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CorePure2 Chapter 6 :: Hyperbolic Functions
Last modified: 12th August 2018
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Overview We will see the definition and purpose of hyperbolic functions such as sinh π₯ , cosh π₯ , their inverses, and how we can manipulate them, such as solving equations, differentiating and integrating. 1 :: Definition of hyperbolic functions and their sketches. 2 :: Inverse hyperbolic functions. βFind the exact value of: π‘ππβ ππ 4 β Prove that πππππ β π₯= ln π₯+ π₯ 2 β1 3 :: Hyperbolic Identities and Solving Equations 4 :: Differentiation Determine π ππ₯ πππ ππβ π₯ Solve for all real π₯ 2 cosh 2 π₯ β 5π ππβ π₯ =5 Teacher Note: This is pretty much all of the old FP3 Chapter 1 (Hyperbolic Functions), much of Chapter 3 (Differentiation) and much of Chapter 4 (Integration). In particular, Exercise 6E (integration) is extremely hefty, so you may wish to split over 2 lessons. The change to integration since FP3 is that some results, e.g sech 2 π₯ ππ₯ have been dropped. 5 :: Integration Determine π₯+2 π₯ 2 ππ₯
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Conic Sections The axis of the parabola is parallel to the side of the cone. In mathematics there are a number of different families of curves. These doing FP1 as their Further Maths option will encounter ellipses, parabolas and hyperbolas in Chapters 2 and Chapter 3 (βConic Sections I and IIβ). Each of these have different properties and their equations have different forms. It is possible to obtain these different types of curves by slicing a cone, hence βconic sectionsβ.
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Comparing circles and hyperbolas
! (Donβt make notes on this slide) You will cover Hyperbolas in FP1, but this will give some context for the eponymously named βhyperbolic functionsβ that we will explore in this chapter. Circles Hyperbolas Source: Wikipedia 1 π₯,π¦ π 1 The βsimplestβ circle is a unit circle centred at the origin. Cartesian equation: π π + π π =π Parametric eqns (in terms of π): π=πππ π½ π=πππ π½ The equivalent hyperbola (which crosses π-axis at (π,π) and βπ,π ) Cartesian equation: π π β π π =π Parametric equations: π=ππππ π½ π=ππππ π½ ? similar ? ? ? similar
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Whatβs the point of hyperbolic functions?
Hyperbolic functions often result from differential equations (e.g. in mechanics), and weβll see later in this module how we can use these functions in calculus. For example, we can consider forces acting on each point on a hanging piece of string. Solving the relevant differential equations, we end up with: π= ππ¨π¬π‘ π ? OMG modelling!
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Equations for hyperbolic functions
Hyperbolic sine: sinh π₯ = π π₯ β π βπ₯ π₯ββ Hyperbolic cosine: cosh π₯ = π π₯ + π βπ₯ π₯ββ Hyperbolic tangent: tanh = sinh π₯ cosh π₯ = π 2π₯ β1 π 2π₯ π₯ββ Hyperbolic secant: sech π₯ = 1 cosh π₯ = 2 π π₯ + π βπ₯ π₯ββ Hyperbolic cosecant: cosech π₯ = 1 sinh π₯ = 2 π π₯ β π βπ₯ π₯ββ, π₯β 0 Hyperbolic cotangent: coth π₯ = 1 tanh π₯ = π 2π₯ +1 π 2π₯ β π₯ββ, π₯β 0 ? Say as βshineβ of π₯ ? Say as βcoshβ Say as βtanchβ ? ? Say as βsetchβ ? ? ? ? Say as βcosetchβ ? ? Say as βcothβ
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Equations for hyperbolic functions
Calculate (using both your π ππβ button and using the formula) π¬π’π§π‘ π =ππ.ππ Write in terms of π: ππ¨π¬πππ‘ π = π π¬π’π§π‘ π = π π π β π βπ = π ππππ βπ π ππππ +π = π ππ π π βπ π ππ π π +π = ππβπ ππ+π = ππ ππ Solve π ππβ π₯=5 π π β π βπ π =π β π π β π βπ =ππ π ππ βππ π π βπ=π π π = ππΒ± πππ+π π =ππ.πππ ππ βπ.πππ π=π.ππ ? Froculator Tip: Press the βhypβ button. Q ? Q ? Find the exact value of: ππππ ππ π Q ?
