Integrating tan & sec Products - Calculus 2

  1. Evaluate the integral ∫dxcos⁡2(x)tan⁡(x)\int \frac{dx}{\cos^2(x)\tan(x)}.
    Answer: ln⁡∣tan⁡(x)∣+C\ln|\tan(x)| + C When you encounter an integral with trigonometric functions like this, your first step should be to simplify the integrand using trigonometric identities. This will often reveal a more manageable form. Start by rewriting the integrand: 1cos⁡2(x)tan⁡(x)=1cos⁡2(x)⋅1tan⁡(x)=sec⁡2(x)⋅cot⁡(x)\frac{1}{\cos^2(x)\tan(x)} = \frac{1}{\cos^2(x)} \cdot \frac{1}{\tan(x)} = \sec^2(x) \cdot \cot(x) Since cot⁡(x)=cos⁡(x)sin⁡(x)\cot(x) = \frac{\cos(x)}{\sin(x)}, you can write this as: sec⁡2(x)⋅cot⁡(x)=1cos⁡2(x)⋅cos⁡(x)sin⁡(x)=1cos⁡(x)sin⁡(x)\sec^2(x) \cdot \cot(x) = \frac{1}{\cos^2(x)} \cdot \frac{\cos(x)}{\sin(x)} = \frac{1}{\cos(x)\sin(x)} Now use the substitution u=tan⁡(x)u = \tan(x), so du=sec⁡2(x)dxdu = \sec^2(x)dx. Notice that 1cos⁡(x)sin⁡(x)=sec⁡2(x)tan⁡(x)\frac{1}{\cos(x)\sin(x)} = \frac{\sec^2(x)}{\tan(x)}, which becomes 1udu\frac{1}{u}du. This integrates to ln⁡∣u∣+C=ln⁡∣tan⁡(x)∣+C\ln|u| + C = \ln|\tan(x)| + C, confirming answer D. Let's examine why the other options are incorrect: A would result from incorrectly thinking the derivative of cot⁡(x)\cot(x) is positive rather than −csc⁡2(x)-\csc^2(x). B comes from misapplying trigonometric identities and confusing this with ∫cot⁡(x)dx\int \cot(x)dx. C represents the antiderivative of sec⁡(x)tan⁡(x)\sec(x)\tan(x), not our integrand. Strategy tip: When facing complex trigonometric integrals, always simplify using identities first, then look for substitutions involving u=tan⁡(x)u = \tan(x), u=sin⁡(x)u = \sin(x), or u=cos⁡(x)u = \cos(x). The form 1u\frac{1}{u} should immediately signal ln⁡∣u∣\ln|u| as the antiderivative.
  2. The integral ∫tan⁡2(x)sec⁡3(x) dx\int \tan^2(x) \sec^3(x) \, dx can be rewritten using the identity tan⁡2(x)=sec⁡2(x)−1\tan^2(x) = \sec^2(x) - 1. What integral results from this substitution?
    Answer: ∫(sec⁡5(x)−sec⁡3(x)) dx\int (\sec^5(x) - \sec^3(x)) \, dx When you encounter integrals involving powers of trigonometric functions, using trigonometric identities to rewrite the integrand is often the key to simplification. This problem tests your ability to apply the Pythagorean identity tan⁡2(x)=sec⁡2(x)−1\tan^2(x) = \sec^2(x) - 1 correctly. Starting with ∫tan⁡2(x)sec⁡3(x) dx\int \tan^2(x) \sec^3(x) \, dx, substitute the identity: ∫(sec⁡2(x)−1)sec⁡3(x) dx\int (\sec^2(x) - 1) \sec^3(x) \, dx Using the distributive property: ∫sec⁡2(x)⋅sec⁡3(x) dx−∫1⋅sec⁡3(x) dx\int \sec^2(x) \cdot \sec^3(x) \, dx - \int 1 \cdot \sec^3(x) \, dx This simplifies to: ∫sec⁡5(x) dx−∫sec⁡3(x) dx=∫(sec⁡5(x)−sec⁡3(x)) dx\int \sec^5(x) \, dx - \int \sec^3(x) \, dx = \int (\sec^5(x) - \sec^3(x)) \, dx This confirms answer D is correct. Looking at the incorrect options: Answer A represents a common misconception where students think they can integrate each factor separately and multiply the results—this violates basic integration rules. Answer B has the wrong sign; it shows addition instead of subtraction, likely from misapplying the identity or making an algebraic error. Answer C incorrectly reduces the powers of secant, possibly from confusion about how exponents combine during multiplication. Remember this pattern: when you see products of trigonometric functions with different powers, look for identities that can split one function into simpler parts. The key is careful algebraic manipulation after substitution—distribute thoroughly and watch your signs.
  3. To evaluate an integral of the form ∫tan⁡m(x)sec⁡n(x) dx\int \tan^m(x) \sec^n(x) \, dx, the substitution u=sec⁡(x)u = \sec(x) is most effective under which general conditions for the integers mm and nn?
    Answer: mm is a positive odd integer and n≥1n \ge 1. The substitution u=sec⁡(x)u = \sec(x) requires the differential du=sec⁡(x)tan⁡(x) dxdu = \sec(x)\tan(x)\,dx. To use this, we must be able to factor out one sec⁡(x)\sec(x) term and one tan⁡(x)\tan(x) term from the integrand. This is possible if the power of tangent, mm, is at least 1 and odd, and the power of secant, nn, is at least 1. If mm is odd, we can factor out tan⁡(x)\tan(x), and the remaining even power tan⁡m−1(x)\tan^{m-1}(x) can be converted to secants using tan⁡2(x)=sec⁡2(x)−1\tan^2(x) = \sec^2(x) - 1.
