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Lecture 3.

Mathematics. Multivariable Calculus

Artur Siemaszko

Faculty of Mathematics and Computer Science University of Warmia and Mazury in Olsztyn

February 25, 2014

(2)

Lecture 3.

What is the difference in the behaviour of the following functions near the point (0, 0)?

f (x , y ) = ( x2y

x2+y2 : (x , y ) 6= (0, 0)

0 : (x , y ) = (0, 0); g(x , y ) = ( x2

x2+y2 : (x , y ) 6= (0, 0) 0 : (x , y ) = (0, 0).

(3)

Lecture 3.

Definitions

Definition

The functionf has a limitLat the point(a, b), written lim

(x ,y )→(a,b)f (x , y ) = L

iff (x , y )is as close toLas we please whenever the distance from the point(x , y )to the point(a, b)is sufficiently small, but not zero. Definition

A functionf is continuous at the point(a, b)if lim

(x ,y )→(a,b)f (x , y ) = f (a, b).

A function is continuous on a region D in the xy -plane if it is continuous at each point of D.

(4)

Lecture 3.

Definitions

Definition

The functionf has a limitLat the point(a, b), written

(x ,y )→(a,b)lim f (x , y ) = L

iff (x , y )is as close toLas we please whenever the distance from the point(x , y )to the point(a, b)is sufficiently small, but not zero.

Definition

A functionf is continuous at the point(a, b)if lim

(x ,y )→(a,b)f (x , y ) = f (a, b).

A function is continuous on a region D in the xy -plane if it is continuous at each point of D.

(5)

Lecture 3.

Definitions

Definition

The functionf has a limitLat the point(a, b), written

(x ,y )→(a,b)lim f (x , y ) = L

iff (x , y )is as close toLas we please whenever the distance from the point(x , y )to the point(a, b)is sufficiently small, but not zero.

Definition

A functionf is continuous at the point(a, b)if lim

(x ,y )→(a,b)f (x , y ) = f (a, b).

A function is continuous on a region D in the xy -plane if it is continuous at each point of D.

(6)

Lecture 3.

Definitions

Definition

The functionf has a limitLat the point(a, b), written

(x ,y )→(a,b)lim f (x , y ) = L

iff (x , y )is as close toLas we please whenever the distance from the point(x , y )to the point(a, b)is sufficiently small, but not zero.

Definition

A functionf is continuous at the point(a, b)if lim

(x ,y )→(a,b)f (x , y ) = f (a, b).

A function is continuous on a region D in the xy -plane if it is continuous at each point of D.

(7)

Lecture 3.

The basic theorem

Recall that anelementary function is a function built up of a finite combination of constant functions, field operations (addition, multiplication, division, and root extractions–the elementary operations)–and algebraic, exponential, and logarithmic functions and their inverses under repeated compositions. Among the simplest elementary functions are the logarithm, exponential function (including the hyperbolic functions), power function, and trigonometric functions.

We can easily extend the above definition to multi-variable functions.

Theorem

All elementary functions are continuous at all points where they are defined.

(8)

Lecture 3.

The basic theorem

Recall that anelementary function is a function built up of a finite combination of constant functions, field operations (addition, multiplication, division, and root extractions–the elementary operations)–and algebraic, exponential, and logarithmic functions and their inverses under repeated compositions. Among the simplest elementary functions are the logarithm, exponential function (including the hyperbolic functions), power function, and trigonometric functions.

We can easily extend the above definition to multi-variable functions.

Theorem

All elementary functions are continuous at all points where they are defined.

(9)

Lecture 3.

The basic theorem

Recall that anelementary function is a function built up of a finite combination of constant functions, field operations (addition, multiplication, division, and root extractions–the elementary operations)–and algebraic, exponential, and logarithmic functions and their inverses under repeated compositions. Among the simplest elementary functions are the logarithm, exponential function (including the hyperbolic functions), power function, and trigonometric functions.

We can easily extend the above definition to multi-variable functions.

Theorem

All elementary functions are continuous at all points where they are defined.

(10)

Lecture 3.

Exercise 3.1

Are the following functions continuous at all points in the given regions?

1 1

x2+y2 on the square −1 ≤ x ≤ 1, −1 ≤ y ≤ 1;

2 1

x2+y2 on the square 1 ≤ x ≤ 2, 1 ≤ y ≤ 2;

3 y

x2+2 on the disk x2+y2≤ 1;

4 esin x

cos y on the rectangle −π/2 ≤ x ≤ π/2, 0 ≤ y ≤ π/4;

5 tan(xy ) on the square −2 ≤ x ≤ 2, −2 ≤ y ≤ 2;

6 p2x − y on the disk x2+y2≤ 4.

