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Calculus - DIW fileDifferentiation I Definition Let f : R !R. Its derivative with respect to a...

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Calculus Anton Velinov DIW WS 2016
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Page 1: Calculus - DIW fileDifferentiation I Definition Let f : R !R. Its derivative with respect to a point x is defined by the following limit f0(x) = df dx = lim!0 f(x + ) f(x)

Calculus

Anton Velinov

DIW WS 2016

Page 2: Calculus - DIW fileDifferentiation I Definition Let f : R !R. Its derivative with respect to a point x is defined by the following limit f0(x) = df dx = lim!0 f(x + ) f(x)

Takeaways

Differentiation: rules, implicit differentiationTaylor and power seriesMaximizationDefinite and indefinite integralsDifferential equationsMultivariate function limits and continuityPartial derivatives, gradient and directional derivativesComplex numbersImplicit function theorem

Anton Velinov Calculus 2 / 57

Page 3: Calculus - DIW fileDifferentiation I Definition Let f : R !R. Its derivative with respect to a point x is defined by the following limit f0(x) = df dx = lim!0 f(x + ) f(x)

Differentiation I

DefinitionLet f : R→ R. Its derivative with respect to a point x is definedby the following limit

f ′(x) =dfdx

= lim∆→0

f (x + ∆)− f (x)

∆.

Class ExerciseUse the above definition to calculate the derivative of

f (x) = a + bx

andf (x) =

xx + 1

with respect to x .

Anton Velinov Calculus 3 / 57

Page 4: Calculus - DIW fileDifferentiation I Definition Let f : R !R. Its derivative with respect to a point x is defined by the following limit f0(x) = df dx = lim!0 f(x + ) f(x)

Differentiation II

Useful Rulesdxk/dx = kxk−1

d(sin(x))/dx = cos(x) and d(cos(x))/dx = −sin(x)

d(ex )/dx = ex

d(log(x))/dx = 1/x

Anton Velinov Calculus 4 / 57

Page 5: Calculus - DIW fileDifferentiation I Definition Let f : R !R. Its derivative with respect to a point x is defined by the following limit f0(x) = df dx = lim!0 f(x + ) f(x)

Differentiation III

TheoremIf a function f (x) is differentiable at some point x , then it iscontinuous at x .

differentiability⇒ continuity.

The converse is not true

continuity ; differentiability.

Class ExerciseShow that f (x) = |x − 2|+ 1 is continuous but not differentiableat x = 2.

Anton Velinov Calculus 5 / 57

Page 6: Calculus - DIW fileDifferentiation I Definition Let f : R !R. Its derivative with respect to a point x is defined by the following limit f0(x) = df dx = lim!0 f(x + ) f(x)

Differentiation Rules I

Product RuleIf functions f (x) and g(x) are differentiable then their product isdifferentiable and given as follows:

(f (x)g(x))′ =d(f (x)g(x))

dx= f ′(x)g(x) + f (x)g′(x).

Quotient RuleIf functions f (x) and g(x) are differentiable then their quotient isdifferentiable and given as follows:(

f (x)

g(x)

)′=

d(f (x)/g(x))

dx=

f ′(x)g(x)− f (x)g′(x)

(g(x))2 .

Anton Velinov Calculus 6 / 57

Page 7: Calculus - DIW fileDifferentiation I Definition Let f : R !R. Its derivative with respect to a point x is defined by the following limit f0(x) = df dx = lim!0 f(x + ) f(x)

Differentiation Rules II

ExampleProve the product rule. Hint: Add and subtract f (x + ∆)g(x).

Chain RuleFor the composite function g(x) = f (u(x)) or g(x) = (f ◦ u)(x)the derivative is given as follows:

dg(x)

dx=

df (·)du

du(x)

dx.

Class ExerciseUse the chain rule to find the derivative of

f (x) = 2x

with respect to x .

Anton Velinov Calculus 7 / 57

Page 8: Calculus - DIW fileDifferentiation I Definition Let f : R !R. Its derivative with respect to a point x is defined by the following limit f0(x) = df dx = lim!0 f(x + ) f(x)

Implicit Differentiation I

It is not always possible to differentiate x explicitly from f (x). Asa direct consequence of the chain rule we can therefore makeuse of implicit differentiation

ExampleFind the derivative of

x2 + y2 = 1

with respect to x and compare this to the explicit solution.

