l'Hôpital's Rule (slides)
Lesson 17: Indeterminate forms and l'Hôpital's Rule (slides)
 
Lesson 18: Maximum and Minimum Values (handout)
Lesson 18: Maximum and Minimum Values (handout)Lesson 18: Maximum and Minimum Values (handout)
Lesson 18: Maximum and Minimum Values (handout)
 
Lesson 17: Indeterminate forms and l'Hôpital's Rule (handout)
Lesson 17: Indeterminate forms and l'Hôpital's Rule (handout)Lesson 17: Indeterminate forms and l'Hôpital's Rule (handout)
Lesson 17: Indeterminate forms and l'Hôpital's Rule (handout)
 
Lesson 16: Inverse Trigonometric Functions (slides)
Lesson 16: Inverse Trigonometric Functions (slides)Lesson 16: Inverse Trigonometric Functions (slides)
Lesson 16: Inverse Trigonometric Functions (slides)
 

Recently uploaded

Quick Doctor In Kuwait +2773`7758`557 Kuwait Doha Qatar Dubai Abu Dhabi Sharj...
Quick Doctor In Kuwait +2773`7758`557 Kuwait Doha Qatar Dubai Abu Dhabi Sharj...Quick Doctor In Kuwait +2773`7758`557 Kuwait Doha Qatar Dubai Abu Dhabi Sharj...
Quick Doctor In Kuwait +2773`7758`557 Kuwait Doha Qatar Dubai Abu Dhabi Sharj...
daisycvs
 
Challenges and Opportunities: A Qualitative Study on Tax Compliance in Pakistan
Challenges and Opportunities: A Qualitative Study on Tax Compliance in PakistanChallenges and Opportunities: A Qualitative Study on Tax Compliance in Pakistan
Challenges and Opportunities: A Qualitative Study on Tax Compliance in Pakistan
vineshkumarsajnani12
 
Al Mizhar Dubai Escorts +971561403006 Escorts Service In Al Mizhar
Al Mizhar Dubai Escorts +971561403006 Escorts Service In Al MizharAl Mizhar Dubai Escorts +971561403006 Escorts Service In Al Mizhar
Al Mizhar Dubai Escorts +971561403006 Escorts Service In Al Mizhar
allensay1
 

Recently uploaded (20)

Putting the SPARK into Virtual Training.pptx
Putting the SPARK into Virtual Training.pptxPutting the SPARK into Virtual Training.pptx
Putting the SPARK into Virtual Training.pptx
 
PARK STREET 💋 Call Girl 9827461493 Call Girls in Escort service book now
PARK STREET 💋 Call Girl 9827461493 Call Girls in  Escort service book nowPARK STREET 💋 Call Girl 9827461493 Call Girls in  Escort service book now
PARK STREET 💋 Call Girl 9827461493 Call Girls in Escort service book now
 
Quick Doctor In Kuwait +2773`7758`557 Kuwait Doha Qatar Dubai Abu Dhabi Sharj...
Quick Doctor In Kuwait +2773`7758`557 Kuwait Doha Qatar Dubai Abu Dhabi Sharj...Quick Doctor In Kuwait +2773`7758`557 Kuwait Doha Qatar Dubai Abu Dhabi Sharj...
Quick Doctor In Kuwait +2773`7758`557 Kuwait Doha Qatar Dubai Abu Dhabi Sharj...
 
Challenges and Opportunities: A Qualitative Study on Tax Compliance in Pakistan
Challenges and Opportunities: A Qualitative Study on Tax Compliance in PakistanChallenges and Opportunities: A Qualitative Study on Tax Compliance in Pakistan
Challenges and Opportunities: A Qualitative Study on Tax Compliance in Pakistan
 
Uneak White's Personal Brand Exploration Presentation
Uneak White's Personal Brand Exploration PresentationUneak White's Personal Brand Exploration Presentation
Uneak White's Personal Brand Exploration Presentation
 
Ooty Call Gril 80022//12248 Only For Sex And High Profile Best Gril Sex Avail...
Ooty Call Gril 80022//12248 Only For Sex And High Profile Best Gril Sex Avail...Ooty Call Gril 80022//12248 Only For Sex And High Profile Best Gril Sex Avail...
Ooty Call Gril 80022//12248 Only For Sex And High Profile Best Gril Sex Avail...
 
