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Matrices turn a system of simultaneous linear equations into a single equation Ax=b, which — when A is invertible — is solved in one stroke by x=A−1b. Just as powerfully, the determinant of A classifies the geometry: a non-zero determinant means the planes meet at exactly one point (a unique solution), while a zero determinant means they fail to do so — either meeting in a line or sheet (infinitely many solutions) or not meeting at all (no solution). This lesson writes systems in matrix form, solves them with the inverse, and decodes every geometric configuration of two lines or three planes. It is where determinants, inverses and geometry all come together. The single most important habit to build is this: always compute detA first. It instantly separates the easy "unique solution" world (where you simply apply x=A−1d) from the more interesting singular world, where a second test — consistency — decides between infinitely many solutions and none at all. Examiners deliberately set systems in that singular world precisely because navigating it demands genuine understanding rather than rote inversion.
Solving systems is compulsory pure content for Papers 1 and 2, and it is the most AO3-rich topic in the matrices strand: it asks you to interpret — to translate between algebra (the value of detA, the consistency of the equations) and geometry (how lines or planes are arranged in space). The mechanics (x=A−1b) draw directly on the inverse-matrix lesson, and the classification draws on the determinant lesson. Expect questions that combine a computation with a "interpret your answer geometrically" demand.
A system of linear equations such as
a1x+b1y+c1za2x+b2y+c2za3x+b3y+c3z=d1=d2=d3is captured by the single matrix equation Ax=d, where
A=a1a2a3b1b2b3c1c2c3,x=xyz,d=d1d2d3.A is the coefficient matrix, x the vector of unknowns, and d the constants. The single equation Ax=d is exactly equivalent to the whole system — multiplying out Ax reproduces the three left-hand sides.
If det(A)=0, then A−1 exists and left-multiplying gives the unique solution
Ax=d⟹A−1Ax=A−1d⟹x=A−1d.
Solve 2x+y=5, 3x+2y=8.
Matrix form: (2312)(xy)=(58). Here detA=4−3=1, so A−1=(2−3−12) and
(xy)=(2−3−12)(58)=(10−8−15+16)=(21).So x=2, y=1. (Check in the original: 2(2)+1=5 ✓, 3(2)+2=8 ✓.)
Mark scheme: M1 write in matrix form and find detA=1; M1 correct A−1; M1 compute A−1d; A1 x=2,y=1. A substitution check is good practice and protects the final mark.
Solve x+y+z=6, x−y+z=2, 2x+y−z=1.
Coefficient matrix A=1121−1111−1. Expanding along row 1,
detA=1−111−1−1121−1+112−11=1(0)−1(−3)+1(3)=6=0,so there is a unique solution. Rather than invert the whole matrix, eliminate: subtracting equation (2) from equation (1) gives 2y=4, so y=2. Then (1) becomes x+z=4 and (3) becomes 2x−z=1−y=−1; adding these, 3x=3, so x=1 and z=3.
Thus x=1,y=2,z=3. (Check (2): 1−2+3=2 ✓; (3): 2+2−3=1 ✓.)
Mark scheme: M1 form the coefficient matrix and compute detA=6 (establishing a unique solution); M1 a valid elimination or inverse method; A1 two of the three values; A1 all three correct with a check. Either the inverse route or systematic elimination earns full marks; elimination is usually faster for a clean 3×3.
The value of detA tells you, before any solving, how many solutions to expect:
| Determinant | Number of solutions | Geometric meaning |
|---|---|---|
| detA=0 | exactly one (unique) | lines/planes meet at a single point |
| detA=0, consistent | infinitely many | lines coincide; planes meet in a line or sheet |
| detA=0, inconsistent | none | lines/planes are parallel or form a prism |
The key subtlety: detA=0 by itself does not decide between "infinitely many" and "none" — you must check consistency (whether the equations are compatible) to tell them apart. That extra step is exactly what the harder exam questions probe.
A special, always-consistent case is the homogeneous system Ax=0. It can never be inconsistent, because x=0 (the trivial solution) always works. So for a homogeneous system the only question is whether there are other solutions: if detA=0 the trivial solution is the unique one, while if detA=0 there are infinitely many (a line or plane of solutions through the origin). This "detA=0⟺ non-trivial solutions exist" principle is precisely what defines eigenvalues in lesson 8, where the homogeneous system is (A−λI)x=0.
Each equation ax+by+cz=d is a plane. The solution set is the intersection of the three planes, and there is a finite menu of configurations:
| Configuration | Description | Solutions | detA |
|---|---|---|---|
| Single point | three planes cross at one point | one | =0 |
| Sheaf (common line) | three planes share a common line | infinitely many (1 parameter) | 0, consistent |
| Coincident planes | two or more planes are identical | infinitely many | 0, consistent |
| Triangular prism | the three pairwise intersection lines are parallel but distinct | none | 0, inconsistent |
| Parallel planes | two or more planes are parallel and distinct | none | 0, inconsistent |
When detA=0 the only possibility is the single point. When detA=0 the planes are in "special position" and you decode which case by attempting to solve: a contradiction (e.g. 0=5) means inconsistent (prism or parallel, no solution); a free parameter means consistent (sheaf or coincident, infinitely many).
It helps to picture the two "no solution" cases distinctly. Parallel planes are the obvious one: like sheets of paper held apart, two (or three) planes with the same orientation but different positions never share a point. The triangular prism is subtler and a favourite of examiners: here no two planes are parallel — each pair meets in a line — but the three lines of intersection are themselves parallel to one another, so the three planes enclose an infinite triangular tube and have no point common to all three. The determinant is zero in both cases, and only by solving (reaching a contradiction) do you confirm there is no solution. Conversely the two "infinitely many" cases are the sheaf (three distinct planes pivoting about one shared line, like pages of an open book meeting at the spine) and coincident planes (literally the same plane written two or three ways).
graph TD
A["3×3 system A x = d"] --> B{"det A = 0 ?"}
B -->|"no"| C["Unique solution<br/>planes meet at a point"]
B -->|"yes"| D{"Consistent?"}
D -->|"yes"| E["Infinitely many<br/>sheaf / coincident planes"]
D -->|"no"| F["No solution<br/>prism / parallel planes"]
Solve x+y+z=6, 2x+2y+2z=12, x+y+z=6.
Here the second equation is exactly twice the first, and the third repeats the first: there is really only one independent equation, x+y+z=6. The coefficient matrix has three identical (up to scaling) rows, so detA=0. The system is consistent (the equations agree), so there are infinitely many solutions: choosing x and y freely as parameters, z=6−x−y. Geometrically, all three planes coincide.
Solve x+y=3, 2x+2y=7.
The second equation says x+y=3.5, contradicting the first (x+y=3). The coefficient matrix (1212) has det=0, and the system is inconsistent, so there is no solution. Geometrically, the two lines are parallel and distinct — they never meet.
These two examples are the heart of the topic: same detA=0, opposite conclusions, separated only by consistency. The lesson to carry into the exam is that a zero determinant is never the end of the analysis — it is the signal to switch from "apply the inverse" to "investigate the geometry", and the quality of your answer is judged on how clearly you then resolve which singular case you are in.
(Specimen-style — not a real past paper.) The system x+2y−z=1, 2x−y+3z=4, x+7y−6z=k is given. (a) Show that the coefficient matrix is singular. (b) Find the value of k for which the system is consistent, and describe the solution set geometrically. (7 marks)
Model solution. (a) det1212−17−13−6=1(6−21)−2(−12−3)+(−1)(14+1)=−15+30−15=0, so the matrix is singular.
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