Class ExerciseFind the derivative of

(x2 + y2)3 = 5x2y2

with respect to x .

Anton Velinov Calculus 8 / 57

Page 9: Calculus - DIW fileDifferentiation I Definition Let f : R !R. Its derivative with respect to a point x is defined by the following limit f0(x) = df dx = lim!0 f(x + ) f(x)

Implicit Differentiation II

Class Exercise (optional)Find the derivative of

y = xx

with respect to x .

Anton Velinov Calculus 9 / 57

Page 10: Calculus - DIW fileDifferentiation I Definition Let f : R !R. Its derivative with respect to a point x is defined by the following limit f0(x) = df dx = lim!0 f(x + ) f(x)

Higher Order Derivatives

DefinitionThe second derivative of f (x) is given by

f ′′(x) =d2f (x)

dx2 =ddx

[df (x)

dx

].

DefinitionIn general the k th-order derivative is the derivative of the(k − 1)th-order derivative.

Anton Velinov Calculus 10 / 57

Page 11: Calculus - DIW fileDifferentiation I Definition Let f : R !R. Its derivative with respect to a point x is defined by the following limit f0(x) = df dx = lim!0 f(x + ) f(x)

Taylor Series Approximation

DefinitionAn r-th-order Taylor series approximation of a function f (x) atx = c + ∆ is as follows:

f (x) = f (c) +dfdx

∣∣∣∣∣x=c

·∆ +12!

d2fdx2

∣∣∣∣∣x=c

·∆2 +

+13!

d3fdx3

∣∣∣∣∣x=c

·∆3 + · · ·+ 1r !

d r fdx r

∣∣∣∣∣x=c

·∆r + R(c, x)

provided that all r derivatives of f (x) exist and are continuous ina neighbourhood of c.

Anton Velinov Calculus 11 / 57

Page 12: Calculus - DIW fileDifferentiation I Definition Let f : R !R. Its derivative with respect to a point x is defined by the following limit f0(x) = df dx = lim!0 f(x + ) f(x)

First Order Taylor Series Approximation

Figure: First Order Approximation

C

Anton Velinov Calculus 12 / 57

Page 13: Calculus - DIW fileDifferentiation I Definition Let f : R !R. Its derivative with respect to a point x is defined by the following limit f0(x) = df dx = lim!0 f(x + ) f(x)

Power Series I

DefinitionA Power series assumes that the remainder term, R(c, x) of theTaylor series goes to 0 as r →∞. It also centres the expansionat c = 0.

Class ExerciseFind the Power series of

f (x) = ex

evaluated at x = 1.

Anton Velinov Calculus 13 / 57

Page 14: Calculus - DIW fileDifferentiation I Definition Let f : R !R. Its derivative with respect to a point x is defined by the following limit f0(x) = df dx = lim!0 f(x + ) f(x)

Power Series II

Class Exercise (Optional)Use the previous result to evaluate

limn→∞

(1 +

1n

)n

.

Anton Velinov Calculus 14 / 57

Page 15: Calculus - DIW fileDifferentiation I Definition Let f : R !R. Its derivative with respect to a point x is defined by the following limit f0(x) = df dx = lim!0 f(x + ) f(x)

Maxima and Minima

DefinitionThe function f : X → R has a global maximum at x = c iff (x) ≤ f (c) for all x ∈ XThe function f : X → R has a local maximum at x = c iff (x) ≤ f (c) for all x in some open interval around x = c.Analogous definitions hold for global and local minima.

Class ExerciseWhat does the Extreme Value Theorem have to do with theabove definition?

Anton Velinov Calculus 15 / 57

Page 16: Calculus - DIW fileDifferentiation I Definition Let f : R !R. Its derivative with respect to a point x is defined by the following limit f0(x) = df dx = lim!0 f(x + ) f(x)

Maximization I

Fermat’s TheoremIf a function f (x) has an extreme point at x = c and f ′(c) exists,then f ′(c) = 0.

This is a necessary condition for an interior maximum.

Class ExerciseFind an example where f ′(x) = 0 does not lead to a maximumor a minimum.

