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Multivariable Calculus
Vectors and Dot Products
01Vectors, Components, and Length in Space02Scaling and Adding Vectors: The Parallelogram Rule03The Dot Product and the Law of Cosines04Finding Angles in Space With the Dot Product05The Perpendicularity Test and the Normal Vector to a PlaneProblem set0/10Problem set 20/10MIT problem set0/2Practice∞
Determinants and the Cross Product
01The Component of a Vector Along Any Unit Direction02The 2x2 Determinant and the Area of a Parallelogram03The 3x3 Determinant and the Volume of a Box04The Cross Product and the Right-Hand Rule05The Triple Product and the Volume of a ParallelepipedProblem set0/10Problem set 20/10MIT problem set0/2Practice∞
Matrices and Inverse Matrices
01Why Swapping a Cross Product Flips Its Sign02The Equation of a Plane Through Three Points03Matrix Multiplication: Rows Dotted With Columns04Matrices as Transformations: Identity and Rotation05The Inverse Matrix and Solving AX = B06Computing a 3x3 Inverse: Minors, Cofactors, AdjointProblem set0/10Problem set 20/10MIT problem set0/2Practice∞
Planes and Square Systems
01Planes From a Point and a Normal Vector02Reading the Normal Vector Off a Plane Equation03Three Planes, One Point: Solving a 3x3 System04Invertibility, det A, and the Homogeneous System05When det A = 0: Coplanar Normals and a Line of SolutionsProblem set0/10Problem set 20/10Practice∞

The Component of a Vector Along Any Unit Direction

Why does a single dot product give a vector's component along any direction, and how does that let a pendulum pick its own axes?


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    1. 1

      Two forms of the dot product

      Write both the componentwise definition A⃗⋅B⃗=a1b1+a2b2+a3b3\vec{A} \cdot \vec{B} = a_1 b_1 + a_2 b_2 + a_3 b_3A⋅B=a1​b1​+a2​b2​+a3​b3​ and the geometric form ∣A⃗∣∣B⃗∣cos⁡θ|\vec{A}||\vec{B}|\cos\theta∣A∣∣B∣cosθ, noting both give the same scalar.

    2. 2

      Component of A⃗\vec{A}A along a unit vector u^\hat{u}u^

      Show the projection length is ∣A⃗∣cos⁡θ|\vec{A}|\cos\theta∣A∣cosθ, and carry through the step using ∣u^∣=1|\hat{u}|=1∣u^∣=1 to reach A⃗⋅u^\vec{A} \cdot \hat{u}A⋅u^.

    3. 3

      Coordinate axes as the special case

      Record that dotting with i^\hat{i}i^, j^\hat{j}j^​, k^\hat{k}k^ recovers a1a_1a1​, a2a_2a2​, a3a_3a3​, and state that the same formula works for any direction.

    4. 4

      Pendulum application

      Describe resolving the weight along a tangent T^\hat{T}T^ and normal n^\hat{n}n^ to the arc, identifying the tangential component with swinging and the normal component with tension, computed via dot products.

    Attempt 1 of 2