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Integration is where all the earlier hyperbolic work pays off. Reversing the derivatives of the previous lesson gives the direct integrals ∫coshxdx=sinhx+c and friends; reversing the inverse-derivatives produces three of the most important standard integrals in the course — ∫x2+a21dx=arsinhax+c and its relatives — which crack a whole class of integrals that have no elementary antiderivative in terms of polynomials and arctan alone. This lesson assembles the standard results, shows how the power-reduction identities handle sinh2 and cosh2, uses completing-the-square to extend the inverse-hyperbolic forms, and works the hyperbolic substitution x=asinht (the hyperbolic analogue of x=asinθ).
Hyperbolic integration is compulsory pure content for Papers 1 and 2 of AQA Further Mathematics (7367). Carrying out a standard integral or a stated substitution is AO1; choosing the right method (recognise a standard form, complete the square, or substitute) and interpreting the result is AO2/AO3. It is the direct continuation of the differentiation lesson — every standard integral here is a derivative from there reversed — and it builds on integration by substitution, definite integrals, and completing the square from A-Level Maths. Examiners love the inverse-hyperbolic integrals because they reward students who can recognise the structure x2±a2 and reach for the right standard form rather than flailing with a generic substitution. Beyond the pure papers, these integrals are the bread and butter of the further-calculus strand — arc lengths, surface areas of revolution and certain volumes all reduce to exactly the forms practised here — so the recognition skill earns marks well outside the immediate topic.
Reversing each standard derivative immediately gives:
∫coshxdx=sinhx+c,∫sinhxdx=coshx+c,∫sech2xdx=tanhx+c,
∫cosech2xdx=−cothx+c,∫sechxtanhxdx=−sechx+c,∫cosechxcothxdx=−cosechx+c.
The first two are pleasingly free of the minus sign that trips students in trig: ∫sinh=+cosh (whereas ∫sin=−cos). The reciprocal-squared and product integrals all do carry a minus, matching their negative derivatives. A quick way to reconstruct any of these under pressure is to think "what differentiates to give the integrand?" — the integral table is just the derivative table read right-to-left, with every entry verifiable on the spot by differentiating your proposed answer.
This "reverse the derivative" mindset is worth making explicit, because it means there is nothing new to memorise in this section beyond the previous lesson. If you can differentiate tanhx to get sech2x, then you automatically know ∫sech2xdx=tanhx+c; if you know dxdsechx=−sechxtanhx, then the slightly awkward integral ∫sechxtanhxdx is just −sechx+c. Whenever you meet an unfamiliar hyperbolic integrand, ask which standard function has that as its derivative; almost always the answer is staring back from the derivative table. The genuinely new skills in this lesson are the three things you cannot do by pure reversal: integrating even powers (power reduction, §3), recognising the inverse-hyperbolic forms (§4), and the substitution method (§6).
Evaluate ∫01coshxdx.
∫01coshxdx=[sinhx]01=sinh1−sinh0=2e−e−1≈1.175.
Mark scheme: M1 antiderivative sinhx; A1 apply limits; A1 exact form 2e−e−1 (a decimal alone, if an exact value is asked, would lose the final mark).
Just as ∫sin2x needs the double-angle identity, the even powers of sinh and cosh are integrated by first applying the power-reduction identities from the identities lesson:
sinh2x=2cosh2x−1,cosh2x=2cosh2x+1.
Integrating term by term (and using ∫cosh2x=21sinh2x):
∫sinh2xdx=4sinh2x−2x+c,∫cosh2xdx=4sinh2x+2x+c
The only difference between the two is the sign of the 2x term — minus for sinh2, plus for cosh2 — which you can anchor by noting that cosh2x≥sinh2x, so its integral should be the larger. The reason a naive attempt fails is instructive: you cannot integrate cosh2x as though it were a power of x (there is no "31cosh3x" rule, because the chain rule would demand an extra sinh factor that is not present). The power-reduction identity sidesteps this by trading the square for a linear combination of cosh2x and a constant, both of which integrate trivially. The same trick — convert a power into a multiple angle — is exactly how ∫sin2,∫cos2 are handled in A-Level Maths, so the method should feel familiar; only the identity changes. For higher even powers such as cosh4x you simply apply power reduction twice, and for odd powers such as sinh3x you peel off one factor and use the fundamental identity (e.g. sinh3x=sinhx(cosh2x−1), then substitute u=coshx).
Evaluate ∫0ln2sinh2xdx.
∫0ln2sinh2xdx=[4sinh2x−2x]0ln2.
Evaluate sinh(2ln2)=sinh(ln4)=2eln4−e−ln4=24−41=815. So
=41⋅815−2ln2−0=3215−2ln2.