(11)

Lecture 3.

Exercise 3.2

Find the limits of the following functions as (x , y ) −→ 0.

1 f (x , y ) = e−x−y;

2 g(x , y ) = x2+y2;

3 h(x , y ) = x2x+1;

4 i(x , y ) = 2+sin yx +y ;

5 j(x , y ) = sin(xx2+y2+y22).

(12)

Lecture 3.

Definition

Definition

For all points at which the limits exist, we define the partial derivatives off at the point (a, b) by

fx(a, b) = lim

h→0

f (a + h, b) − f (a, b)

h ,

fy(a, b) = lim

h→0

f (a, b + h) − f (a, b)

h .

If we let a and b vary, we have the partial derivative functions fx(x , y ) and fy(x , y ).

fx(a, b) is arate of change of f with respect to x at the point (a, b);

fy(a, b) is arate of change of f with respect to y at the point (a, b).

(13)

Lecture 3.

Definition

Definition

For all points at which the limits exist, we define the partial derivatives off at the point (a, b) by

fx(a, b) = lim

h→0

f (a + h, b) − f (a, b)

h ,

fy(a, b) = lim

h→0

f (a, b + h) − f (a, b)

h .

If we let a and b vary, we have the partial derivative functions fx(x , y ) and fy(x , y ).

fx(a, b) is arate of change of f with respect to x at the point (a, b);

fy(a, b) is arate of change of f with respect to y at the point (a, b).

(14)

Lecture 3.

Definition

Definition

For all points at which the limits exist, we define the partial derivatives off at the point (a, b) by

fx(a, b) = lim

h→0

f (a + h, b) − f (a, b)

h ,

fy(a, b) = lim

h→0

f (a, b + h) − f (a, b)

h .

If we let a and b vary, we have the partial derivative functions fx(x , y ) and fy(x , y ).

fx(a, b) is arate of change of f with respect to x at the point (a, b);

fy(a, b) is arate of change of f with respect to y at the point (a, b).

(15)

Lecture 3.

Definition

Definition

For all points at which the limits exist, we define the partial derivatives off at the point (a, b) by

fx(a, b) = lim

h→0

f (a + h, b) − f (a, b)

h ,

fy(a, b) = lim

h→0

f (a, b + h) − f (a, b)

h .

If we let a and b vary, we have the partial derivative functions fx(x , y ) and fy(x , y ).

fx(a, b) is arate of change of f with respect to x at the point (a, b);

fy(a, b) is arate of change of f with respect to y at the point (a, b).

(16)

Lecture 3.

Alternative Notations

If z = f (x , y ), we can write

fx(x , y ) = ∂z∂x and fy(x , y ) = ∂z∂y, fx(a, b) = ∂z∂x |(a,b) and fy(a, b) = ∂y∂z |(a,b).

(17)

Lecture 3.

Visualizing Partial Derivatives on a Graph

The partial derivative fx(a, b) is the slope of the tangent line to the curve

Graph(f ) ∩ {y = b}

at x = a.

Analogically for fy(a, b).

(18)

Lecture 3.

Exercise 3.3

The surface z = f (x , y ) is shown on the following figure. The points A and B are on the plane z = 0.

(a) What is the sign of (i) fx(A)?

(ii) fy(A)?

(b) The point P in the plane z = 0 moves along a straight line from A to B. How does the sign of fx(P) change? How does the sign of fy(P) change?

(19)

Lecture 3.

Exercise 3.4

The following figure shows the saddle-shaped surface z = f (x , y ).

(a) What is the sign of fx(0, 5)?

(b) What is the sign of fy(0, 5)?

(20)

Lecture 3.

Exercise 3.5

The following figure shows contours of f (x , y ) with values of f on the contours omitted.

If fx(P) > 0, find the sign of

(a)fy(P); (b)fy(Q); (c)fx(Q).

(21)

Lecture 3.

Differentiate with the respect to one variable, regarding the others variables as constants!

Example. Find fx(3, 2) and fy(1, 1) algebraically, where

f (x , y ) = x2 y + 1.