CROSS CULTURAL NEGOTIATION BY PANMISEM NS
CROSS CULTURAL NEGOTIATION BY PANMISEM NSCROSS CULTURAL NEGOTIATION BY PANMISEM NS
CROSS CULTURAL NEGOTIATION BY PANMISEM NS
 
Pre Engineered Building Manufacturers Hyderabad.pptx
Pre Engineered  Building Manufacturers Hyderabad.pptxPre Engineered  Building Manufacturers Hyderabad.pptx
Pre Engineered Building Manufacturers Hyderabad.pptx
 
Call 7737669865 Vadodara Call Girls Service at your Door Step Available All Time
Call 7737669865 Vadodara Call Girls Service at your Door Step Available All TimeCall 7737669865 Vadodara Call Girls Service at your Door Step Available All Time
Call 7737669865 Vadodara Call Girls Service at your Door Step Available All Time
 
Dr. Admir Softic_ presentation_Green Club_ENG.pdf
Dr. Admir Softic_ presentation_Green Club_ENG.pdfDr. Admir Softic_ presentation_Green Club_ENG.pdf
Dr. Admir Softic_ presentation_Green Club_ENG.pdf
 
Paradip CALL GIRL❤7091819311❤CALL GIRLS IN ESCORT SERVICE WE ARE PROVIDING
Paradip CALL GIRL❤7091819311❤CALL GIRLS IN ESCORT SERVICE WE ARE PROVIDINGParadip CALL GIRL❤7091819311❤CALL GIRLS IN ESCORT SERVICE WE ARE PROVIDING
Paradip CALL GIRL❤7091819311❤CALL GIRLS IN ESCORT SERVICE WE ARE PROVIDING
 
Arti Languages Pre Seed Teaser Deck 2024.pdf
Arti Languages Pre Seed Teaser Deck 2024.pdfArti Languages Pre Seed Teaser Deck 2024.pdf
Arti Languages Pre Seed Teaser Deck 2024.pdf
 
Lundin Gold - Q1 2024 Conference Call Presentation (Revised)
Lundin Gold - Q1 2024 Conference Call Presentation (Revised)Lundin Gold - Q1 2024 Conference Call Presentation (Revised)
Lundin Gold - Q1 2024 Conference Call Presentation (Revised)
 
joint cost.pptx COST ACCOUNTING Sixteenth Edition ...
joint cost.pptx  COST ACCOUNTING  Sixteenth Edition                          ...joint cost.pptx  COST ACCOUNTING  Sixteenth Edition                          ...
joint cost.pptx COST ACCOUNTING Sixteenth Edition ...
 
Durg CALL GIRL ❤ 82729*64427❤ CALL GIRLS IN durg ESCORTS
Durg CALL GIRL ❤ 82729*64427❤ CALL GIRLS IN durg ESCORTSDurg CALL GIRL ❤ 82729*64427❤ CALL GIRLS IN durg ESCORTS
Durg CALL GIRL ❤ 82729*64427❤ CALL GIRLS IN durg ESCORTS
 
WheelTug Short Pitch Deck 2024 | Byond Insights
WheelTug Short Pitch Deck 2024 | Byond InsightsWheelTug Short Pitch Deck 2024 | Byond Insights
WheelTug Short Pitch Deck 2024 | Byond Insights
 
Berhampur 70918*19311 CALL GIRLS IN ESCORT SERVICE WE ARE PROVIDING
Berhampur 70918*19311 CALL GIRLS IN ESCORT SERVICE WE ARE PROVIDINGBerhampur 70918*19311 CALL GIRLS IN ESCORT SERVICE WE ARE PROVIDING
Berhampur 70918*19311 CALL GIRLS IN ESCORT SERVICE WE ARE PROVIDING
 
Chennai Call Gril 80022//12248 Only For Sex And High Profile Best Gril Sex Av...
Chennai Call Gril 80022//12248 Only For Sex And High Profile Best Gril Sex Av...Chennai Call Gril 80022//12248 Only For Sex And High Profile Best Gril Sex Av...
Chennai Call Gril 80022//12248 Only For Sex And High Profile Best Gril Sex Av...
 