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Click here to sketch π¦= sinh π₯
Sketching hyperbolic functions π¦ π¦ π¦= π π₯ π¦= π βπ₯ π₯ π₯ π¦=β π π₯ π¦=β π βπ₯ sinhβ‘(π₯) is known as an odd function because π βπ₯ =βπ(π₯). Can you think of other odd functions? π π = π¬π’π§ π , π π = π π π¦ ? We can see we have the average of π π₯ and β π βπ₯ π¦= sinh π₯ Click here to sketch π¦= sinh π₯ π₯ As π₯ββ, π βπ₯ β0 β΄ sinh π₯ β 1 2 π π₯ ? sinh π₯ = π π₯ β π βπ₯ 2 ?
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Click here to sketch π¦= cosh π₯
Sketching hyperbolic functions π¦ π¦ π¦= π π₯ π¦= π βπ₯ π₯ π₯ π¦=β π π₯ π¦=β π βπ₯ coshβ‘(π₯) is known as an even function because π βπ₯ =π(π₯). Can you think of other even functions? π π = ππ¨π¬ π , π π = π π π¦ ? π¦= cosh π₯ Click here to sketch π¦= cosh π₯ π₯ As π₯ββ, cosh π₯ β 1 2 π π₯ ? cosh π₯ = π π₯ + π βπ₯ 2
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Click to sketch π¦= tanh π₯
Sketching hyperbolic functions tanh π₯ = sinh π₯ cosh π₯ To sketch π¦=tanh π₯ , consider the usual features when you sketch a graph. When π₯=0, π= π¬π’π§π‘ π ππ¨π¬π‘ π = π π =π As π₯ββ, πππ§π‘ π β π π π π π π π π =π As π₯βββ, πππ§π‘ π β β π π π βπ π π π βπ =βπ ? ? ? π¦ π¦=1 Click to sketch π¦= tanh π₯ π₯ π¦=β1
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Test Your Understanding
Sketch the graph of π¦= sech π₯ π₯ π¦= cosh π₯ 1 ? π₯ π¦ 1 π¦= sech π₯ ? We simply consider the reciprocal of each of the π¦ values.
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Exercise 6A Pearson Core Pure Year 2 Pages
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Inverse Hyperbolic Functions
As you might expect, each hyperbolic function has an inverse. Note that lack of βcβ (e.g. arsinh not arcsinh). π¦ Click to sketch π¦= sinh π₯ π₯ Click to sketch π¦= arsinh π₯ All of them: π=ππππππ π, π=ππππππ π, π=ππππππ π π=ππππππ π, π=ππππππππ π, π=ππππππ π
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Inverse Hyperbolic Functions
Why is there a problem when finding the inverse of π π₯ = cosh π₯ ? π¦ Recall from Pure Year 2 that functions only have an inverse if they are one-to-one. π π₯ = cosh π₯ is many-to-one if the domain is unrestricted, which would become one-to-many. x π¦=πππ β π₯ π¦=πππππ β π₯ π₯ If we restrict the domain to π₯β₯0, then it becomes one-to-one, and we can reflect in π¦=π₯ as before.
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Inverse Hyperbolic Functions
Given that hyperbolic functions can be written in terms of π, naturally (obscure pun intended) inverse hyperbolic can be expressed in terms of ππ. Prove that πππ ππβ π₯= ln π₯+ π₯ 2 +1 ? π=ππππππ π π= π¬π’π§π‘ π π= π π β π βπ π π π β π βπ =ππ π ππ βππ π π βπ=π π=βπ, π=βππ, π=βπ π π = ππΒ± π π π +π π =πΒ± π π +π However since π π +π >π, can only use positive case as π π is positive. π= π₯π§ π+ π π +π ππππππ π= π₯π§ π+ π π +π ? ?