Solution 1.

f (x , 2) = x32, thus f0(x , 2) = 2x3, hence fx(3, 2) = 2.

f (1, y ) = y +11 , thus f0(1, y ) = −(y +1)1 2, hence fy(1, 1) = −14. Solution 2.

fx(x , y ) = y +12x , thus fx(3, 2) = 2. fy(x , y ) = −(y +1)x2 2, thus fy(1, 1) = −14.

(22)

Lecture 3.

Differentiate with the respect to one variable, regarding the others variables as constants!

Example. Find fx(3, 2) and fy(1, 1) algebraically, where

f (x , y ) = x2 y + 1. Solution 1.

f (x , 2) = x32, thus f0(x , 2) = 2x3, hence fx(3, 2) = 2.

f (1, y ) = y +11 , thus f0(1, y ) = −(y +1)1 2, hence fy(1, 1) = −14. Solution 2.

fx(x , y ) = y +12x , thus fx(3, 2) = 2. fy(x , y ) = −(y +1)x2 2, thus fy(1, 1) = −14.

(23)

Lecture 3.

Differentiate with the respect to one variable, regarding the others variables as constants!

Example. Find fx(3, 2) and fy(1, 1) algebraically, where

f (x , y ) = x2 y + 1. Solution 1.

f (x , 2) = x32, thus f0(x , 2) = 2x3, hence fx(3, 2) = 2.

f (1, y ) = y +11 , thus f0(1, y ) = −(y +1)1 2, hence fy(1, 1) = −14.

Solution 2.

fx(x , y ) = y +12x , thus fx(3, 2) = 2. fy(x , y ) = −(y +1)x2 2, thus fy(1, 1) = −14.

(24)

Lecture 3.

Differentiate with the respect to one variable, regarding the others variables as constants!

Example. Find fx(3, 2) and fy(1, 1) algebraically, where

f (x , y ) = x2 y + 1. Solution 1.

f (x , 2) = x32, thus f0(x , 2) = 2x3, hence fx(3, 2) = 2.

f (1, y ) = y +11 , thus f0(1, y ) = −(y +1)1 2, hence fy(1, 1) = −14. Solution 2.

fx(x , y ) = y +12x , thus fx(3, 2) = 2.

fy(x , y ) = −(y +1)x2 2, thus fy(1, 1) = −14.

(25)

Lecture 3.

Differentiate with the respect to one variable, regarding the others variables as constants!

Example. Find fx(3, 2) and fy(1, 1) algebraically, where

f (x , y ) = x2 y + 1. Solution 1.

f (x , 2) = x32, thus f0(x , 2) = 2x3, hence fx(3, 2) = 2.

f (1, y ) = y +11 , thus f0(1, y ) = −(y +1)1 2, hence fy(1, 1) = −14. Solution 2.

fx(x , y ) = y +12x , thus fx(3, 2) = 2.

fy(x , y ) = −(y +1)x2 2, thus fy(1, 1) = −14.

(26)

Lecture 3.

Exercise 3.6

(a) Find all the partial derivatives of f (x , y , z) = x2zy3.

(b) Compute fx(1, 2, 1), fy(2, 1, 1) and fz(1, 1, 2).

Solution:

fx(x , y , z) = 2xyz3; fy(x , y , z) = 3xz2y2; fz(x , y , z) = −x2zy23;

fx(1, 2, 1) = 16; fy(2, 1, 1) = 12; fz(1, 1, 2) = −14.

(27)

Lecture 3.

Exercise 3.6

(a) Find all the partial derivatives of f (x , y , z) = x2zy3. (b) Compute fx(1, 2, 1), fy(2, 1, 1) and fz(1, 1, 2).

Solution:

fx(x , y , z) = 2xyz3; fy(x , y , z) = 3xz2y2; fz(x , y , z) = −x2zy23;

fx(1, 2, 1) = 16; fy(2, 1, 1) = 12; fz(1, 1, 2) = −14.

(28)

Lecture 3.

Exercise 3.6

(a) Find all the partial derivatives of f (x , y , z) = x2zy3. (b) Compute fx(1, 2, 1), fy(2, 1, 1) and fz(1, 1, 2).

Solution:

fx(x , y , z) = 2xyz3;

fy(x , y , z) = 3xz2y2; fz(x , y , z) = −x2zy23;

fx(1, 2, 1) = 16; fy(2, 1, 1) = 12; fz(1, 1, 2) = −14.

(29)

Lecture 3.

Exercise 3.6

(a) Find all the partial derivatives of f (x , y , z) = x2zy3. (b) Compute fx(1, 2, 1), fy(2, 1, 1) and fz(1, 1, 2).

