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Algebra / English

Vectors | Chapter 1, Essence of linear algebra

3Blue1Brown · YouTube · 9:51

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This segment introduces the concept of a vector in linear algebra by contrasting three perspectives: the physics student's view (arrows in space), the computer science student's view (ordered lists of numbers), and the mathematician's abstract view. It establishes the standard geometric representation of vectors anchored at the origin of a coordinate system. The video then defines the two fundamental operations on vectors: addition, demonstrated via the tip-to-tail method and component-wise arithmetic, and scalar multiplication, explained as scaling (stretching, shrinking, or reversing) a vector.

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Chapters

0:00Introduction to Vectors0:31Physics Perspective: Arrows in Space0:52Computer Science Perspective: Lists of Numbers1:26Mathematician's Perspective & Geometric Setup2:53Coordinate Systems and Vector Components4:05Three-Dimensional Vectors4:37Vector Addition6:54Scalar Multiplication

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Linear algebra is built upon the foundation of vectors. To understand them fully, we must look through three distinct lenses. First, the physicist sees a vector as an arrow in space defined solely by its length and direction; it can be moved anywhere without changing its identity. Second, the computer scientist views a vector simply as an ordered list of numbers, like coordinates for a house's size and price. Third, the mathematician generalizes this to any object that supports sensible addition and scalar multiplication. For our purposes, we will primarily use the geometric view: arrows rooted at the origin of a coordinate system.

In a 2D plane with x and y axes intersecting at the origin, a vector's coordinates tell us how to travel from the origin to the vector's tip. The first number dictates horizontal movement (right is positive, left is negative), and the second dictates vertical movement (up is positive, down is negative). We write these pairs vertically in brackets to distinguish them from points. This logic extends to 3D space by adding a z-axis, where a vector is represented by a triplet of numbers corresponding to movements along the x, y, and z axes respectively.

The two most critical operations are vector addition and scalar multiplication. Adding two vectors geometrically involves placing the tail of the second vector at the head of the first; the sum is the vector drawn from the start to the finish. Numerically, this corresponds to adding their respective components (x1+x2x_1+x_2 and y1+y2y_1+y_2). Scalar multiplication acts as 'scaling.' Multiplying by a number greater than 1 stretches the vector, a fraction shrinks it, and a negative number flips its direction while adjusting its length. Component-wise, you simply multiply each entry by the scalar. More precisely, length is multiplied by |c|: only 0<|c|<1 shortens it, negative c reverses it, and c=0c=0 yields the zero vector. Column notation is a convention; bracket orientation alone is not a mathematical distinction between a point and a vector.

Knowledge cards

01

Vector Perspectives

Vectors can be understood physically as free-floating arrows defined by magnitude and direction, or computationally as fixed lists of numerical data. Linear algebra bridges these by treating numerical lists as geometric objects.

v⃗=[xy]\vec{v} = \begin{bmatrix} x \\ y \end{bmatrix}
02

Geometric Representation

Rooting a free vector at the origin is a convenient representative. Its displacement remains unchanged by translation. Vector coordinates depend on the chosen basis; coordinates of points additionally depend on the origin.

Origin→Tip(x,y)\text{Origin} \to \text{Tip}(x,y)
03

Vector Addition

Defined geometrically by the 'tip-to-tail' method. Algebraically, it is performed by summing corresponding components of the input vectors.

[x1y1]+[x2y2]=[x1+x2y1+y2]\begin{bmatrix} x_1 \\ y_1 \end{bmatrix} + \begin{bmatrix} x_2 \\ y_2 \end{bmatrix} = \begin{bmatrix} x_1+x_2 \\ y_1+y_2 \end{bmatrix}
04

Scalar Multiplication

The scalar c multiplies length by |c|. Positive c preserves direction, negative c reverses it, and zero gives the zero vector, whose direction is undefined.

c⋅[xy]=[cxcy]c \cdot \begin{bmatrix} x \\ y \end{bmatrix} = \begin{bmatrix} cx \\ cy \end{bmatrix}

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  • Vectors ExplanationAt 0:52
    Why this connection?

    The reviewed perspectives card and summaries connect vectors as displacements with ordered components, then explain tip-to-tail addition and scalar multiplication. Translating a free vector preserves displacement, while coordinates depend on the chosen basis. Multiplication by cc scales length by ∣c∣|c|; c=0c=0 gives the zero vector with no direction.

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