Al Mizhar Dubai Escorts +971561403006 Escorts Service In Al Mizhar
Al Mizhar Dubai Escorts +971561403006 Escorts Service In Al MizharAl Mizhar Dubai Escorts +971561403006 Escorts Service In Al Mizhar
Al Mizhar Dubai Escorts +971561403006 Escorts Service In Al Mizhar
 
QSM Chap 10 Service Culture in Tourism and Hospitality Industry.pptx
QSM Chap 10 Service Culture in Tourism and Hospitality Industry.pptxQSM Chap 10 Service Culture in Tourism and Hospitality Industry.pptx
QSM Chap 10 Service Culture in Tourism and Hospitality Industry.pptx
 

Lesson24 Implicit Differentiation Slides

  • 1. Lesson 24 (Sections 16.3, 16.7) Implicit Differentiation Math 20 November 16, 2007 Announcements Problem Set 9 on the website. Due November 21. There will be class November 21 and homework due November 28. next OH: Monday 1-2pm, Tuesday 3-4pm Midterm II: Thursday, 12/6, 7-8:30pm in Hall A. Go Harvard! Beat Yale!
  • 2. Outline Cleanup on Leibniz Rule Implicit Differentiation in two dimensions The Math 1a way Old school Implicit Differentation New school Implicit Differentation Compare Application More than two dimensions The second derivative
  • 3. Last Time: the Chain Rule Theorem (The Chain Rule, General Version) Suppose that u is a differentiable function of the n variables x1 , x2 , . . . , xn , and each xi is a differentiable function of the m variables t1 , t2 , . . . , tm . Then u is a function of t1 , t2 , . . . , tm and ∂u ∂u ∂x1 ∂u ∂x2 ∂u ∂xn = + + ··· + ∂ti ∂x1 ∂ti ∂x2 ∂ti ∂xn ∂ti
  • 4. Last Time: the Chain Rule Theorem (The Chain Rule, General Version) Suppose that u is a differentiable function of the n variables x1 , x2 , . . . , xn , and each xi is a differentiable function of the m variables t1 , t2 , . . . , tm . Then u is a function of t1 , t2 , . . . , tm and ∂u ∂u ∂x1 ∂u ∂x2 ∂u ∂xn = + + ··· + ∂ti ∂x1 ∂ti ∂x2 ∂ti ∂xn ∂ti In summation notation n ∂u ∂u ∂xj = ∂ti ∂xj ∂ti j=1
  • 5. Leibniz’s Formula for Integrals Fact Suppose that f (, t, x), a(t), and b(t) are differentiable functions, and let b(t) F (t) = f (t, x) dx a(t)
  • 6. Leibniz’s Formula for Integrals Fact Suppose that f (, t, x), a(t), and b(t) are differentiable functions, and let b(t) F (t) = f (t, x) dx a(t) Then b(t) ∂f (t, x) F (t) = f (t, b(t))b (t) − f (t, a(t))a (t) + dx a(t) ∂t
  • 7. Leibniz’s Formula for Integrals Fact Suppose that f (, t, x), a(t), and b(t) are differentiable functions, and let b(t) F (t) = f (t, x) dx a(t) Then b(t) ∂f (t, x) F (t) = f (t, b(t))b (t) − f (t, a(t))a (t) + dx a(t) ∂t Proof. Apply the chain rule to the function v H(t, u, v ) = f (t, x) dx u with u = a(t) and v = b(t).
  • 8. Tree Diagram H t u v t t
  • 9. More about the proof v H(t, u, v ) = f (t, x) dx u
  • 10. More about the proof v H(t, u, v ) = f (t, x) dx u Then by the Fundamental Theorem of Calculus (see Section 10.1) ∂H ∂H = f (t, v ) = −f (t, u) ∂v ∂u
  • 11. More about the proof v H(t, u, v ) = f (t, x) dx u Then by the Fundamental Theorem of Calculus (see Section 10.1) ∂H ∂H = f (t, v ) = −f (t, u) ∂v ∂u Also, v ∂H ∂f = (t, x) dx ∂t u ∂x since t and x are independent variables.
  • 12. Since F (t) = H(t, a(t), b(t)), dF ∂H ∂H du ∂H dv = + + dt ∂t ∂u dt ∂v dt b(t) ∂f = (t, x) + f (t, b(t))b (t) − f (t, a(t))a (t) a(t) ∂x