Solution:

fx(x , y , z) = 2xyz3; fy(x , y , z) = 3xz2y2;

fz(x , y , z) = −x2zy23;

fx(1, 2, 1) = 16; fy(2, 1, 1) = 12; fz(1, 1, 2) = −14.

(30)

Lecture 3.

Exercise 3.6

(a) Find all the partial derivatives of f (x , y , z) = x2zy3. (b) Compute fx(1, 2, 1), fy(2, 1, 1) and fz(1, 1, 2).

Solution:

fx(x , y , z) = 2xyz3; fy(x , y , z) = 3xz2y2; fz(x , y , z) = −x2zy23;

fx(1, 2, 1) = 16; fy(2, 1, 1) = 12; fz(1, 1, 2) = −14.

(31)

Lecture 3.

Exercise 3.6

(a) Find all the partial derivatives of f (x , y , z) = x2zy3. (b) Compute fx(1, 2, 1), fy(2, 1, 1) and fz(1, 1, 2).

Solution:

fx(x , y , z) = 2xyz3; fy(x , y , z) = 3xz2y2; fz(x , y , z) = −x2zy23;

fx(1, 2, 1) = 16;

fy(2, 1, 1) = 12; fz(1, 1, 2) = −14.

(32)

Lecture 3.

Exercise 3.6

(a) Find all the partial derivatives of f (x , y , z) = x2zy3. (b) Compute fx(1, 2, 1), fy(2, 1, 1) and fz(1, 1, 2).

Solution:

fx(x , y , z) = 2xyz3; fy(x , y , z) = 3xz2y2; fz(x , y , z) = −x2zy23;

fx(1, 2, 1) = 16; fy(2, 1, 1) = 12;

fz(1, 1, 2) = −14.

(33)

Lecture 3.

Exercise 3.6

(a) Find all the partial derivatives of f (x , y , z) = x2zy3. (b) Compute fx(1, 2, 1), fy(2, 1, 1) and fz(1, 1, 2).

Solution:

fx(x , y , z) = 2xyz3; fy(x , y , z) = 3xz2y2; fz(x , y , z) = −x2zy23;

fx(1, 2, 1) = 16; fy(2, 1, 1) = 12; fz(1, 1, 2) = −14.

(34)

Lecture 3.

Exercise 3.7

Find the partial derivatives:

1 fx and fy if f (x , y ) = 5x2y3+8xy2− 3x2;

2

∂y(3x5y7− 32x4y3+5xy );

3

∂x(y√ x );

4 Fv if F = mv22;

5

∂x

1

2πσe−(x−µ)2/(2σ2)

;

6 ∂m

∂v if m = √ m0

1−v2/c2.

7 gx if g(x , y ) = ln(yexy);

8 ∂z

∂y |(1,0,5) if z = ex +2ysin y ;

9 ∂f

∂x |(π/3,1) if f (x , y ) = x ln(y cos x ).

(35)

Lecture 3.

Exercise 3.7

Find the partial derivatives:

1 fx and fy if f (x , y ) = 5x2y3+8xy2− 3x2;

2

∂y(3x5y7− 32x4y3+5xy );

3

∂x(y√ x );

4 Fv if F = mv22;

5

∂x

1

2πσe−(x−µ)2/(2σ2)

;

6 ∂m

∂v if m = √ m0

1−v2/c2.

7 gx if g(x , y ) = ln(yexy);

8 ∂z

∂y |(1,0,5) if z = ex +2ysin y ;

9 ∂f

∂x |(π/3,1) if f (x , y ) = x ln(y cos x ).

(36)

Lecture 3.

Exercise 3.7

Find the partial derivatives:

1 fx and fy if f (x , y ) = 5x2y3+8xy2− 3x2;

2

∂y(3x5y7− 32x4y3+5xy );

3

∂x(y√ x );

4 Fv if F = mv22;

5

∂x

1

2πσe−(x−µ)2/(2σ2)

;

6 ∂m

∂v if m = √ m0

1−v2/c2.

7 gx if g(x , y ) = ln(yexy);

8 ∂z

∂y |(1,0,5) if z = ex +2ysin y ;

9 ∂f

∂x |(π/3,1) if f (x , y ) = x ln(y cos x ).

(37)

Lecture 3.

