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Questions on integration by substitution and by parts
The chain rule and the product rule each reverse into a method of integration. Substitution changes the variable until the integral matches a standard form, and the structure of the integrand determines which substitution to use; integration by parts replaces one integral by another, and it is how the integral of ln x is obtained.
15 original questions · 64 marks · the integration by substitution and by parts notes · Integration
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Jump to: Reverse chain patterns and substitution · Integration by parts
Reverse chain patterns and substitution
Find ∫2x(x2 + 1)3 dx by recognising a reverse chain pattern.
Worked solution and marking guidance
The bracket's derivative, 2x, is sitting alongside as a factor, so the integrand is exactly what the chain rule leaves behind. The integral is (x2 + 1)4/4 + c, the next power up divided by that power. M1 for the recognition, A1 for the answer including the constant.Find ∫2x/(x2 + 3) dx.
Worked solution and marking guidance
The numerator is exactly the derivative of the denominator, so the f′/f pattern applies and the integral is ln(x2 + 3) + c. M1 A1. No modulus signs are needed, since x2 + 3 is positive for every real x.Find ∫sin3 x cos x dx.
Worked solution and marking guidance
The integrand is a power of sin x multiplied by the derivative of sin x, so it is a reverse chain in sin x: raise the power by one and divide by the new power. The integral is (sin4 x)/4 + c. M1 for recognising cos x as the derivative of the function being raised to a power, A1 for the answer including the constant. No substitution is needed once the pattern is seen, and differentiating the answer by the chain rule returns 4 sin3 x cos x ÷ 4.Show that ∫tan x dx = −ln|cos x| + c, and hence write down ∫tan 4x dx.
Worked solution and marking guidance
Write tan x as sin x/cos x. The derivative of cos x is −sin x, so the numerator is minus the derivative of the denominator and the integrand is −f′/f with f = cos x. M1 for rewriting as sin x/cos x and identifying the f′/f pattern with its minus sign. An f′/f integrand integrates to ln|f|, so this one integrates to −ln|cos x| + c. A1 for the printed result. The same shape with an inner coefficient of 4 divides by 4: ∫tan 4x dx = −(ln|cos 4x|)/4 + c. B1 for that. The modulus is needed because cos x is negative on half of its cycle.Use the substitution u = x2 + 1 to find the exact value of ∫02 x(x2 + 1)3 dx.
Worked solution and marking guidance
From u = x2 + 1, du = 2x dx, so x dx = du/2. The limits convert as well: x = 0 gives u = 1 and x = 2 gives u = 5. The integral becomes ½∫15 u3 du = ½[u4/4] from 1 to 5 = (625 − 1)/8 = 78. M1 for du/dx, M1 for the substitution, A1 for the integral fully in u with converted limits, M1 for integrating, A1 for 78. Convert the limits with the substitution: carrying 0 and 2 into a u-integral gives (16 − 0)/8 = 2, which integrates the wrong range.Using a suitable substitution, find ∫x√(2x − 1) dx.
Worked solution and marking guidance
The awkward part is the root of a linear expression, so take that expression as u: u = 2x − 1. Then x = (u + 1)/2. M1 for the choice with x written in terms of u. Differentiating, du/dx = 2, so dx = du/2. M1 for dx. The integral becomes ∫ ((u + 1)/2) × u1/2 × (du/2) = ¼∫(u3/2 + u1/2) du, once the bracket is multiplied through by the root. A1 for the integral wholly in u with nothing in x left. Integrating the two powers gives ¼[(2/5)u5/2 + (2/3)u3/2] = u5/2/10 + u3/2/6. M1 for integrating both powers. Since the integral is indefinite there are no limits to convert, but the answer has to go back into x: (2x − 1)5/2/10 + (2x − 1)3/2/6 + c. A1 for the answer in x.A student tries to find ∫x ex² dx by parts, with u = x and dv/dx = ex², and cannot get past the first line. Explain why parts is the wrong method here, and find the integral.
Worked solution and marking guidance
Parts needs v, and v is ∫ex² dx. That integral is not any combination of the standard functions, so there is no v to write down and the first line of the formula cannot be completed. B1 for v being unavailable. Look at the integrand again instead. The derivative of x2 is 2x, and the factor sitting outside the exponential is x, which is half of it. B1 for x as half the derivative of the exponent. So the integrand is ½ × 2x ex², a reverse chain: something of the form f′(x)ef(x) integrates to ef(x). M1 for the reverse chain. The integral is ½ex² + c. A1 for the answer.Use the substitution u = 1 + √x to show that ∫14 1/(1 + √x) dx = 2 − 2 ln (3/2).
Worked solution and marking guidance
From u = 1 + √x, √x = u − 1 and so x = (u − 1)2, giving dx = 2(u − 1) du. The limits move too: x = 1 gives u = 2 and x = 4 gives u = 3. The integral becomes ∫23 2(u − 1)/u du = 2∫23 (1 − 1/u) du = 2[u − ln u] from 2 to 3 = 2[(3 − ln 3) − (2 − ln 2)] = 2[1 − ln (3/2)] = 2 − 2 ln (3/2), as required. M1 for x in terms of u, M1 for dx, A1 for the new limits, M1 for the integrand fully in u, M1 for integrating, A1 for the printed form.Use the substitution x = 2 sin θ to show that ∫02 √(4 − x2) dx = π, and explain how the value can be checked from the graph of y = √(4 − x2).