Anton Velinov Calculus 16 / 57

Page 17: Calculus - DIW fileDifferentiation I Definition Let f : R !R. Its derivative with respect to a point x is defined by the following limit f0(x) = df dx = lim!0 f(x + ) f(x)

Maximization II

Second Derivative TestIf the second derivative of f (x) exists and if x = c is a criticalpoint of f (x) then:

If f ′′(x) < 0, f (x) has a local maximum at xIf f ′′(x) > 0, f (x) has a local minimum at xIf f ′′(x) = 0, the test is inconclusive.

Class ExerciseUse the second derivative test for the previous exercise.

Anton Velinov Calculus 17 / 57

Page 18: Calculus - DIW fileDifferentiation I Definition Let f : R !R. Its derivative with respect to a point x is defined by the following limit f0(x) = df dx = lim!0 f(x + ) f(x)

Indefinite Integral

DefinitionInformally speaking, in case of a continuous function,integration, denoted by

∫·dx , is the inverse of differentiation:∫f ′(x)dx = f (x).

However, we assume that we only know f ′(x) and hence, whenintegrating a function we always add a constant, C to it. This iscalled an indefinite integral. It is over ±∞.

NoteIntegration is not quite the opposite of differentiation asfunctions that are non-differentiable can still be integrated.

Anton Velinov Calculus 18 / 57

Page 19: Calculus - DIW fileDifferentiation I Definition Let f : R !R. Its derivative with respect to a point x is defined by the following limit f0(x) = df dx = lim!0 f(x + ) f(x)

Indefinite Integral Rules

Integration Rules∫xkdx = xk+1

k+1 + C for k 6= −1∫x−1dx =log(|x |) + C∫cos(x)dx = sin(x) + C∫sin(x)dx = −cos(x) + C∫eaxdx = (1/a)eax + C∫af (x)dx = a

∫f (x)dx for some constant a not depending

on x∫[af (x) + bg(x)]dx = a

∫f (x)dx + b

∫g(x)dx for some

constants a,b not depending on x .

Anton Velinov Calculus 19 / 57

Page 20: Calculus - DIW fileDifferentiation I Definition Let f : R !R. Its derivative with respect to a point x is defined by the following limit f0(x) = df dx = lim!0 f(x + ) f(x)

Definite Integral

DefinitionFrom the fundamental theorem of calculus a definite integral isdefined as:∫ b

af (x)dx =

[∫f (x)dx

]∣∣∣∣∣x=b

[∫f (x)dx

]∣∣∣∣∣x=a

= F (b)− F (a).

Intuitively, it is the area under a function over the domain [a,b].

Class ExerciseFind the integral of ∫ b

ax

1b − a

dx .

Anton Velinov Calculus 20 / 57

Page 21: Calculus - DIW fileDifferentiation I Definition Let f : R !R. Its derivative with respect to a point x is defined by the following limit f0(x) = df dx = lim!0 f(x + ) f(x)

Integration by Substitution

DefinitionFor the function that can be composed as f (g(x))g′(x), itsintegral over the domain a,b is given as∫ b

af (g(x))g′(x)dx =

∫ g(b)

g(a)f (u)du.

This is known as integration by substitution. This definitionapplies to indefinite integration analogously.

Class Exercise1 What is

∫x/(x2 + 1)dx?

2 What is∫

(x + 1)3dx?

Anton Velinov Calculus 21 / 57

Page 22: Calculus - DIW fileDifferentiation I Definition Let f : R !R. Its derivative with respect to a point x is defined by the following limit f0(x) = df dx = lim!0 f(x + ) f(x)

Integration by Parts

DefinitionThrough the product rule we can derive the following formulafor integration by parts∫

f (x)g′(x)dx = f (x)g(x)−∫

f ′(x)g(x)dx .

Class ExerciseFind the integral of ln x .

Anton Velinov Calculus 22 / 57

Page 23: Calculus - DIW fileDifferentiation I Definition Let f : R !R. Its derivative with respect to a point x is defined by the following limit f0(x) = df dx = lim!0 f(x + ) f(x)

Differential Equations I

DefinitionA differential equation is an equation that involves an unknownfunction as its solution. It usually involves a general and aparticular solution given some initial conditions.

Intuitively, we are given the nth order derivatives of a function inan equation and we need to solve this in order to find theoriginal function.In economics differential equations are mainly used ingrowth theory

ExampleFind the solution to

dydx

=√

x/y

given the initial condition y = 4, x = 1.