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Test Your Understanding
Prove that πππππ β π₯= ln π₯+ π₯ 2 β1 , π₯β₯1 Proof that ππβ‘(πβ π π βπ ) is negative: π₯β π₯ 2 β1 π₯+ π₯ 2 β1 =1 π₯β π₯ 2 β1 = 1 π₯+ π₯ 2 β1 Taking logs of both sides: ln π₯β π₯ 2 β1 =β ln π₯+ π₯ 2 β1 Since π₯β₯1, π₯+ π₯ 2 β1 β₯1, thus RHS is negative. ? π=ππππππ π π= ππ¨π¬π‘ π π= π π + π βπ π π π + π βπ =ππ π ππ βππ π π +π=π π=βπ, π=βππ, π=+π π π = ππΒ± π π π βπ π =πΒ± π π βπ However this time, both + and β cases are possible. We can prove that lnβ‘(π₯β π₯ 2 β1 ) gives a negative value. Show > But recall from the graph that we only include positive values of π¦ in the function to avoid it being one-to-many. Thus πππππ β π₯= ln π₯+ π₯ 2 β1 only. π¦=πππππ β π₯
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Summary so Far πππ ππβ π₯= ln π₯+ π₯ πππππ β π₯= ln π₯+ π₯ 2 β1 , π₯β₯1 πππ‘ππβ π₯= 1 2 ln 1+π₯ 1βπ₯ , π₯ <1 Hyperbolic Domain Sketch Inverse Hyperbolic π¦= sinh π₯ π₯ββ π¦=πππ ππβ π₯ π¦= cosh π₯ π₯β₯0 π¦=πππππ β π₯ π₯β₯1 π¦= tanh π₯ π¦=πππ‘ππβ π₯ π₯ <1 π¦= sech π₯ π¦=πππ ππβ π₯ 0<π₯β€1 π¦=πππ ππβ π₯ π₯β 0 π¦=πππππ ππβ π₯ π¦= coth π₯ π¦= arcoth π₯ π₯ >1 ? ? ? ? 1 1 ? 1 ? -1 ? ? 1 ? ? ? ? 1 -1
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Exercise 6B Pearson Core Pure Year 2 Pages
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Hyperbolic Identities
From Pure Year 1 we know that sin 2 π₯ + cos 2 π₯ =1. Are there similar identities for hyperbolic functions? Use the definitions of π ππβ and πππ β to prove thatβ¦ ? ππ¨π¬π‘ π π β π¬π’π§π‘ π π =π ? πππ π π π=πβπππ π π π ? πππππ π π π=πππ π π πβπ
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Hyperbolic Identities
We can similar prove that: Similar to sinβ‘(π΄+π΅) identity. ππππ π¨Β±π© =ππππ π¨ ππππ π©Β±ππππ π¨ ππππ π© ππππ π¨Β±π© =ππππ π¨ ππππ π©Β±ππππ π¨ ππππ π© However this is Β± not β, unlike in cosβ‘(π΄+π΅) Prove that: ππππ π¨Β±π© = ππππ π ππππ π = ππππ π¨+ππππ π© π+ππππ π¨ ππππ π© Notice this is + rather than - .
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Osbornβs Rule We can get these identities from the normal sin/cos ones by: Osbornβs Rule: Replacing π ππβπ ππβ and πππ βπππ β Negate any explicit or implied product of two sines. sin π΄ sin π΅ ββ sinh π΄ sinh π΅ tan 2 π΄ ββ tanh 2 π΄ ? ? Since tan 2 π΄ = sin 2 π΄ cos 2 π΄ ? πππ 2π΄=2 cos 2 π΄ β1 β ππ¨π¬π‘ ππ¨ =πππ¨π¬ π π π¨βπ tan π΄βπ΅ = tan π΄ β tan π΅ 1+ tan π΄ tan π΅ β πππ§π‘ π¨ β πππ§π‘ π© πβ πππ§π‘ π¨ πππ§π‘ π© ?
