The equation is the so-called “standard form” equation of a line.
The inequality represents a region of the plane called a “half-space”, and the points that satisfy the inequality constitute the entire half of the plane which lies to one side of the line.
A geometric approach
Let be a vector. We’ll show its direction is perpendicular to the line .
Suppose is any fixed point on the line, so . Then let be some other point. Now is on the line if and only if . Equivalently, . But the equation holds exactly when the displacement is a vector perpendicular to .
So the points which satisfy form a line perpendicular to .
Since the ray is perpendicular to the line, we can find a point which lies on the line. Solving for we have: and satisfies . It is also the closest point on the line to the origin and has magnitude .
So changing in the equation moves the solution set (line) forwards or backwards along to a new line whose distance to is proportional to .
Inequality
Define the function . We know is a solution to and the other solutions form a line perpendicular to which passes through . Since is computed as a dot product, the value of is proportional to the length of the projection of along the direction. Also, is negative when the projection points in the opposite direction of . In particular for every .
To know which points satsify simply look at all the points which satisfy for
The solutions of form a line perpendicular to passing through with equation so the contours of are the lines .
The half-space is generated by the lines . Equivalently, if is any point on the line then the half-space consists of all points whose projections in the direction are “not as far” along as achieves. So starting anywhere on the line and moving along gives a point in the half-space .