Partial Fractions
Splitting a complicated fraction into simple pieces sounds like an exam-only ritual, yet it is
exactly how engineers decode the behaviour of circuits, autopilots and camera stabilisers — and
how a computer integrates any rational function you hand it. The move behind all of that is
surprisingly homely.
You have spent years adding fractions: put them over a common denominator, combine,
tidy up. Partial fractions is that skill played backwards — un-adding. Watch
what happens when we add two utterly harmless fractions:
\frac{1/2}{x-1} - \frac{1/2}{x+1} \;=\; \frac{\tfrac12(x+1) - \tfrac12(x-1)}{(x-1)(x+1)} \;=\; \frac{1}{x^2-1}.
So \dfrac{1}{x^2-1} is secretly two simple fractions in a
trench coat. Why does a calculus course care? Because as written,
\displaystyle\int \frac{dx}{x^2-1} looks hopeless — it is not a
power, not a standard form, and no obvious
substitution
cracks it. But each piece integrates to a logarithm in one line:
\int \frac{dx}{x^2-1} = \frac{1}{2}\ln|x-1| - \frac{1}{2}\ln|x+1| + C = \frac{1}{2}\ln\left|\frac{x-1}{x+1}\right| + C.
That is the whole method in one sentence: factor the denominator, split the fraction
into its simple parts, integrate each part in one line. A single algebraic move
unlocks an entire family of integrals — every rational function
\dfrac{P(x)}{Q(x)} whose denominator factors becomes a sum of
pieces you already know how to integrate. The calculus here is trivial; the craft is in the
un-adding. This page is about that craft.
Worked example 1: \displaystyle\int \frac{dx}{(x-1)(x+2)}
Step 1 — write the decomposition with unknowns. Two distinct linear factors,
so two simple fractions:
\frac{1}{(x-1)(x+2)} = \frac{A}{x-1} + \frac{B}{x+2}.
Step 2 — clear the denominators. Multiply both sides by
(x-1)(x+2):
1 = A(x+2) + B(x-1).
This is an identity — it must hold for every
x, not just some solution. That single fact gives us two different
ways to hunt down A and B. Learn both:
one is fast, the other never lets you down.
Route 1 — substitute the roots (the cover-up idea)
Since the identity holds for every x, pick values that make terms
vanish. Setting x = 1 kills the B term
(x - 1 = 0):
1 = A(1 + 2) + B(0) = 3A \qquad\Longrightarrow\qquad A = \frac{1}{3}.
Setting x = -2 kills the A term:
1 = A(0) + B(-2 - 1) = -3B \qquad\Longrightarrow\qquad B = -\frac{1}{3}.
Route 2 — equate coefficients
Alternatively, expand the right side and gather powers of x:
1 = A(x+2) + B(x-1) = (A + B)\,x + (2A - B).
The left side is 0 \cdot x + 1. Two polynomials are identical only
if their coefficients match, power by power:
x^1:\;\; A + B = 0, \qquad x^0:\;\; 2A - B = 1.
Solve the pair: adding gives 3A = 1, so
A = \tfrac13 and B = -\tfrac13 — the
same answer, as it must be. Substituting roots is quicker when the factors are distinct and
linear; equating coefficients works for every shape of decomposition, and doubles as
a check on your arithmetic.
Finish — integrate each piece
\frac{1}{(x-1)(x+2)} = \frac{1/3}{x-1} - \frac{1/3}{x+2},
and each piece is a one-line logarithm (via u = x - 1 and
u = x + 2):
\int \frac{dx}{(x-1)(x+2)} = \frac{1}{3}\ln|x-1| - \frac{1}{3}\ln|x+2| + C = \frac{1}{3}\ln\left|\frac{x-1}{x+2}\right| + C.
The full-speed version of Route 1 is the cover-up method: to find the
constant over (x - r), put your finger over that factor in the
original fraction and evaluate everything left at x = r. For our
example, cover (x-1) and read off
A = \left.\frac{1}{\;x + 2\;}\right|_{x = 1} = \frac{1}{3}, \qquad B = \left.\frac{1}{\;x - 1\;}\right|_{x = -2} = -\frac{1}{3}.
No equations, no clearing denominators — done in your head. Why is this legal? Multiply the
identity \frac{1}{(x-1)(x+2)} = \frac{A}{x-1} + \frac{B}{x+2}
through by (x - 1) alone:
\frac{1}{x+2} = A + \frac{B(x-1)}{x+2}.