Anton Velinov Calculus 23 / 57

Page 24: Calculus - DIW fileDifferentiation I Definition Let f : R !R. Its derivative with respect to a point x is defined by the following limit f0(x) = df dx = lim!0 f(x + ) f(x)

Differential Equations II

Class ExerciseFind the solution to

dydx

= x/y

given the initial condition y = 1, x = 1.

DefinitionThe previous two exercises deal with separable differentialequations, i.e. when the xs and ys can be separated on bothsides of the equation.

Anton Velinov Calculus 24 / 57

Page 25: Calculus - DIW fileDifferentiation I Definition Let f : R !R. Its derivative with respect to a point x is defined by the following limit f0(x) = df dx = lim!0 f(x + ) f(x)

Homogeneous Differential Equations (Optional)

DefinitionAn equation of the form

dydx

= f (x , y)

is referred to as a homogeneous differential equation. If the xsand ys are not separable, v = y/x is used to solve theequation.

Class ExerciseFind the solution to

1dydx = x+y

x

2dydx = x2+3y2

2xy (optional).

Anton Velinov Calculus 25 / 57

Page 26: Calculus - DIW fileDifferentiation I Definition Let f : R !R. Its derivative with respect to a point x is defined by the following limit f0(x) = df dx = lim!0 f(x + ) f(x)

Multivariate Function Limits I

DefinitionA multivariate or multivariable function, f has n > 1 argumentsmapping onto R, i.e. f : Rn → R. Written as f (x1, x2, . . . , xn) orf (x).

Multivariate function limitIn Euclidean space f has a limit L as x approaches x0 if

∀ ε > 0 ∃ δ(ε) > 0; |f (x)−L| < εwhenever 0 < ‖x−x0‖2 < δ(ε).

We write f (x)→ L as x→ x0 or limx→x0 f (x) = L.

NoteUnlike the univariate case, there are an infinite number ofdirections for x to approach x0.

Anton Velinov Calculus 26 / 57

Page 27: Calculus - DIW fileDifferentiation I Definition Let f : R !R. Its derivative with respect to a point x is defined by the following limit f0(x) = df dx = lim!0 f(x + ) f(x)

Multivariate Function Limits II

Class ExerciseDetermine whether the following limits exist

1 lim(x ,y)→(0,0)x2

x2+y2

2 lim(x ,y)→(0,0)xy

x2+y2 .

Anton Velinov Calculus 27 / 57

Page 28: Calculus - DIW fileDifferentiation I Definition Let f : R !R. Its derivative with respect to a point x is defined by the following limit f0(x) = df dx = lim!0 f(x + ) f(x)

Multivariate Function Limits III

Class ExerciseShow that the following limit exists

lim(x ,y)→(0,0)

x2yx2 + y2 .

Anton Velinov Calculus 28 / 57

Page 29: Calculus - DIW fileDifferentiation I Definition Let f : R !R. Its derivative with respect to a point x is defined by the following limit f0(x) = df dx = lim!0 f(x + ) f(x)

Continuity of Multivariate Functions

Epsilon-Delta Definition

A function f : Rn → R is said to be continuous at x0 ∈ Rn if

∀ ε > 0 ∃ δ(ε,x0) > 0 ; |f (x)− f (x0)| < ε

whenever 0 < ‖x− x0‖2 < δ(ε,x0)

Limit DefinitionA function f : Rn → R is said to be continuous at x0 ∈ Rn if

limx→x0

f (x) = f (x0).

TheoremPolynomial functions are continuous everywhere. Rationalfunctions are continuous everywhere they are defined.

Anton Velinov Calculus 29 / 57

Page 30: Calculus - DIW fileDifferentiation I Definition Let f : R !R. Its derivative with respect to a point x is defined by the following limit f0(x) = df dx = lim!0 f(x + ) f(x)

Partial Derivatives I

DefinitionFor the function f : Rn → R, its partial derivative w.r.t. xi isdefined as

fxi =∂f∂xi

= lim∆→0

[f (x1, x2, . . . , xi−1, xi + ∆, xi+1, . . . , xn)

− f (x1, x2, . . . , xi−1, xi , xi+1, . . . , xn)]/∆.

Class ExerciseFind the partial derivatives with respect to x and y for thefollowing function

f (x , y) = x4 + 6√

y + 10.