Exercise 3.7

Find the partial derivatives:

1 fx and fy if f (x , y ) = 5x2y3+8xy2− 3x2;

2

∂y(3x5y7− 32x4y3+5xy );

3

∂x(y√ x );

4 Fv if F = mv22;

5

∂x

1

2πσe−(x−µ)2/(2σ2)

;

6 ∂m

∂v if m = √ m0

1−v2/c2.

7 gx if g(x , y ) = ln(yexy);

8 ∂z

∂y |(1,0,5) if z = ex +2ysin y ;

9 ∂f

∂x |(π/3,1) if f (x , y ) = x ln(y cos x ).

(38)

Lecture 3.

Exercise 3.7

Find the partial derivatives:

1 fx and fy if f (x , y ) = 5x2y3+8xy2− 3x2;

2

∂y(3x5y7− 32x4y3+5xy );

3

∂x(y√ x );

4 Fv if F = mv22;

5

∂x

1

2πσe−(x−µ)2/(2σ2)

;

6 ∂m

∂v if m = √ m0

1−v2/c2.

7 gx if g(x , y ) = ln(yexy);

8 ∂z

∂y |(1,0,5) if z = ex +2ysin y ;

9 ∂f

∂x |(π/3,1) if f (x , y ) = x ln(y cos x ).

(39)

Lecture 3.

Exercise 3.7

Find the partial derivatives:

1 fx and fy if f (x , y ) = 5x2y3+8xy2− 3x2;

2

∂y(3x5y7− 32x4y3+5xy );

3

∂x(y√ x );

4 Fv if F = mv22;

5

∂x

1

2πσe−(x−µ)2/(2σ2)

;

6 ∂m

∂v if m = √ m0

1−v2/c2.

7 gx if g(x , y ) = ln(yexy);

8 ∂z

∂y |(1,0,5) if z = ex +2ysin y ;

9 ∂f

∂x |(π/3,1) if f (x , y ) = x ln(y cos x ).

(40)

Lecture 3.

Exercise 3.7

Find the partial derivatives:

1 fx and fy if f (x , y ) = 5x2y3+8xy2− 3x2;

2

∂y(3x5y7− 32x4y3+5xy );

3

∂x(y√ x );

4 Fv if F = mv22;

5

∂x

1

2πσe−(x−µ)2/(2σ2)

;

6 ∂m

∂v if m = √ m0

1−v2/c2.

7 gx if g(x , y ) = ln(yexy);

8 ∂z

∂y |(1,0,5) if z = ex +2ysin y ;

9 ∂f

∂x |(π/3,1) if f (x , y ) = x ln(y cos x ).

(41)

Lecture 3.

Exercise 3.7

Find the partial derivatives:

1 fx and fy if f (x , y ) = 5x2y3+8xy2− 3x2;

2

∂y(3x5y7− 32x4y3+5xy );

3

∂x(y√ x );

4 Fv if F = mv22;

5

∂x

1

2πσe−(x−µ)2/(2σ2)

;

6 ∂m

∂v if m = √ m0

1−v2/c2.

7 gx if g(x , y ) = ln(yexy);

8 ∂z

∂y |(1,0,5) if z = ex +2ysin y ;

9 ∂f

∂x |(π/3,1) if f (x , y ) = x ln(y cos x ).

(42)

Lecture 3.

Exercise 3.7

Find the partial derivatives:

1 fx and fy if f (x , y ) = 5x2y3+8xy2− 3x2;

2

∂y(3x5y7− 32x4y3+5xy );

3

∂x(y√ x );

4 Fv if F = mv22;

5

∂x

1

2πσe−(x−µ)2/(2σ2)

;

6 ∂m

∂v if m = √ m0

1−v2/c2.

7 gx if g(x , y ) = ln(yexy);

8 ∂z

∂y |(1,0,5) if z = ex +2ysin y ;

9 ∂f

∂x |(π/3,1) if f (x , y ) = x ln(y cos x ).

(43)

Lecture 3.

Exercise 3.7

Find the partial derivatives:

1 fx and fy if f (x , y ) = 5x2y3+8xy2− 3x2;

2

∂y(3x5y7− 32x4y3+5xy );

3

∂x(y√ x );

4 Fv if F = mv22;

5

∂x

1

2πσe−(x−µ)2/(2σ2)

;

6 ∂m

∂v if m = √ m0

1−v2/c2.

7 gx if g(x , y ) = ln(yexy);

8 ∂z

∂y |(1,0,5) if z = ex +2ysin y ;

9 ∂f

∂x |(π/3,1) if f (x , y ) = x ln(y cos x ).

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