schedule
week 1
- Part A: Vectors, Determinants, Planes
- Part B: Matrices and Systems of Equations
- Part C: Parametric Equations for Curves
week 2
- Part A: Functions of Two Variables, Tangent Approximation and Optimization
- Part B: Chain Rule, Gradient and Directional Derivatives
- Part C: Lagrange Multipliers and Constrained Differentials
week 3
- Part A: Double Integrals
- Part B: Vector Fields and Line Integrals
- Part C: Green’s Theorem
week 4
- Part A: Triple Integrals
- Part B: Flux and the Divergence Theorem
- Part C: Line Integrals and Stokes’ Theorem
Vectors and Matrices
Part A: Vectors, Determinants, Planes
- vector: has direction and magnitude/length
- represented using coordinate system
a1î + a2ĵ + a3k̂ = < a1, a2, a3> $$|\vec{A}| = \sqrt{a_1 + a_2 + a_3}$$
A⃗ ⋅ B⃗ = ∑aibi = a1b1 + a2b2 + a3b3
geometrically A⃗ ⋅ B⃗ = |A⃗||B⃗|cosθ
- law of cosines: if C⃗ = A⃗ − B⃗, then define
|C⃗| = |A⃗|2 + |B⃗|2 − 2|A⃗||B⃗|cosθ
we know |C⃗|2 = C⃗ ⋅ C⃗ = (A⃗ − B⃗) ⋅ (A⃗ − B⃗) = |A⃗|2 + |B⃗|2 − 2A⃗ ⋅ B⃗
then we get: 2|A⃗||B⃗|cosθ = 2A⃗ ⋅ B⃗
- the dot product can be used for
- computing lengths and angles
- detect orthogonality
- A⃗ ⋅ B⃗ = 0 means they are perpendicular to each other, cosθ, θ = 0deg, 90deg
- vector components
vector components
- find a component A⃗ along direction u⃗, where u⃗ is a unit vector: |A⃗cosθ|
- orthogonal projection of A on u⃗, leg parallel to u⃗: |A|cosθ or $$\frac{\vec{A} \vec{u}}{|\vec{u}|}$$
- component (length) of a vector is scalar
- find a component A⃗ along direction u⃗, where u⃗ is a unit vector: |A⃗cosθ|
area and determinants in 2D
determinant of A⃗, B⃗ is +/- area of a parallelogram, |A⃗||B⃗|sinθ = det(A⃗, B⃗)
area of triangle: $$\frac{1}{2} det(\vec{A}, \vec{B})$$
volumes and determinants in space
- det(A⃗, B⃗, C⃗) = +/- volume of parallelepiped
- Aij = (−1)i + j|Aij|
cross products
- 2 vectors in 3D space => vector
$$\vec{A} \times \vec{B} = \begin{vmatrix} \vec{i} & \vec{j} & \vec{k}\\ a_1 & a_2 & a_3\\ b_1 & b_2 & b_3\\ \end{vmatrix}$$
- theorem:
- the length of the cross product of A⃗ and B⃗, is the area of the parallelogram
- the direction of the cross product of A⃗ and B⃗ is perpendicular to the plane of the parallelogram
- direction is based on the right-hand rule
- volume of parallelepiped:
- area(base) times height
- |B⃗ × C⃗| × (A⃗ ⋅ n⃗)
- where n⃗ is the vector perpendicular to $$\frac{\vec{B} \times \vec{C}}{|\vec{B} \times \vec{C}|}$$
- rules of cross products
- B⃗ × C⃗ ≠ C⃗ × B⃗, B⃗ × C⃗ = −C⃗ × B⃗
- B⃗ × B⃗ = 0
equations of planes
- application of cross product: 3 points in space, equation of plane P1, P2, P3, is point P on that plane?
- consider vectors P1, P, P1, P2, P1, P3: is the parallelogram completely flat?
- is det(P1P, P1P2, P1P3) = 0
- P is in the plane, only when $$\vec{P_1 P}$$ is perpendicular N⃗, where N⃗ is a cross product
- $$\vec{P_1 P} \cdot (\vec{P_1 P_2} \times \vec{P_1 P_3}) = 0$$
- consider vectors P1, P, P1, P2, P1, P3: is the parallelogram completely flat?
- application of cross product: 3 points in space, equation of plane P1, P2, P3, is point P on that plane?