Anton Velinov Calculus 30 / 57

Page 31: Calculus - DIW fileDifferentiation I Definition Let f : R !R. Its derivative with respect to a point x is defined by the following limit f0(x) = df dx = lim!0 f(x + ) f(x)

Partial Derivatives II

Anton Velinov Calculus 31 / 57

Page 32: Calculus - DIW fileDifferentiation I Definition Let f : R !R. Its derivative with respect to a point x is defined by the following limit f0(x) = df dx = lim!0 f(x + ) f(x)

Gradient I

DefinitionThe column vector of partial derivatives of the n dimensionalvector valued function f (x) is known as the gradient (denoted∇) of f :

∂f (x)/∂x = ∇ =

∂f (x)/∂x1∂f (x)/∂x2

...∂f (x)/∂xn

=∂f (x)

∂x1e1+

∂f (x)

∂x2e2+· · ·+∂f (x)

∂xnen,

where the eis are orthogonal unit vectors.

Geometric InterpretationThe gradient is always orthogonal to the level set f (x) = k . Itgives the direction of the steepest ascent (in Rn).

Anton Velinov Calculus 32 / 57

Page 33: Calculus - DIW fileDifferentiation I Definition Let f : R !R. Its derivative with respect to a point x is defined by the following limit f0(x) = df dx = lim!0 f(x + ) f(x)

Gradient II

Anton Velinov Calculus 33 / 57

Page 34: Calculus - DIW fileDifferentiation I Definition Let f : R !R. Its derivative with respect to a point x is defined by the following limit f0(x) = df dx = lim!0 f(x + ) f(x)

Directional Derivatives I

DefinitionPartial derivatives examine the rate of change when allowingone variable to change while the rest are kept constant.Directional derivatives examine the rate of change whenallowing all of a function’s variables to vary. For the functionf : Rn → R the directional derivative with the direction of therate of change denoted by the n dimensional vectoru = [u1 u2 . . . un]′ is given by

Duf (x1, x2, . . . , xn) = lim∆→0

[f (x1 + u1∆, x2 + u2∆, . . . , xn + un∆)

− f (x1, x2, . . . , xn)]/∆

Anton Velinov Calculus 34 / 57

Page 35: Calculus - DIW fileDifferentiation I Definition Let f : R !R. Its derivative with respect to a point x is defined by the following limit f0(x) = df dx = lim!0 f(x + ) f(x)

Directional Derivatives II

The limit in the above definition is sometimes difficult tocalculate so an equivalent formula based on the partialderivative is often used

Duf (x1, x2, . . . , xn) = (∂f/∂x1)u1 + (∂f/∂x2)u2 + · · ·+ (∂f/∂xn)un

=n∑

i=1

(∂f/∂xi)ui =n∑

i=1

fxi ui .

Notice that this can be expressed in terms of the gradientvector as

Duf (x) = ∇ · uwhere · denotes the dot product.

ExampleShow that the above formula is equivalent to the one on theprevious slide. Hint: Define the univariate functiong(z) = f (x0

1 + u1z, x02 + u2z, . . . , x0

n + unz) and take itsderivative at z = 0.

Anton Velinov Calculus 35 / 57

Page 36: Calculus - DIW fileDifferentiation I Definition Let f : R !R. Its derivative with respect to a point x is defined by the following limit f0(x) = df dx = lim!0 f(x + ) f(x)

Directional Derivatives III

The u VectorNote that the vector u can describe a rate of change in anyinfinite amount of directions. It is normalized to a unit length as

‖uN‖2 =

√√√√ n∑i=1

u2iN = 1,

whereuN =

u‖u‖2

,

and ‖ · ‖2 is the L− 2 vector norm.

Anton Velinov Calculus 36 / 57

Page 37: Calculus - DIW fileDifferentiation I Definition Let f : R !R. Its derivative with respect to a point x is defined by the following limit f0(x) = df dx = lim!0 f(x + ) f(x)

The Gradient and the Directional Derivative

NoteUnlike a directional derivative, the gradient is not a scalar but avector.

Class ExerciseFor the function

f (x , y , z) = x2z + y3z2 − xyz

1 Calculate the gradient2 Determine the directional derivative in the direction of

u = [−1 0 3]′

3 Would the directional derivative go in the steepestdirection?

Anton Velinov Calculus 37 / 57

Page 38: Calculus - DIW fileDifferentiation I Definition Let f : R !R. Its derivative with respect to a point x is defined by the following limit f0(x) = df dx = lim!0 f(x + ) f(x)

Hessian I

DefinitionThe second derivative of the n dimensional vector valuedfunction f (x) is given by:

∂2f (x)

∂xi∂xj∀i , j = 1, . . . ,n.

