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Antiderivatives of exponential and trigonometric functions (TCE Mathematics Methods, Tasmania)

Syllabus dot point

“Find antiderivatives of exponential and trigonometric functions and apply them in definite integrals.”

8 min read

Quick answer

Reversing the derivatives gives the standard antiderivatives ∫ekx dx=1kekx+C\displaystyle\int e^{kx}\,dx = \tfrac{1}{k}e^{kx}+C, ∫sin⁡(kx) dx=−1kcos⁡(kx)+C\displaystyle\int \sin(kx)\,dx = -\tfrac{1}{k}\cos(kx)+C and ∫cos⁡(kx) dx=1ksin⁡(kx)+C\displaystyle\int \cos(kx)\,dx = \tfrac{1}{k}\sin(kx)+C. The reciprocal factor 1k\tfrac{1}{k} undoes the chain-rule factor that differentiation produced.

What this dot point is asking

Integration is antidifferentiation, so every derivative rule you learned in Unit 3 reverses into an integration rule. This dot point collects the antiderivatives of the exponential and trigonometric functions, completing the toolkit alongside the power and reciprocal rules.

Reversing each derivative

Because ddx(ekx)=kekx\dfrac{d}{dx}(e^{kx}) = ke^{kx}, integrating ekxe^{kx} must divide by kk to cancel that factor. The trigonometric antiderivatives follow the same logic, with the added care that integrating sine introduces a minus sign.

Standard antiderivatives

∫ekx dx=1kekx+C\displaystyle\int e^{kx}\,dx = \frac{1}{k}e^{kx} + C

∫sin⁡(kx) dx=−1kcos⁡(kx)+C\displaystyle\int \sin(kx)\,dx = -\frac{1}{k}\cos(kx) + C

∫cos⁡(kx) dx=1ksin⁡(kx)+C\displaystyle\int \cos(kx)\,dx = \frac{1}{k}\sin(kx) + C

Integration of sine and cosine swap roles with a sign

Differentiating, sin⁡\sin leads to cos⁡\cos and cos⁡\cos leads to −sin⁡-\sin. Integrating reverses this: the integral of cos⁡\cos is +sin⁡+\sin, and the integral of sin⁡\sin is −cos⁡-\cos. The minus sign lands on the antiderivative of sine, the opposite place from where it sat in differentiation.

Checking by differentiating back

The reliable way to confirm any antiderivative is to differentiate your answer and check you recover the original integrand. For instance, differentiating −13cos⁡(3x)-\tfrac{1}{3}\cos(3x) gives −13⋅(−3sin⁡(3x))=sin⁡(3x)-\tfrac{1}{3}\cdot(-3\sin(3x)) = \sin(3x), which confirms the antiderivative of sin⁡(3x)\sin(3x).

Worked example

A definite integral with exponential and trigonometric terms

Evaluate ∫0π/2(e2x+cos⁡x) dx\displaystyle\int_0^{\pi/2} \big(e^{2x} + \cos x\big)\,dx.

Step 1: Find the antiderivative of each term

Because the integrand is a sum, we antidifferentiate each term separately. For e2xe^{2x} the coefficient of xx is 22, so the antiderivative carries a reciprocal factor of 12\tfrac{1}{2}. For cos⁡x\cos x the antiderivative is sin⁡x\sin x:

∫(e2x+cos⁡x) dx=12e2x+sin⁡x+C.\int \big(e^{2x} + \cos x\big)\,dx = \frac{1}{2}e^{2x} + \sin x + C.

Step 2: Apply the fundamental theorem by substituting the limits

Evaluate the antiderivative at the upper limit x=π2x = \tfrac{\pi}{2} and subtract its value at the lower limit x=0x = 0:

[12e2x+sin⁡x]0π/2=(12eπ+sin⁡π2)−(12e0+sin⁡0).\left[\frac{1}{2}e^{2x} + \sin x\right]_0^{\pi/2} = \left(\frac{1}{2}e^{\pi} + \sin\frac{\pi}{2}\right) - \left(\frac{1}{2}e^{0} + \sin 0\right).

