Lessons

Lesson material is from the Study Guide by Richard St. Andre which accompanies Multivariable Calculus: Fourth Edition by James Steward

Section(s)

Concepts to Master

13.1

Rectangular three-dimensional coordinates

Distance between two points

Planes, spheres, and regions in space                          
This section extends the two dimensional x-, y- coordinate system to three dimensions (x, y, z) with three axes, each perpendicular to the others as you might visualize the corner of a room.

13.2

Vectors; Position vector; Length: Unit vector: Standard basis vector (i, j, k)
Vector arithmetic; scalars; Vector properties
This section extends the two dimensional x-, y- coordinate system to three dimensions (x, y, z) with three axes, each perpendicular to the others as you might visualize the corner of a room.                 

13.3

Dot product; properties of dot product
Angle between two vectors; Scalar projection; Work; Direction cosines
The previous section showed you how to add vectors and stretch them (scalar multiplication).   This section gives one way to multiply vectors with the result being a scalar.   The dot product defined in this section provides a convenient way to determine the angle between two vectors.

13.4

Cross product and properties
Area of parallelogram: Scalar triple product; Volume of parallelepiped
This section provides a second way to multiply two three-dimensional vectors - this time producing a third vector perpendicular to the given vectors.  Cross product is defined only for three-dimensional vectors and has many uses; we shall see, for example, in the next section that the cross product of two vectors is useful for determining the equation of the plane formed by those vectors. 

13.5

Equations of lines in space (vector, parametric, and symmetric: Parallel and skew lines
Normal vector; Equations of planes (vector and scalar): Parallel planes: Angle between intersecting planes; Distance from a point to a plane and distance between two planes
This section gives three different, but equivalent "equations" for a line in three-dimensional space - a vector form, a parametric form, and a form similar to that of a line in two dimensions.   Planes in three-dimensional space, which may be thought of as all vectors perpendicular to a given vector, will have an equation form very similar to that of lines in two dimensions.  We will use equations of lines and planes in later chapters when we discuss tangent planes to surfaces - the analog of tangent lines to graphs.

13.6

Cylinders in three-dimensional space
Non-degenerate quadric surfaces
This section describes the equations and graphs of several types of surfaces in three dimensions; they are reminiscent of the conic sections (ellipses, parabolas, and hyperbolas) in two dimensions.  We first start with cylinders, which consist of collections of parallel lines.

13.7
Surfaces

Cylindrical coordinates; Spherical coordinates: Conversion from one set of coordinates to another  
This section describes two other coordinate systems for three-dimensional space.  The first, cylindrical coordinates, is simply polar coordinates in the xy-plane with a z-axis added.  The other, spherical coordinates, is the generalization of polar coordinates to three dimensions, where a distance and two angles are necessary to specify a point.

14.1

Curves

Vector Functions: Limits: Continuity: Curves in Space 
This section extends the concepts of limits and continuity to vector functions.  The "graphs" of vector functions are curves in two- or three-dimensional space.    (In two dimensions, vector functions are another way to look at curves defined by a pair of parametric equations as was done in chapter 11.)

14.2

Derivatives of vector functions; Tangent vector; Properties of derivatives
Smooth curves; Piecewise smooth curves
Integral of vector functions
This section extends the concepts of derivatives and integrals to vector functions.   As you might expect, differentiation and integration is performed component-wise.

14.3

Arc Length of an arc in space: Arc length function: reparametrization
Curvature
Tangent vector: Unit normal vector: Normal plane
This section show you how to determine the arc length of a smooth curve.  Not surprisingly, the process is the same as that for two-dimensional curves defined paramaterically in chapter 11.  This section also contains several concepts for characterizing the shape of a curve; for example, curvature - a measure of how fast the curve is bending at a given point.

14.4

Velocity; Speed; Acceleration
Tangent and normal components of acceleration
All previous notions, such as tangent vectors and curvature, are used in this section to describe motion of an object in tree-dimensional space.

 

Practice Test 1

 

 

15.1

Functions of Several Variables

(AH) Sec 15.1   2, 5, 6, 14, 18, 30, 32, 40, 51-56
In the last chapter we saw that the range of a function could be a multi-dimensional vector.   In this section we study functions whose domains are multi-dimensional; that is, a function whose values are of the form f (x, y) or f (x, y, z).   (Later in chapter 17 we sill study functions with both domain and range multi-dimensional).  A function of two variables, z = f(x, y), will have a graph in three dimensions (x, y, and z).  Since these graphs are sometimes difficult to visualize, we introduce the concept of a "level curve" - a subset of the domain that correspond to a given functional value.

15.2

Limits and Continuity

(AH) Sec 15.2   4, 6, 12, 15, 24, 31, 37
This section extends the concepts of limits and continuity to functions of two or more variables.  Be careful to note that a function can be "one dimensionally" continuous along every line approaching a point and still fail to be continuous at that point.