Mark scheme: M1 use sinh2x=2cosh2x−1; A1 antiderivative 4sinh2x−2x; M1 evaluate sinh(ln4)=815 using the exponential definition; A1 3215−2ln2.
Reversing the inverse-hyperbolic derivatives gives the three high-value standard integrals:
∫x2+a21dx=arsinhax+c,∫x2−a21dx=arcoshax+c (x>a)
∫a2−x21dx=a1artanhax+c (∣x∣<a)
The decisive clue is the sign inside the surd: x2+a2 gives arsinh; x2−a2 gives arcosh; and a2−x2 (no surd) gives a1artanh. Contrast the inverse-trig forms ∫a2−x21=arcsinax and ∫a2+x21=a1arctanax: reading the ± pattern correctly is the whole skill.
It is worth laying out the complete decision table side by side, because all five quadratic-surd reciprocals appear interchangeably in exams and the only thing distinguishing them is the position and sign of the squares. With a surd in the denominator: a2−x2 (constant minus square) routes to arcsinax; x2+a2 (square plus constant) routes to arsinhax; x2−a2 (square minus constant) routes to arcoshax. Without a surd, with the squares in the denominator directly: a2+x2 routes to a1arctanax; a2−x2 routes to a1artanhax. Memorising this five-row map — and the mnemonic that "a plus under a surd is hyperbolic-sine, a minus under a surd is hyperbolic-cosine, a plus without a surd is arctan, a minus without a surd is artanh" — converts what feels like five separate results into one organised picture, and it is precisely the recognition examiners are probing. Most marks lost in this topic come from grabbing arcsin when an arsinh was wanted, simply because a sign was misread under time pressure.
Why are there two hyperbolic forms (arsinh and arcosh) but only one circular form (arcsin) for the surd cases? Because the circular world only has a2−x2 as a "nice" surd — the expression a2+x2 cannot be tamed by x=asinθ, since a2+a2sin2θ does not collapse. The hyperbolic identities, with their minus sign, are exactly what is needed to handle the + and the larger − cases, which is the whole reason hyperbolic functions earn a place in the integration toolkit.
Find ∫x2+161dx, giving the answer as a logarithm.
Here a=4:
∫x2+16dx=arsinh4x+c=ln(x+x2+16)+c.
Mark scheme: M1 recognise arsinh(x/a) with a=4; A1 arsinh(x/4)+c; A1 log form (note the additive constant absorbs the −lna that appears when converting).
Evaluate ∫513x2−251dx.
Here a=5, and the lower limit x=5=a is the edge of the domain (the integral is improper there but convergent):
∫513x2−25dx=[arcosh5x]513=arcosh513−arcosh1=ln(513+512)−0=ln5.
Mark scheme: M1 arcosh(x/5) form; M1 apply limits, noting arcosh1=0; A1 arcosh513=ln5 (since (13/5)2−1=512).
When the surd is a general quadratic ax2+bx+c, complete the square to turn it into one of the standard x′2±a′2 forms, then substitute the shift. This is the single most common "harder" integral in the topic, and the procedure is mechanical once you see it: complete the square to get (x+p)2±q2, let u=x+p so that du=dx, and the integral collapses to a bare standard form in u. The sign of the constant left after completing the square tells you which standard form you land in — +q2 means arsinh, −q2 means arcosh — and the shift u=x+p carries through to the final answer unchanged. Because du=dx (the shift has gradient 1), there is no awkward scaling to track; the only thing to be careful of is reading off q correctly and stating the domain when an arcosh appears.
Find ∫x2+6x+131dx.
Complete the square: x2+6x+13=(x+3)2+4. With u=x+3 (so du=dx) the integral becomes ∫u2+41du, an arsinh form with a=2:
∫x2+6x+13dx=arsinh2u+c=arsinh2x+3+c.
Mark scheme: M1 complete the square to (x+3)2+4; M1 substitute u=x+3; A1 arsinh2x+3+c. The +a2=+4 signals arsinh; had it been (x+3)2−4 the answer would be arcosh2x+3.
For surds that multiply the rest of the integrand (so recognition alone is not enough), use a hyperbolic substitution, the analogue of the trig substitution x=asinθ:
| Surd | Substitution | Result of the surd |
|---|---|---|
| x2+a2 | x=asinht | x2+a2=acosht |
| x2−a2 | x=acosht | x2−a2=asinht |
The magic is that the substitution makes the surd vanish: with x=asinht, x2+a2=a2sinh2t+a2=a2(sinh2t+1)=a2cosh2t, so x2+a2=acosht (positive, as cosh≥1). And dx=acoshtdt is also acosht, which usually cancels beautifully.
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