2.2 Homogeneous and Particular
Consider the system of two equations and . Chapter 1 tells us what to expect: two independent conditions on three unknowns leave a line of solutions. This section is about the structure of that line — a structure shared by the solution set of every linear system, of any size.
First replace the right-hand sides by zeros: and . This is the homogeneous version of the system, in the sense of Section 1.4. It is guaranteed to be consistent, since works, and a short elimination shows its solutions are all multiples of a single vector: . In the language of the previous section, the homogeneous solution set is a span — here, a line through the origin.
Now return to the original right-hand sides. One solution can be found by trial: satisfies both equations (check: and ). It is a particular solution in the sense of Section 1.4 — nothing special about it, just some point that works. The figure below shows both solution sets at once.
Explore in 3D (opens in a new tab)Two parallel straight lines in 3D: a blue line through the origin holding the homogeneous solutions, and a red line through the marked point (2, 0, 1) holding the full solution set. A short gray segment connects the origin to that point, showing the translation by one particular solution. There are no sliders.
Explore the figure
- Orbit until both lines are clearly visible. Confirm they are parallel — same direction vector, different anchor points.
- The blue line passes through the origin; the red line does not. Which of the two systems could you have guessed is the homogeneous one, from the picture alone?
- Follow the gray segment from the origin to the red point. Every point of the red line is reached the same way: start on the blue line, then add .
- Would a different particular solution — any other point of the red line — have served equally well as the anchor?
One solution plus all homogeneous solutions
Here is the reasoning, and it never uses the specific numbers. Write the system as , shorthand that Section 2.4 makes official: is the matrix of coefficients, is the list of left-hand sides evaluated at the point , and is the list of right-hand sides. Left-hand sides of linear equations add and scale term by term, so and ; that is all the argument uses. Suppose solves the system and solves the homogeneous system . Then , so is again a solution. Conversely, if is any solution, then , so differs from by a homogeneous solution. Both directions together say:
Geometrically: the solution set of a consistent system is a translated copy of the homogeneous solution set — the same span, picked up and carried to , exactly as the gray segment in the figure shows. The homogeneous system contributes the shape and direction; the particular solution contributes only the location.
"A short elimination shows its solutions are all multiples of a single vector" is the one step above that the section asks you to take on faith. Here it is, done by machine: the null space of the coefficient matrix, which is precisely the solution set of .
Worth noticing what the check had to tolerate. The engine returns the basis vector ; the text states . Those are different vectors spanning the same line. The null space itself is a fact — one definite subspace, here that line — but a basis for it is a choice, and the two choices differ. The comparison is therefore made by span rather than entry-by-entry, so the text keeps the scaling it chose for readability and still gets a certificate. An entrywise check would have called a correct book wrong.
An original work of XYZ Homework, built around interactive XYZ 3D figures. Chapters 1–6 follow the topic sequence of Interactive Linear Algebra (Margalit & Rabinoff, Georgia Tech, GNU FDL). Chapter 0's scope (its topics, their order, and the idea each figure shows) follows the Vectors chapter of Ximera's Linear Algebra: An Interactive Introduction. The prose, worked examples and figures were written for this book, which is not affiliated with or endorsed by the authors of either work. License: CC-BY-NC-SA-4.0.