Part B: Matrices and Systems of Equations
matrix multiplication
- often have linear relations
- entries in matrix product AX
- dot products between rows of A and columns of X
- product AB represents doing transformation B then transformation A
- identity matrix: do nothing
matrix inverse
if we have function of u in terms of x, can use matrix inverse to express function of x in terms of u
if A is the inverse of M: AM = I, MA = I
- M = A−1
if AX = B
A−1(AX) = A−1B
X = A−1B
invert matrix by hand:
- $$A^{-1} = \frac{1}{det(A)}adj(A)$$
equations of planes ii
ax + by + cz = d
- find plane perpendicular to a vector
- point P is in the plane, whenever $$\vec{OP} \cdot \vec{N} = 0$$
- if plane goes through origin
- < a, b, c>, is the normal vector for the plane
- plane in point-normal form:
- need point P0 and vector N orthogonal to plane, we can also say N is normal to the plane
- since the vector $$\vec{P_0 P}$$ is in the plane, we can say $$N \cdot \vec{P_0 P} = 0$$
- need point P0 and vector N orthogonal to plane, we can also say N is normal to the plane
distance to plane/line
- point to plane: need a point P, plane with normal N⃗ and containing point Q $$\text{distance} = |PR| = |\vec{PQ}| \text{cos} \theta = |\vec{PQ} \cdot \frac{N}{|N|}|$$
- point to line: point P, line with direction vector v and containing point Q $$d = |QP| \text{sin} \theta = |\vec{QP} \cdot \frac{v}{|v|}|$$
- distance between parallel planes
- reduce the problem to distance from point to plane
- distance between skew lines
- place lines in parallel planes and find distance between planes
- find normal M = v1 × v2
- find plane perpendicular to a vector
linear systems and planes
- 3 planes intersect => two planes intersect and form a line => find the line that intersects in the third plane
- if set of solutions to 3by3 linear system is not a single point => no solution, line or plane
- 3rd plane might be parallel to the line where the first two planes intersect
- if line contained in third plane: infinite solution
- if line is parallel to third plane and not contained, then there are no solutions
- 3rd plane might be parallel to the line where the first two planes intersect
solutions to square systems
- can’t always find the inverse of the matrix; when the determinant is 0
- homogenous system: right hand side is 0
- origin is always a solution
- if det(A) is not 0: can solve the system using inverse of A
- if det(A) = 0: det(vecN1, vecN2, vecN3) = 0 then vecN1, vecN2, vecN3 are coplanar (in the same plane)
- infinite many solutions
- origin is always a solution
- general case:
- if det(A) is not zero: X = A−1B
- if det(A) is zero, either no solution or infinitely many solutions
Part C: Parametric Equations for Curves
Session 15: Equations of Lines
- intersection of 2 planes
- trajectory of moving point
- paramatric form: point moving in space traces out path over time => position of point and time
- parametric form: equation of line that passes through the point P and is parallel to the vector v⃗
r⃗ = r⃗0 + tv⃗ = < x0 + tv1, y0 + tv2, z0 + tv3>, where r⃗0 is the vector using the point P
- then you break the vector into equations
- parametric form: intersection of two planes
- parametric form: line through two points
Session 16: Intersection of a Line and a Plane
- two points vs. a line
- substitute the point, and see if value is larger than the sum of the unknowns => tells you which side the points are on
- if line is in the plane, than plugging (x(t), y(t), z(t)), we always get the value for the plane
- if the line is parallel to the plane, then never get that value, get another constant
- two points vs. a line
Session 17: General Parametric Equations; the Cycloid
- parametric curves:
Session 18: Point (Cusp) on Cycloid
Session 19: Velocity and Acceleration
Session 20: Velocity and Arc Length
Session 21: Kepler’s Second Law
Partial Derivatives
Part A: Functions of Two Variables, Tangent Approximation and Optimization
Session 24: Functions of Two Variables: Graphs
Session 25: Level Curves and Contour Plots
Session 26: Partial Derivatives
Session 27: Approximation Formula
Session 28: Optimization Problems
Session 29: Least Squares
Session 30: Second Derivative Test
Session 31: Example
Part B: Chain Rule, Gradient and Directional Derivatives
Session 32: Total Differentials and the Chain Rule
Session 33: Examples
Session 34: The Chain Rule with More Variables
Session 35: Gradient: Definition, Perpendicular to Level Curves
Session 36: Proof
Session 37: Example
Session 38: Directional Derivatives
Part C: Lagrange Multipliers and Constrained Differentials
Session 39: Statement of Lagrange Multipliers and Example
Session 40: Proof of Lagrange Multipliers
Session 41: Advanced Example
Session 42: Constrained Differentials
Session 43: Clearer Notation
Session 44: Example
Double Integrals and Line Integrals in the Plane
Part A: Double Integrals
Session 47: Definition of Double Integration
Session 48: Examples of Double Integration
Session 49: Exchanging the Order of Integration
Session 50: Double Integrals in Polar Coordinates
Session 51: Applications: Mass and Average Value
Session 52: Applications: Moment of Inertia
Session 53: Change of Variables
Session 54: Example: Polar Coordinates
Session 55: Example
Part B: Vector Fields and Line Integrals
Session 56: Vector Fields
Session 57: Work and Line Integrals
Session 58: Geometric Approach
Session 59: Example: Line Integrals for Work
Session 60: Fundamental Theorem for Line Integrals
Session 61: Conservative Fields, Path Independence, Exact Differentials
Session 62: Gradient Fields
Session 63: Potential Functions
Session 64: Curl
Part C: Green’s Theorem
Session 65: Green’s Theorem
Session 66: Curl(F) = 0 Implies Conservative
Session 67: Proof of Green’s Theorem
Session 68: Planimeter: Green’s Theorem and Area
Session 69: Flux in 2D
Session 70: Normal Form of Green’s Theorem
Session 71: Extended Green’s Theorem: Boundaries with Multiple Pieces
Session 72: Simply Connected Regions and Conservative
Triple Integrals and Surface Integrals in 3-Space
Part A: Triple Integrals
Session 74: Triple Integrals: Rectangular and Cylindrical Coordinates
Session 75: Applications and Examples
Session 76: Spherical Coordinates
Session 77: Triple Integrals in Spherical Coordinates
Session 78: Applications: Gravitational Attraction
Part B: Flux and the Divergence Theorem
Session 79: Vector Fields in Space
Session 80: Flux Through a Surface
Session 81: Calculating Flux; Finding ndS
Session 82: ndS for a Surface z = f(x, y)
Session 83: Other Ways to Find ndS
Session 84: Divergence Theorem
Session 85: Physical Meaning of Flux; Del Notation
Session 86: Proof of the Divergence Theorem
Session 87: Diffusion Equation
Part C: Line Integrals and Stokes’ Theorem
Session 88: Line Integrals in Space
Session 89: Gradient Fields and Potential Functions
Session 90: Curl in 3D
Session 91: Stokes’ Theorem
Session 92: Proof of Stokes’ Theorem
Session 93: Example
Session 94: Simply Connected Regions; Topology
Session 95: Stokes’ Theorem and Surface Independence
Session 96: Summary of Multiple Integration