Visual walkthrough — Partial fractions — linear, repeated, irreducible quadratic factors
Step 0 — What is a "rational function", and what are we allowed to touch?
We will trace one running example the whole way:
- — the top, degree .
- — the bottom, degree .
Because , this fraction is proper — the top is genuinely smaller than the bottom. Why we check this first: only proper fractions can be built purely from simple pieces; an oversized top would need a leftover polynomial (that is Polynomial long division, handled separately). Every step below assumes proper.
Step 1 — See the denominator "un-multiply" into factors
WHAT. We split the bottom into a product of the simplest possible factors: Here and are linear factors — each is just " minus a number". The numbers and are the roots: the -values that make the bottom zero (this is Factoring polynomials over the reals).
WHY. The denominator is a product. A product of two things is only zero when one of them is zero. So the whole fraction blows up ("explodes to infinity") at exactly two places: and . Those two explosion points are the fingerprints we will chase.
PICTURE. Below, the blue curve is . Notice the two vertical dashed walls — one yellow at , one red at — where the curve shoots off to infinity. Each wall is caused by one factor turning zero.

Step 2 — Guess the shape: one simple fraction per explosion
WHAT. We claim the fraction is a sum, one term per factor:
- — a piece that explodes only at (its own wall).
- — a piece that explodes only at .
- and — two unknown numbers ("how strong is each explosion") we must still find.
WHY this exact shape. Adding fractions is reversible. If someone added over a common denominator, they would land back on on the bottom. So going backwards, our fraction must have come from pieces with those very denominators. The top of each piece is a lone constant because each denominator is degree , and a proper piece needs a top of degree .
PICTURE. The blue curve (the full function) is drawn as the sum of the two coloured simple curves: the red one owns the wall, the yellow one owns the wall. Away from the walls they gently add up to the blue.

Recall
Why is the top of each simple piece just a constant (not )? ::: Each denominator has degree , so a proper piece needs a numerator of degree — a lone constant.
Step 3 — The cover-up trick, watched term by term
WHAT. To find , multiply both sides by the factor :
Look at each piece:
- Left: the cancelled the that was in the bottom, leaving .
- Right, term 1: — bare, no left.
- Right, term 2: — still carries a live .
WHY. We engineered the situation so that at the annoying -term is multiplied by and vanishes. That leaves alone:
PICTURE. The animation-frame shows the -term's contribution collapsing to zero as slides to (green curve pinched to the axis), while the surviving quantity (blue) is read off cleanly at the yellow dot.

Repeat, covering and setting :
Step 4 — Assemble and sanity-check the split
WHAT. With , :
WHY check. Two unknowns, two conditions — but let us verify by testing a safe point (far from both walls):
- Left: .
- Right: . ✓
PICTURE. Blue (original) and the coloured sum are drawn on the same axes; they lie exactly on top of each other everywhere except the two walls. The green vertical tie-line at shows both giving .

Step 5 — Integrate: why each simple wall becomes a logarithm
WHAT.
WHY log? The only function whose derivative is is — that is a standard integral. So a fraction that behaves like near its wall must integrate to a scaled log. This is the whole payoff: we traded one un-integrable mess for two instant logs.
PICTURE. Each coloured spike (top) sits above its own curve (bottom), with the vertical wall at becoming the point where the log dives to .

Step 6 — Edge case: what if the bottom doesn't split into linear walls?
WHAT. Suppose the bottom carries an irreducible quadratic like — one that has no real roots (its discriminant ). Then there is no real wall for it: the curve never explodes.
WHY it needs a linear top . With no real root to "cover up", we cannot isolate a single constant. The quadratic denominator has degree , so a proper piece over it needs a numerator of degree : . The part integrates to a log (via Integration by substitution, ); the leftover constant integrates to an arctan — the smooth "no-wall" swirl, another standard integral. See Completing the square for the general .
PICTURE. Contrast panel: left, with its real wall (→ log); right, , a smooth hump with no wall (→ arctan). Different geometry ⇒ different integral.

The one-picture summary

One messy blue curve, two explosion-walls → two coloured simple fractions found by cover-up → two logs when integrated. That is the entire machine.
Recall Feynman retelling — the whole walkthrough in plain words
I have one lumpy fraction. First I look at its bottom and factor it — every factor marks a spot where the graph shoots to infinity, a "wall". I guess that my lumpy fraction is really a sum, one baby fraction per wall, each baby exploding at only its own wall. To find how strong a baby is, I use the cover-up trick: I multiply through by that wall's factor so every other baby gets multiplied by something that goes to zero right at the wall — they all disappear, and the survivor hands me its number. I do this for each wall, glue the babies back together, and test one easy point to make sure they add to the original. Finally I integrate: each wall is just . If instead the bottom had a piece with no real wall (an irreducible quadratic), that piece keeps a linear top and integrates to a log plus a smooth arctan swirl instead. Walls → logs, no-walls → arctans. Done.