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Solving Equations Either use hyperbolic identities or basic definitions of hyperbolic functions. Solve for all real π₯ 6 sinh π₯ β2 cosh π₯ =7 Solve for all real π₯ 2 cosh 2 π₯ β 5π ππβ π₯ =5 ? ? Using cosh 2 π₯ βsin β 2 π₯=1 2 1+ sinh 2 π₯ β5 sinh π₯ =5 2 sinh π₯ +1 sinh π₯ β3 =0 sinh π₯ =β 1 2 , sinh π₯ =3 π₯=πππ ππβ β 1 2 , π₯=πππ ππβ 3 π₯= ln β , π₯= ln 6 π π₯ β π βπ₯ 2 β2 π π₯ + π βπ₯ 2 =7 β¦ 2 π π₯ +1 π π₯ β4 =0 π₯= ln 4
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Further Examples Pure Year 1 one: If cos π₯ = 3 5 , find sin π₯ . ? sin 2 π₯ + cos 2 π₯ =1 sin π₯ = 1β = 4 5 ? If sinh π₯ = 3 4 , find the exact value of: cosh π₯ tanh π₯ sinh 2π₯ cosh 2 π₯ β sinh 2 π₯ =1 cosh π₯ = = tanh π₯ = sinh π₯ cosh π₯ = sinh 2π₯ =2 sinh π₯ cosh π₯ = 15 8 ? ?
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Test Your Understanding
? ?
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Exercise 6C Pearson Core Pure Year 2 Pages ?
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Differentiating hyperbolic functions
π ππ₯ sinh π₯ = cosh π₯ π ππ₯ cosh π₯ = sinh π₯ π ππ₯ tanh π₯ = sech 2 π₯ π ππ₯ coth π₯ =βπππ ππ β 2 π₯ Important Memorisation Tip: Theyβre all the same as non-hyperbolic results, other than that πππ β is not negated and sech π₯ becomes β sech π₯ tanβ π₯ (i.e. is negated). Prove that π ππ₯ sinh π₯ = cosh π₯ ? sinh π₯ = π π₯ β π βπ₯ 2 π ππ₯ sinh π₯ = π π₯ + π βπ₯ 2 = cosh π₯
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Test Your Understanding
Hint: Did someone say chain rule? ?
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Inverse Hyperbolic Functions
Proof π ππ₯ arsinh π₯ = 1 π₯ π ππ₯ arcosh π₯ = 1 π₯ 2 β1 π ππ₯ artanh π₯ = 1 1β π₯ 2 π¦=πππ ππβ π₯ sinh π¦ =π₯ ππ₯ ππ¦ = cosh π¦ ππ₯ ππ¦ = sinh 2 π¦ = π₯ ππ¦ ππ₯ = 1 π₯ 2 +1 ? ? ? ? Examples Given that π¦= πππππ β π₯ 2 prove that π₯ 2 β1 ππ¦ ππ₯ 2 =4π¦ Find π ππ₯ πππ‘ππβ 3π₯ By chain rule: π
π
π ππππππ ππ = π πβ ππ π Γπ = π πβπ π π π
π π
π =π ππππππ π π π π βπ π π βπ π
π π
π =π ππππππ π π π βπ π
π π
π π =π ππππππ π π π π βπ π
π π
π π =ππ ? ?
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Test Yarrr Understanding
? ? ?
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Using Maclaurin expansions for approximations
[Textbook] (a) Show that π ππ₯ πππ ππβ π₯ = π₯ [We did this earlier] (b) Find the first two non-zero terms of the series expansion of πππ ππβ π₯. The general form for the series expansion of πππ ππβ π₯ is given by πππ ππβ π₯= π=0 β β1 π 2π ! 2 2π π! π₯ 2π+1 2π+1 (c) Find, in simplest terms, the coefficient of π₯ 5 . (d) Use your approximation up to and including the term in π₯ 5 to find an approximate value for πππ ππβ 0.5. (e) Calculate the percentage error in using this approximation. b ? Need to use a Maclaurin expansion. π π₯ =πππ ππβ π₯ β π 0 =0 π β² π₯ = 1+ π₯ 2 β β π β² 0 =1 π β²β² π₯ =βπ₯ 1+ π₯ 2 β β π β²β² 0 =0 π β²β²β² π₯ = 2 π₯ 2 β π₯ β π β²β²β² 0 =β1 Maclaurin expansion: π π₯ =π 0 + π β² 0 1! π₯+ π β²β² 0 2! π₯ 2 + π β²β²β² 0 3! π₯ 3 +β¦ β΄πππ ππβ π₯βπ₯β π₯ 3 3! =π₯β 1 6 π₯ 3 π₯ 5 term will occur when π=2 β β1 2 4! ! π₯ 5 5 = π₯ 5 Coefficient is 3 40 d ? πππ ππβ 0.5β0.5β = % error = βπππ ππβ 0.5 πππ ππβ 0.5 Γ100 =0.062% (3dp) Need to keep going until we have two non-zero terms for the Maclaurin expansion. e ? c ?