Step 3: Simplify using known values

Substitute the exact values sin⁡π2=1\sin\tfrac{\pi}{2} = 1, e0=1e^0 = 1 and sin⁡0=0\sin 0 = 0:

(12eπ+1)−(12+0)=12eπ+12.\left(\frac{1}{2}e^{\pi} + 1\right) - \left(\frac{1}{2} + 0\right) = \frac{1}{2}e^{\pi} + \frac{1}{2}.

Numerically eπ≈23.14e^{\pi} \approx 23.14, so the integral is about 12(23.14)+0.5≈12.07\tfrac{1}{2}(23.14) + 0.5 \approx 12.07.

Final answer: 12eπ+12\dfrac{1}{2}e^{\pi} + \dfrac{1}{2} (approximately 12.0712.07).

Linear inner functions

Each rule extends to a linear inner function kx+ckx + c, because the chain rule only contributes the constant factor kk. So

∫ekx+c dx=1kekx+c+C,∫sin⁡(kx+c) dx=−1kcos⁡(kx+c)+C,\int e^{kx + c}\,dx = \frac{1}{k}e^{kx + c} + C, \qquad \int \sin(kx + c)\,dx = -\frac{1}{k}\cos(kx + c) + C,

and similarly for cosine. The shift cc does not change the reciprocal factor; only the coefficient of xx matters. For example, ∫cos⁡(2x−1) dx=12sin⁡(2x−1)+C\displaystyle\int \cos(2x - 1)\,dx = \frac{1}{2}\sin(2x - 1) + C. This linear-substitution shortcut covers the large majority of TASC antidifferentiation questions, because the inner functions in the course are almost always linear.

A definite integral with a phase shift

Evaluate ∫0π/4sin⁡ ⁣(2x+π2) dx\displaystyle\int_{0}^{\pi/4} \sin\!\left(2x + \tfrac{\pi}{2}\right)\,dx.

Step 1: Find the antiderivative of the shifted sine

The inner function is 2x+π22x + \tfrac{\pi}{2}, a linear expression with coefficient k=2k = 2 on xx. The antiderivative of sin⁡(kx+c)\sin(kx + c) is −1kcos⁡(kx+c)-\tfrac{1}{k}\cos(kx + c); the phase shift π2\tfrac{\pi}{2} travels through unchanged into the antiderivative:

∫sin⁡ ⁣(2x+π2) dx=−12cos⁡ ⁣(2x+π2)+C.\int \sin\!\left(2x + \tfrac{\pi}{2}\right)\,dx = -\frac{1}{2}\cos\!\left(2x + \tfrac{\pi}{2}\right) + C.

Step 2: Apply the limits and evaluate

Substitute x=π4x = \tfrac{\pi}{4} and x=0x = 0 into the antiderivative and subtract. At x=π4x = \tfrac{\pi}{4} the argument becomes π2+π2=π\tfrac{\pi}{2} + \tfrac{\pi}{2} = \pi; at x=0x = 0 it becomes π2\tfrac{\pi}{2}:

[−12cos⁡ ⁣(2x+π2)]0π/4=−12cos⁡(π)+12cos⁡ ⁣(π2)=−12(−1)+12(0)=12.\left[-\frac{1}{2}\cos\!\left(2x + \tfrac{\pi}{2}\right)\right]_{0}^{\pi/4} = -\frac{1}{2}\cos(\pi) + \frac{1}{2}\cos\!\left(\tfrac{\pi}{2}\right) = -\frac{1}{2}(-1) + \frac{1}{2}(0) = \frac{1}{2}.

The phase shift π2\dfrac{\pi}{2} rides along untouched; only the factor 12\dfrac{1}{2} from k=2k = 2 enters the antiderivative.

Final answer: 12\dfrac{1}{2}.

Where these antiderivatives are used

These rules let you find areas under exponential and trigonometric curves, recover totals from exponential or oscillating rates of change, and compute the mean of a continuous random variable whose density involves e−kxe^{-kx}. They also combine with the area-between-curves method whenever one of the boundaries is an exponential or trigonometric graph.