15.3

Partial Derivatives

(AH) Sec 15.3   4, 5, 6, 12, 20, 28, 35, 40, 50, 58, 64
This section starts the process of finding derivatives for functions of two or more variables.   For two variables, we shall see that there is a derivative in the x-direction and another in the y-direction and these may be obtained by a process similar to that for functions of one variable.  Each of these two "partial" derivatives has, in turn, two partial derivatives; so the original functions has four "second derivatives."  Clairaut's Theorem says that for some functions two of these four are the same.

15.4

Tangent Planes and Linear Approximations

(AH) Sec 15.4   2, 6, 14, 17, 26, 30
This section generalizes the notion of a tangent line for a curve to that of a tangent plane for a surface.  The tangent plane is determined by the tangent lines in the x and y directions.  Tangent planes will be used to define a differential that may be used to find a linear approximation of a functional value.  Differentials and linear approximations generalize to functions with more than two variables.

15.5

The Chain Rule

(AH) Sec 15.5  2, 6, 7, 10, 14, 21, 26, 34, 37
The Chain Rule has different versions depending upon the number of variables involved.   The Chain Rule also comes in handy for finding derivatives by implicit differentiation.

15.6

Directional Derivatives and Gradient

(AH) Sec 15.6  2, 4, 9, 10, 14, 16, 23, 24, 34, 38, 42
The partial derivatives fx (x, y) and fy (x,y) may be thought of as the derivatives in the x-direction and y-directions, respectively.   This sections defines the "directional" derivative for an arbitrary direction u=<a,b> in the xy-plane. fx (x, y) and fy (x, y) will be special cases where the x-direction is specified by i=<1,0> and the y-direction by j=<0,1>.  The vector that points in the direction where the directional derivatives is the largest is called the gradient.

15.7

Maximum and Minimum

(AH) Sec 15.7  2, 6, 11, 16, 28, 31, 50
In this section you will learn how to use partial derivatives to find the maxima and minima of functions of two variables.  The terms, concepts, and procedures are very similar to those for functions of one variable.

15.8

LaGrange Multipliers

(AH) Sec 15.8  4, 8, 10, 18
Maximum and minimum value problems are frequently stated in terms of finding the maximum (or minimum) of a function given a constraint on the variables in the form of an equation.    This section gives another method for doing some of the same type of problems done in Section 15.7.

 

 

16.1

Double Integrals over Rectangles
(AH) Sec 16.1  8, 12

Recall that definite integrals are the limits of Riemann sums and may be used to determine the area under a curve.  This section defines double integrals as the limits of "double" Riemann sums and uses them to find the volume of a solid under a surface.

16.2

Iterated Integrals
(AH) Sec 16.2  4, 8, 16, 23, 26

This section includes Fubini's Theorem - a method for calculating a double integral as two successive uses of the Fundamental Theorem of Calculus for single integrals.  Just as we needed to hold a variable constant when performing partial differentiation, we will need to hold a variable constant in the "partial integration" in this section.

16.3

Double Integrals over General Regions
(AH) Sec 16.3  4, 12, 16, 19, 26, 35, 40

This section extends the idea of a double integral to bounded regions other than rectangles.   Fubini's Theorem may be applied to write them as iterated integrals.

16.4

Double Integrals in Polar Coordinates
(AH) Sec 16.4  8, 11, 15, 20, 24, 29
This section show you how to change a double integral into an iterated integral when the region of integration is described with polar coordinates.

16.5

Applications of Double Integrals
(AH) Sec 16.5  5, 9, 11, 17

This section gives some applications of double integrals for physical phenomenon and for probability distributions involving two variables.

16.6

Surface Area
(AH) Sec 16.6  2, 6, 10, 21
This section computes the area of a surface using a double integral.

16.7

Triple integrals
(AH) Sec 16.7  4, 10, 15, 18, 29, 35
This section extends all the concepts of double integrals to functions of three variables.

16.8

Triple Integrals in Cylindrical and Spherical Coordinates
(AH) Sec 16.8  3, 10, 13, 19, 22, 26
This section extends the notion of polar coordinates for double integrals to cylindrical coordinates for triple integrals.   It also discusses spherical coordinates for triple integrals.  As before, the advantage is that some integrals are easier to evaluate in one of these coordinate systems.

16.9

Change of Variables in Multiple Integrals
(AH) Sec 16.9  3, 6, 8, 11, 13, 20
Change of variable in one dimensions involved determining an intermediate function u = g(x) and corresponding du = g'(x)dx.  The function u = g(x) may be thought of as a transformation of the reals (x is "transformed " to g(x)).   In higher dimensions, there are several intermediate variables involved.  We arrange the analog of du into a maxtrix whose deteminant is called a Jacobian.