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Exercise 6D Pearson Core Pure Year 2 Pages
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Standard Integrals Same as non-hyperbolic version? sinh π₯ ππ₯ = cosh π₯ +πΆ cosh π₯ ππ₯ = sinh π₯ +πΆ sech 2 π₯ ππ₯ = tanh π₯ +πΆ cosech 2 π₯ ππ₯ = βcoth π₯ +πΆ sech π₯ tanh π₯ ππ₯ = β sech π₯ +πΆ cosech π₯ coth π₯ ππ₯ = βcosech π₯ +πΆ β π₯ 2 ππ₯ = arcsin π₯ +πΆ, π₯ < π₯ 2 ππ₯ = arctan π₯ +πΆ π₯ 2 ππ₯ = arcsinβ π₯ +πΆ π₯ 2 β1 ππ₯ = arccosh π₯ +πΆ, π₯>1 ? ο» ? οΌ ? οΌ Not in this chapter but worth briefly mentioning. ? οΌ Not in formula booklet. ? ο» οΌ ? ? Was covered in Chapter 3. ? ? ?
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Click only if youβve forgotten them.
Quickfire Examples β Do From Memory! Recall that: π β² ππ+π π
π = π π π ππ+π +πͺ e.g. π 3π₯+2 ππ₯ = 1 3 π 3π₯+2 cosh 4π₯β1 ππ₯ = π π π¬π’π§π‘ ππβπ +πͺ π ππβ π₯ ππ₯= π π ππ¨π¬π‘ π π π +πͺ π₯ 2 ππ₯ =π ππππππ π π₯ 2 β1 ππ₯ =π ππππππ π π ππβ 3π₯ ππ₯= π π ππ¨π¬π‘ ππ +πͺ π₯ 2 β1 ππ₯ =ππ ππππππ π π₯ 2 ππ₯ =π ππππππ π ? ? ? ? ? ? Click only if youβve forgotten them. sinh π₯ ππ₯ = cosh π₯ +πΆ cosh π₯ ππ₯ = sinh π₯ +πΆ β π₯ 2 ππ₯ = arcsin π₯ +πΆ, π₯ < π₯ 2 ππ₯ = arctan π₯ +πΆ π₯ 2 ππ₯ = arcsinβ π₯ +πΆ π₯ 2 β1 ππ₯ = arccosh π₯ +πΆ, π₯>1 ? ?
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Further Example ? [Textbook] 2+5π₯ π₯ 2 +1 ππ₯
Integration Strategy Recap: If multiple terms in numerator, split fraction. 2+5π₯ π₯ ππ₯ = π₯ ππ₯ π₯ π₯ ππ₯ = π₯ ππ₯ + 5π₯ π₯ ππ₯ =2 πππ ππβ π₯ π₯ 2 +π sinh π₯ ππ₯ = cosh π₯ +πΆ cosh π₯ ππ₯ = sinh π₯ +πΆ π₯ 2 ππ₯ = arcsinβ π₯ +πΆ π₯ 2 β1 ππ₯ = arccosh π₯ +πΆ, π₯>1
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Integrating when not quite so standard
cosh 5 2π₯ sinh 2π₯ ππ₯ In the past weβve integrated expressions of the form sin π π₯ cos π₯ ππ₯ and cos π π₯ sin π₯ ππ₯ by the βconsider and scaleβ method. (Using Method 1) Try π= ππ¨π¬π‘ π ππ π
π π
π =π ππ¨π¬π‘ π ππ Γπππππ ππ =ππ ππ¨π¬π‘ π ππ ππππ ππ β΄ ππππ π ππ ππππ ππ π
π = π ππ ππ¨π¬π‘ π ππ +πͺ ? tanh π₯ ππ₯ ? = sinh π₯ cosh π₯ ππ₯ = ln cosh π₯ +πΆ Use the same method for integrating tan π₯ , i.e. expressing first as a division. Note that because πππ β differentiates to positive π ππβ, unlike the non-hyperbolic version, we donβt have the minus.