Forgetting the reciprocal factor or misplacing the sign

Two slips dominate. Writing ∫e3x dx=e3x+C\displaystyle\int e^{3x}\,dx = e^{3x}+C omits the 13\tfrac{1}{3} factor; the correct result is 13e3x+C\tfrac{1}{3}e^{3x}+C. Writing ∫sin⁡x dx=cos⁡x+C\displaystyle\int \sin x\,dx = \cos x + C drops the minus; the correct result is −cos⁡x+C-\cos x + C. Differentiating your answer to recover the integrand catches both errors immediately.

Summary

Reverse each derivative: dividing by kk for ekxe^{kx} and for sin⁡(kx)\sin(kx) or cos⁡(kx)\cos(kx), and remembering that the integral of sine carries a minus sign while the integral of cosine does not. Always verify by differentiating back. With these antiderivatives added to the power and reciprocal rules, you can integrate any standard function in the course and apply it in definite integrals.

Exam-style questions

Questions in the style of TASC exam questions on this dot point, each with a worked answer. They are written by ExamExplained unless tagged "Past paper"; the year shows the paper a question is modelled on.

Practice4 marks
Calculator-free. Evaluate the following integrals: (a) ∫−cos⁡ ⁣(π3x) dx\displaystyle\int -\cos\!\left(\tfrac{\pi}{3}x\right)\,dx; (b) ∫1/21e2x−1 dx\displaystyle\int_{1/2}^{1} e^{2x - 1}\,dx.
Show worked answer →

(a) The antiderivative of cos⁡(kx)\cos(kx) is 1ksin⁡(kx)\dfrac{1}{k}\sin(kx). Here k=π3k = \dfrac{\pi}{3}, so 1k=3π\dfrac{1}{k} = \dfrac{3}{\pi}:

∫−cos⁡ ⁣(π3x) dx=−3πsin⁡ ⁣(π3x)+C.\int -\cos\!\left(\tfrac{\pi}{3}x\right)\,dx = -\frac{3}{\pi}\sin\!\left(\tfrac{\pi}{3}x\right) + C.

The reciprocal factor 3π\dfrac{3}{\pi} comes from reversing the chain rule.

(b) The antiderivative of e2x−1e^{2x - 1} is 12e2x−1\dfrac{1}{2}e^{2x - 1} (divide by the coefficient of xx).

[12e2x−1]1/21=12e1−12e0=12(e−1).\left[\tfrac{1}{2}e^{2x - 1}\right]_{1/2}^{1} = \tfrac{1}{2}e^{1} - \tfrac{1}{2}e^{0} = \tfrac{1}{2}(e - 1).

Marks reward the correct reciprocal factor in each case and the correct substitution of limits in (b).

Practice4 marks
Calculator-assumed. (a) Evaluate ∫2x−3 dx\displaystyle\int \sqrt{2x - 3}\,dx. (b) Evaluate ∫e5x+1e2x−3 dx\displaystyle\int \dfrac{e^{5x + 1}}{e^{2x - 3}}\,dx.
Show worked answer →

(a) Write 2x−3=(2x−3)1/2\sqrt{2x - 3} = (2x - 3)^{1/2}. Antidifferentiate using the rule for a linear inner function: raise the power, divide by the new power, then divide by the coefficient of xx (which is 22):

∫(2x−3)1/2 dx=12⋅23(2x−3)3/2+C=13(2x−3)3/2+C.\int (2x - 3)^{1/2}\,dx = \frac{1}{2}\cdot\frac{2}{3}(2x - 3)^{3/2} + C = \frac{1}{3}(2x - 3)^{3/2} + C.

(b) First simplify using index laws: e5x+1e2x−3=e(5x+1)−(2x−3)=e3x+4\dfrac{e^{5x + 1}}{e^{2x - 3}} = e^{(5x + 1) - (2x - 3)} = e^{3x + 4}.

∫e3x+4 dx=13e3x+4+C.\int e^{3x + 4}\,dx = \frac{1}{3}e^{3x + 4} + C.

The key step in (b) is simplifying to a single exponential before integrating; one mark for that, one for the antiderivative.

Practise this

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