These derivatives can be grouped in a matrix known as theHessian matrix, H:

H =∂f (x)

∂x∂x′=

∂2f/∂x1∂x1 ∂2f/∂x1∂x2 · · · ∂2f/∂x1∂xn∂2f/∂x2∂x1 ∂2f/∂x2∂x2 · · · ∂2f/∂x2∂xn

...... · · ·

...∂2f/∂xn∂x1 ∂2f/∂xn∂x2 · · · ∂2f/∂xn∂xn

.Since the order of differentiation does not matter, H is asymmetric matrix.

Anton Velinov Calculus 38 / 57

Page 39: Calculus - DIW fileDifferentiation I Definition Let f : R !R. Its derivative with respect to a point x is defined by the following limit f0(x) = df dx = lim!0 f(x + ) f(x)

Hessian II

Second Derivative TestIf x = c ∈ Rn is a critical point of f (x) and if the matrix H exists,then it can be used as a second derivative test in determininglocal optima as follows:

If H is positive definite, then f (·) attains a local minimum atcIf H is negative definite, then f (·) attains a local maximumat cIf the Eigenvalues of H alternate in sign, then f (·) has asaddle point at c.

Anton Velinov Calculus 39 / 57

Page 40: Calculus - DIW fileDifferentiation I Definition Let f : R !R. Its derivative with respect to a point x is defined by the following limit f0(x) = df dx = lim!0 f(x + ) f(x)

Jacobian and the Vector-Valued Function

DefinitionSuppose we have the following vector-valued functionf : Rn → Rm, that is we have fi(x1, x2, . . . , xn) = fi(x),x ∈ Rn fori = 1, . . . ,m. Collect all the m functions in an (m × 1) columnvector

f (x) = [f1(x) f2(x) · · · fm(x)]′,

then the derivative of f (x) w.r.t. x is called the Jacobian matrix:

J =∂f (x)

∂x′=

∂f1/∂x1 ∂f1/∂x2 · · · ∂f1/∂xn∂f2/∂x1 ∂f2/∂x2 · · · ∂f2/∂xn

...... · · ·

...∂fm/∂x1 ∂fm/∂x2 · · · ∂fm/∂xn

.

NoteBoth H and J are sometimes defined as their respectivedeterminants.Anton Velinov Calculus 40 / 57

Page 41: Calculus - DIW fileDifferentiation I Definition Let f : R !R. Its derivative with respect to a point x is defined by the following limit f0(x) = df dx = lim!0 f(x + ) f(x)

Matrix Differentiation Rules

Matrix Differentiation RulesFor the (n × 1) vector a we have ∂a′x/∂x = ∂x′a/∂x = aFor the (m × n) matrix A we have ∂Ax/∂x′ = AFor the (n × n) matrix C, the quadratic form x′Cx has thederivative ∂x′Cx/∂x = (C′ + C)x, which is 2Cx if C issymmetricFor the (n × n) matrix C, ∂C−1/∂x = −C−1(∂C/∂x)C−1

Class ExerciseShow that the first two points hold.

Anton Velinov Calculus 41 / 57

Page 42: Calculus - DIW fileDifferentiation I Definition Let f : R !R. Its derivative with respect to a point x is defined by the following limit f0(x) = df dx = lim!0 f(x + ) f(x)

Multiple Integrals

DefinitionMultiple integrals are of the form∫ ∫

· · ·∫

f (x1, x2, . . . , xn)dx1dx2 · · · dxn.

They can be solved by integrating x1 out, then x2 and so on.Note however that the order of integration does not matter.

Class ExerciseSolve ∫ 2

0

∫ 2

1e−(x+y)dxdy

by integrating out x and y and then y and x . Compare youranswers.

Anton Velinov Calculus 42 / 57

Page 43: Calculus - DIW fileDifferentiation I Definition Let f : R !R. Its derivative with respect to a point x is defined by the following limit f0(x) = df dx = lim!0 f(x + ) f(x)

Logarithms in Economics

DefinitionThe natural logarithm is the inverse of e

ln(ex ) = x .