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Using Identities ? ? cosh 2 3π₯ ππ₯
Use double angle formulae for cos 2π΄ = cosh 6π₯ ππ₯ = 1 2 π₯ sinh 6π₯ +πΆ sinh 3 π₯ ππ₯ ? = sinh 2 π₯ sinh π₯ ππ₯ = cosh 2 π₯ β1 sinh π₯ ππ₯ = cosh 2 π₯ sinh π₯ β sinh π₯ ππ₯ = cosh 3 π₯ β cosh π₯ +πΆ Use this approach in general for small odd powers of sinh and cosh.
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When that doesnβt workβ¦
Sometimes there are techniques which work on non-hyperbolic trig functions but doesnβt work on hyperbolic ones. Just first replace any hyperbolic functions with their definition. Find π 2π₯ sinh π₯ ππ₯ Find sech π₯ ππ₯ ? ? π 2π₯ sinh π₯ ππ₯ = π 2π₯ π π₯ β π βπ₯ 2 = π 3π₯ β π π₯ ππ₯ = π 3π₯ β3 π π₯ +πΆ = π π₯ + π βπ₯ ππ₯ = 2 π π₯ π 2π₯ +1 ππ₯ Use the substitution π’= π π₯ ππ’ ππ₯ = π π₯ β΄ππ’= π π₯ ππ₯ 2 π π₯ π 2π₯ +1 ππ₯= π’ 2 +1 ππ’ =2 arctan π’ +πΆ =2 arctan π π₯ +πΆ (Integration by parts DOES also work, but requires a significantly greater amount of working!) (Fro Exam Note: This very question appeared FP3(Old) June 2014, except involving definite integration)
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Dealing with 1/ π 2 + π₯ 2 , 1/ π₯ 2 β π 2 , β¦.
sin 2 π + cos 2 π =1 1+ tan 2 π = sec 2 π 1+ sinh 2 π’ = cosh 2 π’ Sensible substitution and why? 1 π 2 + π₯ 2 ππ₯ π₯=π sinh π’ tan wouldnβt work as well this time because the denominator would simplify to π sec π’ , but weβd be multiplying by π sec 2 π , meaning not all the secs would cancel. With sinh π’ the two cosh π’ βs obtained would fully cancel. ? 1 π₯ 2 β π 2 ππ₯ ? π₯=π cosh π’ Show that π₯ 2 β π 2 ππ₯ =πππππ β π₯ π +π ! 1 π 2 + π₯ 2 ππ₯ =πππ ππβ π₯ π +π 1 π₯ 2 β π 2 ππ₯ =πππππ β π₯ π +π, π₯>π ? Let π₯=π cosh π’ β ππ₯ ππ’ =π sinh π’ 1 π₯ 2 β π 2 ππ₯ = π 2 cosh 2 π’ β π 2 π sinh π’ ππ’ = 1 π π sinh π’ cosh 2 π’ β1 ππ’= sinh π’ sinh π’ ππ’ =π’+π=πππππ β π₯ π +π
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Dealing with 1/ π 2 + π₯ 2 , 1/ π₯ 2 β π 2 , β¦.