Worked solution and marking guidance
A root of a difference of two squares is what x = a sin θ is for, with a2 = 4 here, so a = 2. Differentiating, dx = 2 cos θ dθ. M1 for dx. Under the substitution 4 − x2 = 4 − 4 sin2θ = 4 cos2θ by the Pythagorean identity, so the root is 2 cos θ; θ runs over [0, π/2], where cos θ is not negative, so no modulus is needed. M1 for the root becoming 2 cos θ, with the sign settled. The limits move with the substitution: x = 0 gives sin θ = 0 and θ = 0, and x = 2 gives sin θ = 1 and θ = π/2. A1 for the new limits. The integral is now ∫0π/2 2 cos θ × 2 cos θ dθ = 4∫0π/2 cos2θ dθ, and cos2θ = ½ + ½ cos 2θ. M1 for the double-angle identity. So the value is 4[θ/2 + (sin 2θ)/4] from 0 to π/2 = 4(π/4 + 0) − 0 = π, as required. A1 for reaching π. For the check, y = √(4 − x2) is the upper half of the circle x2 + y2 = 4, so the region for 0 ≤ x ≤ 2 is a quarter of a disc of radius 2, of area ¼ × π × 22 = π. B1 for the quarter-circle check.
Integration by parts
Use integration by parts to find ∫xe2x dx.
Worked solution and marking guidance
Choose the factor that simplifies when differentiated, so u = x and dv/dx = e2x. Then ∫xe2x dx = (x/2)e2x − ∫(1/2)e2x dx = (x/2)e2x − e2x/4 + c. M1 for a correct application of the formula, A1 for the first stage, M1 for integrating the remaining term, A1 for the answer with its constant.Use integration by parts to find ∫x ln x dx.
Worked solution and marking guidance
Here the logarithm has to be the differentiated factor, because ∫ln x dx is not a standard result you can quote. Take u = ln x and dv/dx = x. Then ∫x ln x dx = (x2/2) ln x − ∫(x2/2)(1/x) dx = (x2/2) ln x − x2/4 + c. M1 for the choice and the formula, A1 for the first stage, M1 for simplifying x2/2 × 1/x to x/2, A1 for the answer.Find the exact value of ∫0π/2 x sin x dx.
Worked solution and marking guidance
Parts with u = x and dv/dx = sin x gives [−x cos x]0π/2 + ∫0π/2 cos x dx = [−x cos x + sin x] from 0 to π/2. At the upper limit that is −(π/2)(0) + 1 = 1, and at the lower limit it is 0 + 0 = 0, so the value is exactly 1. M1 for the parts, A1 for −x cos x + sin x, M1 for substituting the limits, A1 for 1. The boundary term vanishes at both ends for different reasons, cos (π/2) = 0 at the top and x = 0 at the bottom, and the two minus signs in −∫(−cos x) dx cancel.Find ∫ln x dx, and hence find the exact value of ∫1e ln x dx.
Worked solution and marking guidance
There is only one factor, so supply a second: write the integrand as ln x × 1, take u = ln x and dv/dx = 1, giving v = x. M1 for taking dv/dx = 1. Then ∫ln x dx = x ln x − ∫x × (1/x) dx = x ln x − ∫1 dx. A1 for that first stage. The remaining integral is x, so ∫ln x dx = x ln x − x + c. A1 for the antiderivative. Now the definite value. At x = e the bracket is e ln e − e = e − e = 0, and at x = 1 it is 1 × 0 − 1 = −1. M1 for substituting both limits, A1 for the two bracket values. The value is 0 − (−1) = 1. A1 for 1. Differentiating x ln x − x gives ln x + 1 − 1, which is the check.Find the exact value of ∫01 x2 ex dx, giving your answer in terms of e.
Worked solution and marking guidance
Parts with u = x2 and dv/dx = ex gives x2ex − 2∫x ex dx. The remaining integral needs parts a second time, giving ∫x ex dx = x ex − ex. So the antiderivative is x2ex − 2x ex + 2ex. At x = 1 that is e − 2e + 2e = e, and at x = 0 it is 0 − 0 + 2 = 2, so the value is e − 2. M1 for the first parts, A1 for the first stage, M1 for the second parts, A1 for the full antiderivative, A1 for e − 2. Each application drops the power on x by one, so a polynomial of degree n needs n rounds and the sign alternates as you go.Find ∫e2x sin x dx.
Worked solution and marking guidance
Neither factor simplifies when differentiated, so parts will not terminate; it comes back to where it started instead, and that is what makes the answer available. Write I for the integral. With u = sin x and dv/dx = e2x, so v = e2x/2, I = (e2x sin x)/2 − ½∫e2x cos x dx. M1 for the first application, A1 for that stage. Apply parts again to the new integral, with u = cos x and the same dv/dx: ∫e2x cos x dx = (e2x cos x)/2 + ½∫e2x sin x dx, the plus coming from the minus in the derivative of cos x meeting the minus in the formula. M1 for the second application, A1 for the second stage. The last integral is I again, so substituting gives I = (e2x sin x)/2 − (e2x cos x)/4 − I/4, and collecting, (5/4)I = e2x(2 sin x − cos x)/4. M1 for recognising I and solving for it. Hence I = e2x(2 sin x − cos x)/5 + c. A1 for the answer with its constant. Both applications must differentiate the trigonometric factor; swapping roles halfway undoes the first application and returns the identity I = I. The constant is added at the end, after the equation for I has been solved, and differentiating the answer by the product rule returns e2x sin x.
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