Now let x \to 1. The B term carries a
factor (x-1), so it dies, leaving exactly
A = \tfrac{1}{1+2}. "Covering up" the factor is just this
multiply-and-substitute compressed into one gesture.
The trick is often credited to Oliver Heaviside, the self-taught Victorian
engineer who used it to solve circuit equations at scandalous speed. When mathematicians
complained his shortcuts weren't rigorously justified, he shot back: "Shall I refuse my
dinner because I do not fully understand the process of digestion?" (One caution
before you feast: cover-up reads off the constant for a simple linear factor only —
for repeated or quadratic factors it gives you some of the constants, never all of them.)
The shapes of decomposition
Distinct linear factors are the easy case; two more shapes round out the method. The guiding
principle: each factor of the denominator contributes its own template of unknowns,
and the total number of unknowns always equals the degree of the denominator.
Write a proper rational function (degree of P below
degree of Q) as a sum of these building blocks, one per factor of
Q:
-
Distinct linear factor (x - r) contributes
\dfrac{A}{x - r}.
-
Repeated linear factor (x - r)^k contributes
one term per power,
\dfrac{A_1}{x - r} + \dfrac{A_2}{(x - r)^2} + \cdots + \dfrac{A_k}{(x - r)^k}.
-
Irreducible quadratic factor (x^2 + bx + c)
contributes \dfrac{Bx + C}{x^2 + bx + c} (a linear numerator).
The linear-factor pieces integrate to logarithms; the higher powers
\dfrac{A}{(x-r)^k} integrate by the power rule to
\dfrac{-A}{(k-1)(x-r)^{k-1}}; and the quadratic pieces split into a
logarithm plus an \arctan. Every proper rational function, without
exception, dissolves into these three kinds of one-line integrals — which is why partial
fractions is the closing move of the integration toolkit: it guarantees that every
rational function can be integrated in elementary terms.
Three traps swallow more exam marks than all the algebra combined:
-
Check the degrees FIRST. If the top's degree is
\ge the bottom's, the templates above simply do not apply —
no choice of constants can make \frac{A}{x-1}+\frac{B}{x+2}
(which shrinks to 0 for large x)
equal an improper fraction like \frac{x^2}{(x-1)(x+2)} (which
tends to 1). Do
polynomial division
first, then decompose the proper remainder. Worked example 3 below does exactly this.
-
Repeated factors need BOTH powers.
\dfrac{x+2}{(x-1)^2} needs
\dfrac{A}{x-1} + \dfrac{B}{(x-1)^2} — writing only
\dfrac{B}{(x-1)^2} loses a term, and writing
\dfrac{A}{x-1}+\dfrac{B}{x+1} invents a factor that isn't
there. One unknown per power, from 1 up to
k.
-
An irreducible quadratic gets Bx + C on top — not just
B. Over x^2+4 a constant
numerator is not general enough (count the unknowns: a degree-2 factor must carry 2 of
them). And don't try to split x^2+4 into linear factors — it
has no real roots, which is exactly what "irreducible" means.
Worked example 2: a repeated factor — \displaystyle\int \frac{x+2}{(x-1)^2}\,dx
The denominator is (x-1)^2: one linear factor, squared. The
template demands a term for each power:
\frac{x+2}{(x-1)^2} = \frac{A}{x-1} + \frac{B}{(x-1)^2}.
Multiply through by (x-1)^2:
x + 2 = A(x-1) + B.
Substituting the root x = 1 gives
3 = B — note that the root only reaches the highest power's
constant; that is why cover-up alone cannot finish a repeated-factor problem. For
A, equate the x-coefficients:
1 = A. So
\frac{x+2}{(x-1)^2} = \frac{1}{x-1} + \frac{3}{(x-1)^2}.
Now integrate: the first piece is a log, and the second is just the power rule in disguise
(3(x-1)^{-2} integrates to -3(x-1)^{-1}):
\int \frac{x+2}{(x-1)^2}\,dx = \ln|x-1| - \frac{3}{x-1} + C.
A quick sanity check never hurts: differentiate the answer —
\frac{1}{x-1} + \frac{3}{(x-1)^2} — and you are looking at the
decomposition again. The circle closes.