For x > 0 it also follows that

x = eln(x).

In economics texts this is usually denoted as log instead of ln.

Class ExerciseFrom the above definition show that

ln(xa) = a ln(x).

Anton Velinov Calculus 43 / 57

Page 44: Calculus - DIW fileDifferentiation I Definition Let f : R !R. Its derivative with respect to a point x is defined by the following limit f0(x) = df dx = lim!0 f(x + ) f(x)

Logarithms as Percentages

Logarithms as PercentagesIn economics the logarithm is often used to describe apercentage. For some small ∆

ln(1 + ∆) ≈ ∆.

Class ExerciseShow that this holds by taking a first-order Taylor expansion ofthe function f (x) = ln(x) around c = 1 evaluated at x = 1.

Anton Velinov Calculus 44 / 57

Page 45: Calculus - DIW fileDifferentiation I Definition Let f : R !R. Its derivative with respect to a point x is defined by the following limit f0(x) = df dx = lim!0 f(x + ) f(x)

Complex Numbers C I

DefinitionA complex number, c is written in the form of

c = a + bi

where a and b are real numbers and i is an imaginary numbersuch that i =

√−1.

The Set CThe real number set is a subset of the complex numberset, R ⊂ CC is a field obeying the field axioms (since R is also a field)C however does not satisfy the order axioms, unlike R.

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Page 46: Calculus - DIW fileDifferentiation I Definition Let f : R !R. Its derivative with respect to a point x is defined by the following limit f0(x) = df dx = lim!0 f(x + ) f(x)

Complex Numbers C II

Figure: Complex Circle

Imaginary axis (i)

Real axis (a)

a+bi

bi

a

R

θ

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Page 47: Calculus - DIW fileDifferentiation I Definition Let f : R !R. Its derivative with respect to a point x is defined by the following limit f0(x) = df dx = lim!0 f(x + ) f(x)

Complex Numbers C III

DefinitionA complex conjugate, of a complex number a + bi is given by

a− bi .

Both numbers are known as a complex conjugate pair. Additionand multiplication of complex conjugate pairs produce realnumbers.

DefinitionThe modulus or absolute value of a complex number, is itsdistance from the origin as measured by the L− 2 norm

R ≡ ‖a + bi‖2 =√

a2 + b2.

Anton Velinov Calculus 47 / 57

Page 48: Calculus - DIW fileDifferentiation I Definition Let f : R !R. Its derivative with respect to a point x is defined by the following limit f0(x) = df dx = lim!0 f(x + ) f(x)

Complex Numbers C IV

Polar CoordinatesA complex number can also be written in Polar coordinate form.Note that

cos(θ) = a/R

andsin(θ) = b/R

hence,a + bi = R[cos(θ) + i · sin(θ)].

Anton Velinov Calculus 48 / 57

Page 49: Calculus - DIW fileDifferentiation I Definition Let f : R !R. Its derivative with respect to a point x is defined by the following limit f0(x) = df dx = lim!0 f(x + ) f(x)

Complex Numbers C V

Exponent FormUsing the Power series it is also possible to write a complexnumber as

a + bi = Reiθ.

ExampleVerify the above result by taking the Power series of f (x) =sin(x) and f (x) = cos(x). Hint: Also take the Power series ofex evaluated at x = iθ and plug in all the results in the Polarcoordinate form.

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Page 50: Calculus - DIW fileDifferentiation I Definition Let f : R !R. Its derivative with respect to a point x is defined by the following limit f0(x) = df dx = lim!0 f(x + ) f(x)

L’ Hôpital’s Rule

DefinitionLet f (·) and g(·) be functions, which are differentiable on theopen interval set X . Then for some point x0 ∈ X if

limx→x0 f (x) = 0 and limx→x0 g(x) = 0 and limx→x0f ′(x)g′(x)

exists or iflimx→x0 f (x) = ±∞ and limx→x0 g(x) = ±∞ andlimx→x0

f ′(x)g′(x) exists

then limx→x0f (x)g(x) = limx→x0

f ′(x)g′(x) .

Class ExerciseUse L’ Hôpital’s Rule to evaluate

limx→0

f (x)

g(x)= lim

x→0

2 sin(x)− sin(2x)

x − sin(x).

