Vector calculus in plane and space: Distances, Angles and Inner Product
Normal vectors
The dot product in can be used to describe a linear equation with three unknowns.
Normal vector
Let , , , and be real numbers. Write . The linear equation can be written with the aid of the dot product as where . If is not the zero vector, then the set of solutions of the equation is a plane and we call a normal vector of the plane.
If and are two vectors in the plane with equation , then we have and . Subtracting these two equalities yields
We can also read this equality as follows:
that is, the difference vector is perpendicular to the vector . In particular, is a vector which is perpendicular to all the directional vectors of the plane: a normal vector of the plane.
Let be a plane in , and let be a normal vector of .
- The vector is uniquely determined, apart from a scalar multiple.
- A vector in is then, and only then, a directional vector of if .
If and are two vectors in the plane, then and apply. Subtracting these equalities yields , which means that through the properties of the dot product (additivity and associativity with respect to scalar multiplication): In other words, the difference vector is perpendicular to . In particular, directional vectors of the plane are perpendicular to the normal vector .
Something similar applies to lines in the plane: if is the equation of a line, then is a normal vector of the line. The vector is perpendicular to each directional vector of the line.
To see this, we find a linear equation to which is the set of solutions. We do this by choosing three points of that do not to go through one line, and entering them in the general form of the equation:
We choose the three points by the parametric choices , , . In coordinates:
Entering the coordinates of each of these points in the equation above, gives the following system of linear equations in , , , :
A solution with integer values is . This means that the three points, and therefore all points of , are solutions of the equation According to the theory, is a normal vector.
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