Worked example 3: an improper fraction — \displaystyle\int \frac{x^2}{(x-1)(x+2)}\,dx
Degree check first: the top has degree 2, the bottom has degree
2 — top \ge bottom, so this fraction is
improper and we must divide before we may decompose. Expanding the
denominator, (x-1)(x+2) = x^2 + x - 2, and dividing:
\frac{x^2}{x^2 + x - 2} = 1 + \frac{2 - x}{x^2 + x - 2} = 1 + \frac{2 - x}{(x-1)(x+2)}.
The polynomial part 1 integrates trivially; the remainder is now
proper (degree 1 over degree 2), so the
templates apply. Cover-up on
\dfrac{2-x}{(x-1)(x+2)} = \dfrac{A}{x-1} + \dfrac{B}{x+2}:
A = \left.\frac{2-x}{\;x+2\;}\right|_{x=1} = \frac{1}{3}, \qquad B = \left.\frac{2-x}{\;x-1\;}\right|_{x=-2} = \frac{4}{-3} = -\frac{4}{3}.
(Check by coefficients: A + B = \tfrac13 - \tfrac43 = -1 matches
the -x, and 2A - B = \tfrac23 + \tfrac43 = 2
matches the constant. It works.) Assemble and integrate term by term:
\int \frac{x^2}{(x-1)(x+2)}\,dx = \int \left( 1 + \frac{1/3}{x-1} - \frac{4/3}{x+2} \right) dx = x + \frac{1}{3}\ln|x-1| - \frac{4}{3}\ln|x+2| + C.
Three moves — divide, decompose, integrate — and a fraction that offered no way in has become
a polynomial plus two logarithms.
See it: a rational function and its antiderivative
The faint curve is the integrand \dfrac{1}{(x-1)(x-s)}, blowing up
at its two vertical asymptotes x = 1 and
x = s. The bold curve is the antiderivative that partial fractions
hands us,
\dfrac{1}{1-s}\big(\ln|x-1| - \ln|x-s|\big) — cover-up gives
A = \tfrac{1}{1-s} and B = -\tfrac{1}{1-s},
so the two log coefficients are always equal and opposite.
Slide the right root s and watch the pair respond. Two things are
worth spotting. First, the antiderivative has its own vertical asymptotes at the very same
places — where the integrand blows up, its accumulated area blows up too, so
\ln|x-r| plunges to -\infty at each
root. Second, drag s down towards 1:
the coefficient \tfrac{1}{1-s} grows without bound as the two
roots close in on each other. The distinct-roots formula is tearing itself apart — a preview
of why a repeated root demands the different template
\tfrac{A}{x-r} + \tfrac{B}{(x-r)^2} you met in worked example 2.
Partial fractions might look like an exam-only ritual, but it is quietly running inside
every control system you have ever trusted — autopilots, cruise control, the stabiliser
in your phone's camera. The reason is the Laplace transform: engineers
convert a differential equation describing a circuit or a robot arm into an algebraic
equation in a new variable s. Solving that is easy — but the
answer comes out as a rational function like
F(s) = \frac{s + 3}{(s+1)(s+2)},
and to translate it back into the real world (a voltage over time, a wing's response to a
gust) you must first split it into partial fractions:
\frac{2}{s+1} - \frac{1}{s+2}. Each simple piece
\frac{A}{s+a} converts back to a term
A e^{-at} — a decaying exponential. The roots of the denominator
(the "poles") literally tell the engineer whether the system settles smoothly, rings like a
bell, or shakes itself to pieces. The same un-adding also powers the standard trick for
summing series by telescoping, and it is how computer algebra systems integrate every
rational function you throw at them. Not bad for reversed fraction addition.
The method is genuinely old: Johann Bernoulli and
Gottfried Leibniz worked it out around 1700, precisely because they wanted
to integrate rational functions. Leibniz briefly worried that fractions like
\tfrac{1}{x^4+1} might not split over the reals — the
denominator has no real roots, and he suspected no real factorisation existed. Bernoulli
disagreed, and Bernoulli was right:
x^4 + 1 = (x^2 + \sqrt{2}\,x + 1)(x^2 - \sqrt{2}\,x + 1). In
fact every real polynomial factors into real linear and quadratic pieces — a consequence of
the fundamental theorem of algebra, proved rigorously a century later by Gauss. That
theorem is the quiet guarantee behind this whole page: the three templates in the box above
are always enough.
See it explained