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Page 51: Calculus - DIW fileDifferentiation I Definition Let f : R !R. Its derivative with respect to a point x is defined by the following limit f0(x) = df dx = lim!0 f(x + ) f(x)

Homogenous Functions

DefinitionThe function f (x1, x2, . . . , xn) is homogenous of degree r ∈ R iffor any t > 0

f (tx1, tx2, . . . , txn) = t r f (x1, x2, . . . , xn).

Such functions are commonly used in economics. A functionthat is homogenous of degree 1 can be manipulated as

f (1, x2/x1, . . . , xn/x1) = (1/x1)f (x1, x2, . . . , xn).

Class Exercise1 Give an example of a homogenous function in economics.2 Show that f (x1, x2) =

√x1x2 is homogenous of degree 1.

Anton Velinov Calculus 51 / 57

Page 52: Calculus - DIW fileDifferentiation I Definition Let f : R !R. Its derivative with respect to a point x is defined by the following limit f0(x) = df dx = lim!0 f(x + ) f(x)

Implicit Function Theorem I

SettingSuppose we have a system of n functions fi : Rn+m → R, whichdepend on n ’parameters’ x = [x1 x2 · · · xn]′ and m’endogenous’ variables y = [y1 y2 · · · ym]′, i.e. fi(x,y),where x ∈ X ⊂ Rn and y ∈ Y ⊂ Rm. Further, suppose that

fi(x,y) = 0 i = 1, . . . ,n. (1)

Assume the vectors x0 ∈ X and y0 ∈ Y satisfy (1).

GoalWe want to solve for y as a function of x locally around x0 andy0.

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Page 53: Calculus - DIW fileDifferentiation I Definition Let f : R !R. Its derivative with respect to a point x is defined by the following limit f0(x) = df dx = lim!0 f(x + ) f(x)

Implicit Function Theorem II

DefinitionEquation (1) can be solved locally around (x0,y0) so that y is afunction of x if there are open neighbourhoods of x0 and y0

such that

fi(x, (g1(x),g2(x), . . . ,gn(x))) = 0, i = 1, . . . ,n, (2)

whereyi = gi(x), i = 1, . . . ,n,

provided that x is in its open neighbourhood. gi(x) are know asunique implicit functions.

DefinitionAn open neighbourhood of x ∈ Rn is defined as

{x0 ∈ Rn : ‖x0 − x‖2 < ε}.Anton Velinov Calculus 53 / 57

Page 54: Calculus - DIW fileDifferentiation I Definition Let f : R !R. Its derivative with respect to a point x is defined by the following limit f0(x) = df dx = lim!0 f(x + ) f(x)

Implicit Function Theorem III

Implicit Function TheoremSuppose all n functions are continuously partially differentiablew.r.t. their n + m variables. A solution of the type of (2),involving unique implicit functions for the endogenous variables,is possible provided that

|Jy|(x=x0,y=y0) 6= 0.

Further, the effect of a change of x on y at (x0,y0) can beexpressed as

∂g(x)

∂x′= −

[∂f (x,y)

∂y

]−1∂f (x,y)

∂x,

evaluated at (x0,y0).

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Page 55: Calculus - DIW fileDifferentiation I Definition Let f : R !R. Its derivative with respect to a point x is defined by the following limit f0(x) = df dx = lim!0 f(x + ) f(x)

Implicit Function Theorem IV

Intuitively, the IFT provides a sufficient condition for theexistence of unique solutions (equilibria) and gives us thefirst-order comparative static effects of such a solution.

Example

For the unit circle, x2 + y2 = 1⇔ f (x , y) = x2 + y2 − 1 = 0 canwe solve uniquely for x in terms of y at the point(x0, y0) = (1,0) s.t. f (x ,g(x)) = 0?

Class ExerciseCan we do this at a point (x0, y0) where y0 > 0 or wherey0 < 0?

Class ExerciseTo illustrate that the IFT only gives a sufficient condition for theexistence of unique solutions solve f (x , y) = y3 − x = 0 for y interms of x at the point (x0, y0) = (0,0).

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Inverse Function Theorem

Inverse Function TheoremWhen the number of parameters are the same as the numberof endogenous variables, m = n we have that

fi(x,y) = gi(x)− yi , i = 1, . . . ,n.

which is known as the Inverse Function Theorem.

This is a special case of the IFT.

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End of Theme 4

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