  • 13. Application Example (Example 16.8 with better notation) Let the profit of a firm be π(t). The present value of the future profit π(τ ) where τ > t is π(τ )e −r (τ −t) , where r is the discount rate. On a time interval [0, T ], the present value of all future profit is T V (t) = π(τ )e −r (τ −t) dt. t Find V (t).
  • 14. Application Example (Example 16.8 with better notation) Let the profit of a firm be π(t). The present value of the future profit π(τ ) where τ > t is π(τ )e −r (τ −t) , where r is the discount rate. On a time interval [0, T ], the present value of all future profit is T V (t) = π(τ )e −r (τ −t) dt. t Find V (t). Answer. V (t) = rV (t) − π(t)
  • 15. Solution Since the upper limit is a constant, the only boundary term comes from the lower limit: T ∂ V (t) = −π(t)e −r (t−t) + π(τ )e −r τ e rt dτ t ∂t T = −π(t) + r π(τ )e −r τ e rt dτ t = rV (t) − π(t). This means that π(t) + V (t) r= V (t) So if the fraction on the right is less than the rate of return for another, “safer” investment like bonds, it would be worth more to sell the business and buy the bonds.
  • 16. Outline Cleanup on Leibniz Rule Implicit Differentiation in two dimensions The Math 1a way Old school Implicit Differentation New school Implicit Differentation Compare Application More than two dimensions The second derivative
  • 17. An example 4 Consider the utility function 1 1 3 u(x, y ) = − − x y What is the 2 slope of the tangent line along the indifference 1 curve u(x, y ) = −1? 1 2 3 4
  • 18. The Math 1a way Solve for y in terms of x and differentiate: 1 1 1 + = 1 =⇒ y = x y 1 − 1/x So dy −1 1 = 1/x )2 dx (1 − x2 −1 −1 = 2 1/x )2 = x (1 − (x − 1)2
  • 19. Old school Implicit Differentation Differentiate the equation remembering that y is presumed to be a function of x: 1 1 dy − 2− 2 =0 x y dx So dy y2 y 2 =− 2 =− dx x x
  • 20. New school Implicit Differentation This is a formalized version of old school: If F (x, y ) = c Then by differentiating the equation and treating y as a function of x, we get ∂F ∂F dy + =0 ∂x ∂y dx F So dy ∂F /∂x =− dx F ∂F /∂x The (·)F notation reminds us that y is not explicitly a function of x, but if F is held constant we can treat it implicitly so.
  • 21. Tree diagram F x y x ∂F ∂F dy + =0 ∂x ∂y dx F
  • 22. The big idea Fact Along the level curve F (x, y ) = c, the slope of the tangent line is given by dy dy ∂F /∂x F (x, y ) = =− =− 1 dx dx F ∂F /∂x F2 (x, y )
  • 23. Compare Explicitly solving for y is tedious, and sometimes impossible. Either implicit method brings out more clearly the important fact that (in our example) dy dx depends only on the ratio u y/x . Old-school implicit differentiation is familiar but (IMO) contrived. New-school implicit differentiation is systematic and generalizable.
  • 24. Outline Cleanup on Leibniz Rule Implicit Differentiation in two dimensions The Math 1a way Old school Implicit Differentation New school Implicit Differentation Compare Application More than two dimensions The second derivative
  • 25. Application If u(x, y ) is a utility function of two goods, then u(x, y ) = c is a indifference curve, and the slope represents the marginal rate of substitution: dy ux MUx Ryx = − = = dx u uy MUy
  • 26. Outline Cleanup on Leibniz Rule Implicit Differentiation in two dimensions The Math 1a way Old school Implicit Differentation New school Implicit Differentation Compare Application More than two dimensions The second derivative