1 π 2 + π₯ 2 ππ₯ =πππ ππβ π₯ π +π 1 π₯ 2 β π 2 ππ₯ =πππππ β π₯ π +π, π₯>π πππ ππβ π₯= ln π₯+ π₯ πππππ β π₯= ln π₯+ π₯ 2 β1 , π₯β₯1 [Textbook] Show that π₯ 2 β16 ππ₯ = ln ? = πππππ β π₯ =πππππ β 2βπππππ β = ln β ln = ln β ln 2 = ln
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? Using a seemingly-sensible-but-turns-out-rather-nasty substitution
Harder Example sin 2 π + cos 2 π =1 1+ tan 2 π = sec 2 π 1+ sinh 2 π’ = cosh 2 π’ Show that π₯ 2 ππ₯ = 1 2 πππ ππβ π₯+ 1 2 π₯ 1+ π₯ 2 +πΆ. (Hint: Use a sensible substitution) ? Using a seemingly-sensible-but-turns-out-rather-nasty substitution Trying π₯=tanβ‘π: ππ₯ ππ = sec 2 π β ππ₯= sec 2 π ππ 1+ π₯ 2 ππ₯ = π πππ sec 2 π ππ Using integration by parts: π’=π πππ ππ£ ππ₯ = sec 2 π ππ’ ππ₯ =π πππ tan π π£=π‘πππ sec 3 π ππ = sec π tan π β sec π tan 2 π ππ+πΆ sec 3 π ππ = sec π tan π β sec π ( sec 2 πβ1) ππ +πΆ sec 3 π ππ = sec π tan π β sec 3 π + π πππ +πΆ sec 3 π ππ =π πππ tan π + ln sec π + tan π +πΆ sec 3 π ππ = 1 2 secπ tan π ln sec π + tan π +πΆβ² = 1 2 π₯ 1+ π₯ ln π₯ 2 +π₯ +πΆβ² = 1 2 π₯ 1+ π₯ πππ ππβ π₯+πΆβ² ? Using the other-possible-substitution-that-turns-out-much-more-pretty-yay Trying π₯= sinh π’ : ππ₯ ππ’ = cosh π’ β ππ₯= cosh π’ ππ’ 1+ π₯ 2 ππ₯ = cosh π’ Γ cosh π’ ππ’ = cosh 2 π’ ππ’ = cosh 2π’ ππ’ = 1 2 π’ sinh 2π’ +πΆ = 1 2 πππ ππβ π₯+ 1 2 π₯ 1+ π₯ 2 +πΆ
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Test Your Understanding So Far
Hint: You may want to factorise out first, as we did in Chapter 3. ? Using a hyperbolic substitution, evaluate π₯ π₯ ππ₯ ? ? Using π₯=3 sinh π’ yields
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Integrating by Completing the Square
Determine π₯ 2 β8π₯+8 ππ₯ By completing the square, we can then use one of the standard results. = π₯ 2 β8π₯+8 ππ₯ = π₯β4 2 β8 ππ₯ Let π’=π₯β4 β ππ’=ππ₯ = π’ 2 β8 ππ’ = ln π’β 8 π’ πΆ = ln π₯β4β2 2 π₯β πΆ ? This is not in the standard form yet, but a simple substitution would make it so. Standard results: (in formula booklet) 1 π 2 β π₯ 2 ππ₯ = arcsin π₯ π +πΆ, π₯ <π π 2 + π₯ 2 ππ₯ = 1 π arctan π₯ π +πΆ π 2 + π₯ 2 ππ₯ = arcsinβ π₯ π +πΆ π₯ 2 β π 2 ππ₯ = arccosh π₯ π +πΆ, π₯>π π 2 β π₯ 2 ππ₯ = 1 2π ln π+π₯ πβπ₯ +πΆ π₯ 2 β π 2 ππ₯ = 1 2π ln π₯βπ π₯+π +πΆ
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Further Example ? Determine 1 12π₯+2 π₯ 2 ππ₯
2 π₯ 2 +12π₯=2 π₯ 2 +6π₯ =2 π₯+3 2 β9 1 12π₯+2 π₯ 2 ππ₯ = π₯+3 2 β9 ππ₯ = π₯+3 2 β9 ππ₯ Let π’=π₯+3 β ππ’=ππ₯ = π’ 2 β9 ππ’ = πππππ β π’ 3 +πΆ = πππππ β π₯ πΆ Standard results: (in formula booklet) 1 π 2 β π₯ 2 ππ₯ = arcsin π₯ π +πΆ, π₯ <π π 2 + π₯ 2 ππ₯ = 1 π arctan π₯ π +πΆ π 2 + π₯ 2 ππ₯ = arcsinβ π₯ π +πΆ π₯ 2 β π 2 ππ₯ = arccosh π₯ π +πΆ, π₯>π π 2 β π₯ 2 ππ₯ = 1 2π ln π+π₯ πβπ₯ +πΆ π₯ 2 β π 2 ππ₯ = 1 2π ln π₯βπ π₯+π +πΆ
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Test Your Understanding
? b ? c
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Exercise 6E Pearson Core Pure Year 2 Pages 140-142
(If I was to pick one chapter where it was worth doing the Mixed Exercises [6F], it would be this one!)
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