Focused Review 

 

 

 

17.1

Vector Fields
(AH) Sec 17.1  4, 22
This section describes functions from R2 to R2, or from R3 to R3.  The functions are knows as vector fields because we think of the domain elements as points in a set (a field of points in a plane or three dimensions) and range elements as two- or three-dimensional vectors associated with those points.  A conservative vector field is one that is the gradient of a function.

17.2

Line Integrals
(AH) Sec 17.2  2, 6, 10, 14, 20, 22, 38
This section generalizes the idea of integrating a single-variable real function over an interval [a, b] in two ways:  (1) to an integral of a function of two or three variables over a curve in two- or three-dimensional space, and (2) to the integral of a vector field over a curve,  Applications of these line integrals include calculating work and finding the mass and center of mass of a wire whose density varies along its length.

17.3

Fundamental Theorem for Line Integrals
(AH) Sec 17.3  5, 6, 8, 13, 16, 18, 20, 22
The Fundamental Theorem of Calculus for functions of one variable tell us how to find the value of a definite integral.  If you think of the gradient of f as analogous to f '(x), then this section uses a similar result to evaluate line integrals in certain forms. 

17.4

Green’s Theorem
(AH) Sec 17.4  4, 8, 10, 14, 16, 20
This section shows you a handy relationship between a double integral over a plane region D and a line integral around teh boundary curve for D.  It also provides an alternate method to calculate the area of a region D.

17.5

Curl and Divergence
(AH) Sec 17.5  3, 7, 13, 15, 16
This section describes two operations in three dimensions that resemble differentiation and may be used to describe fluid flow.  The curl at a point produces a vector that measures the rotation of fluid about a point in the flow.  The div at a point measures the rate of change of fluid flowing from the point (how much the fluid is diverging from the point).

17.6

Parametric Surfaces and their Areas
(AH) Sec 17.6  1, 4, 12, 14, 17, 21, 24, 30, 32, 34, 36, 40
Surfaces in space are two-dimensional objects.  This section shows how to parametrize a surface in a manner similar to the way curves are parameterized except that we need two parametric variables instead of one.  You will also learn how to calculate tangent planes and areas for parametric surfaces.

17.7

Surface Integrals
(AH) Sec 17.7  5, 7, 10, 16, 19, 22, 23
In this section you will see that a surface integral is the two-dimensional version of a line integral.  Just as a line integral was used to determine the length, mass, etc. of a curve, a surface integral will be sued to calculate the area, mass, etc. of a surface.

17.8

Stokes’ Theorem
(AH) Sec 17.8  2, 4, 8, 13...find both sides if Stokes' Theorem and show they are equal
This section and the next provide extensions of Green's Theorem.  Stokes' Theorem may be thought of as Green's Theorem in three dimensions.  Rather than relate a double over a (flat) region in the plane to a line integral around the boundary curve, Stokes' Theorem relates a surface integral for a surface S in three-dimensions to a line-integral around the boundary curve of S.

17.9

Divergence Theorem

(AH) Sec 17.9  5, 6, 8, 11, 16
Stokes' Theorem moves the double integrals and line integrals of Green's Theorem to three-dimensions.  In this section, you will see that the Divergence Theorem may be thought of as boosting the integrals in Green's Theorem up by one dimension.  Instead of Green's double integral relationship to a line integral,  the Divergence Theorem relates a triple integral over a solid E in three- dimensions to a surface integral around the boundary of E.

Focused Review

    

 

 

Linear Algebra

 

4.1

Vector Spaces and Subspaces
(AH) Sec 4.1  2, 9, 12, 16, 34

4.2

Null Spaces, Column Spaces, and Linear Transformations
(AH) Sec 4.2  2, 5, 8, 13, 15, 18, 24

4.3

Linearly Independent Sets; Bases
(AH) Sec 4.3  3, 5, 10, 14, 15 18

4.4

Coordinate Systems
(AH) Sec 4.4  1, 7, 10 11, 14, 28

4.5

The Dimension of a Vector Space
(AH) Sec 4.5  4, 8, 12, 13, 16

4.6

Rank
(AH) Sec 4.6  2, 4, 8, 12, 15

More statements about the Invertible Matrix Theorem

About Rank

4.7

Change of Basis
(AH) Sec 4.7  2, 3, 6, 8, 10

5.1

Eigenvectors and Eigenvalues
(AH) Sec 5.1  3, 6, 8, 15, 20

5.2

The Characteristic Equation
(AH) Sec 5.2  3, 6, 13, 16

5.3

Diagonalization
(AH) Sec 5.3  2, 6, 8, 15, 18

5.4

Eigenvectors and Linear Transformations
(AH) Sec 5.4  2, 4, 6, 8, 12, 15

Final Review