  • 27. More than two dimensions The basic idea is to close your eyes and use the chain rule: Example Suppose a surface is given by F (x, y , z) = c. If this defines z as a function of x and y , find zx and zy .
  • 28. More than two dimensions The basic idea is to close your eyes and use the chain rule: Example Suppose a surface is given by F (x, y , z) = c. If this defines z as a function of x and y , find zx and zy . Solution Setting F (x, y , z) = c and remembering z is implicitly a function of x and y , we get ∂F ∂F ∂z ∂z Fx + = 0 =⇒ =− ∂x ∂z ∂x F ∂x F Fz ∂F ∂F ∂z ∂z Fy + = 0 =⇒ =− ∂y ∂z ∂y F ∂y F Fz
  • 29. Tree diagram F x y z x ∂F ∂F ∂z ∂z Fx + = 0 =⇒ =− ∂x ∂z ∂x F ∂x F Fz
  • 30. Example Suppose production is given by a Cobb-Douglas function P(A, K , L) = AK a Lb where K is capital, L is labor, and A is technology. Compute the changes in technology or capital needed to sustain production if labor decreases.
  • 31. Example Suppose production is given by a Cobb-Douglas function P(A, K , L) = AK a Lb where K is capital, L is labor, and A is technology. Compute the changes in technology or capital needed to sustain production if labor decreases. Solution ∂K PL AK a bLb−1 b K =− =− a−1 Lb =− · ∂L P PK AaK a L ∂A PL AK a bLb−1 bA =− =− a Lb =− ∂L P PA K L b K So if labor decreases by 1 unit we need either a · L more capital or bA L more tech to sustain production.
  • 32. Outline Cleanup on Leibniz Rule Implicit Differentiation in two dimensions The Math 1a way Old school Implicit Differentation New school Implicit Differentation Compare Application More than two dimensions The second derivative
  • 33. The second derivative: Derivation What is the concavity of an indifference curve? We know dy Fx G =− =− dx F Fy H Then HG − GH y =− H2 Now d ∂F ∂2F ∂ 2 F dy G = = + dx ∂x ∂x 2 ∂y ∂x dx ∂ 2F ∂ 2F ∂F /∂x = − ∂x 2 ∂y ∂x ∂F /∂y So ∂F ∂ 2 F ∂ 2 F ∂F HG = − = Fy Fxx − Fyx Fx ∂y ∂x 2 ∂y ∂x ∂x
  • 34. Also d ∂F ∂F ∂ 2 F dy H = = + dx ∂y ∂x ∂y ∂y 2 dx ∂2F ∂ 2 F ∂F /∂x = − ∂x ∂y ∂y 2 ∂F /∂y So Fyy (Fx )2 GH = Fx Fxy − Fy Fx Fxy Fy − Fyy (Fx )2 = Fy
  • 35. Putting this all together we get Fx Fxy Fy − Fyy (Fx )2 Fy Fxx − Fyx Fx − Fy y =− (Fy )2 1 =− F (F )2 − 2Fxy Fx Fy + Fyy (Fx )2 (Fy )3 xx y 0 Fx Fy 1 = Fx Fxx Fxy (Fy )3 Fy Fxy Fyy
  • 36. Example Along the indifference curve 1 1 + =c x y d compute (y )u . What does this say about dx Ryx ?
  • 37. Example Along the indifference curve 1 1 + =c x y d compute (y )u . What does this say about dx Ryx ? Solution 1 1 We have u(x, y ) = x + y , so 0 −1/x 2 −1/y 2 d 2y 1 = −1/x 2 2/x 3 0 dx 2 u (−1/y 2 )3 −1/y 2 0 −2/y 3
  • 38. Solution (continued) 0 −1/x 2 −1/y 2 d 2y 1 = −1/x 2 2/x 3 0 dx 2 u (−1/y 2 )3 −1/y 2 0 −2/y 3 −1 −1 2 −1 2 −1 = −y 6 − − x2 x2 y3 y2 x3 y2 1 1 = 2y 6 + x 4y 3 y 4x 3 y 3 1 1 y 3 =2 + = 2c x x y x dy This is positive, and since Ryx = − dx , we have u d y 3 Ryx = −2u <0 dx x So the MRS diminishes with increasing consumption of x.
  • 39. Bonus: Elasticity of substitution See Section 16.4 The elasticity of substitution is the elasticity of the MRS with respect to the ratio y/x : ∂Ryx y/x σyx = εRyx ,(y/x ) = · ∂(y/x ) Ryx In our case, Ryx = (y/x )2 , so y/x σyx = 2 (y/x ) =2 (y/x )2 1 1 which is why the function u(x, y ) = x + y is called a constant elasticity of substitution function.