  4. Which of the following is an antiderivative of f(x)=tan⁡2(x)sec⁡(x)f(x) = \tan^2(x) \sec(x)?
    Answer: 12sec⁡(x)tan⁡(x)−12ln⁡∣sec⁡(x)+tan⁡(x)∣+C\frac{1}{2}\sec(x)\tan(x) - \frac{1}{2}\ln|\sec(x) + \tan(x)| + C First, use the identity tan⁡2(x)=sec⁡2(x)−1\tan^2(x) = \sec^2(x) - 1. The integral becomes ∫(sec⁡2(x)−1)sec⁡(x) dx=∫(sec⁡3(x)−sec⁡(x)) dx\int (\sec^2(x) - 1)\sec(x)\,dx = \int (\sec^3(x) - \sec(x))\,dx. This separates into ∫sec⁡3(x) dx−∫sec⁡(x) dx\int \sec^3(x)\,dx - \int \sec(x)\,dx. Using the known formulas for these integrals, we get (12sec⁡(x)tan⁡(x)+12ln⁡∣sec⁡(x)+tan⁡(x)∣)−(ln⁡∣sec⁡(x)+tan⁡(x)∣)+C(\frac{1}{2}\sec(x)\tan(x) + \frac{1}{2}\ln|\sec(x) + \tan(x)|) - (\ln|\sec(x) + \tan(x)|) + C. Combining the logarithmic terms gives the final answer: 12sec⁡(x)tan⁡(x)−12ln⁡∣sec⁡(x)+tan⁡(x)∣+C\frac{1}{2}\sec(x)\tan(x) - \frac{1}{2}\ln|\sec(x) + \tan(x)| + C.
  5. The evaluation of ∫tan⁡m(x)sec⁡n(x) dx\int \tan^m(x) \sec^n(x) \, dx where mm is a non-negative even integer and nn is a positive odd integer typically requires which sequence of steps?
    Answer: Using identities to express the integrand in terms of sec⁡(x)\sec(x) alone, followed by integration by parts. This case (even tangent, odd secant) is the most complex scenario. Neither of the standard u-substitutions works directly. The typical strategy is to use the identity tan⁡2(x)=sec⁡2(x)−1\tan^2(x) = \sec^2(x) - 1 to convert all even powers of tangent into powers of secant. This results in a sum of integrals of the form ∫sec⁡k(x) dx\int \sec^k(x)\,dx where kk is odd. These integrals are then solved using integration by parts, often via a reduction formula.
  6. The area of the region bounded by the curve y=sec⁡2(x)tan⁡(x)y = \sec^2(x)\tan(x), the x-axis, and the lines x=0x=0 and x=π/3x=\pi/3 is given by which value?
    Answer: 32\frac{3}{2} The area is given by the definite integral ∫0π/3sec⁡2(x)tan⁡(x) dx\int_0^{\pi/3} \sec^2(x)\tan(x) \, dx. This integral can be solved with the substitution u=tan⁡(x)u = \tan(x), which gives du=sec⁡2(x) dxdu = \sec^2(x)\,dx. The bounds of integration change from x=0x=0 to u=tan⁡(0)=0u = \tan(0) = 0 and from x=π/3x=\pi/3 to u=tan⁡(π/3)=3u = \tan(\pi/3) = \sqrt{3}. The integral becomes ∫03u du\int_0^{\sqrt{3}} u \, du. Evaluating this gives [u22]03=(3)22−022=32[\frac{u^2}{2}]_0^{\sqrt{3}} = \frac{(\sqrt{3})^2}{2} - \frac{0^2}{2} = \frac{3}{2}.
  7. Which of the following integrals is equivalent to ∫tan⁡3(x) dx\int \tan^3(x) \, dx?
    Answer: ∫(sec⁡2(x)−1)tan⁡(x) dx\int (\sec^2(x) - 1)\tan(x) \, dx When you encounter integrals of powers of trigonometric functions, the key strategy is to use trigonometric identities to rewrite the integrand in a more manageable form. For tan⁡3(x)\tan^3(x), you need to break it down using the fundamental identity tan⁡2(x)=sec⁡2(x)−1\tan^2(x) = \sec^2(x) - 1. Starting with ∫tan⁡3(x) dx\int \tan^3(x) \, dx, rewrite this as ∫tan⁡(x)⋅tan⁡2(x) dx\int \tan(x) \cdot \tan^2(x) \, dx. Now substitute the identity: ∫tan⁡(x)⋅(sec⁡2(x)−1) dx=∫(sec⁡2(x)−1)tan⁡(x) dx\int \tan(x) \cdot (\sec^2(x) - 1) \, dx = \int (\sec^2(x) - 1)\tan(x) \, dx. This matches option C exactly. Looking at the wrong answers: Option A suggests 14tan⁡4(x)+C\frac{1}{4}\tan^4(x) + C, which would be correct if we were integrating tan⁡3(x)sec⁡2(x)\tan^3(x) \sec^2(x) using substitution, but that's not our original integral. Option B has (sec⁡2(x)+1)tan⁡(x)(\sec^2(x) + 1)\tan(x), which incorrectly adds 1 instead of subtracting it from sec⁡2(x)\sec^2(x) in the identity. Option D includes −x+C-x + C at the end, suggesting someone partially integrated (sec⁡2(x)−1)tan⁡(x)(\sec^2(x) - 1)\tan(x) and remembered that ∫(−1) dx=−x\int (-1) \, dx = -x, but this represents a completed integral, not an equivalent form of the original. The correct answer is C because it shows the proper application of the Pythagorean identity to transform tan⁡3(x)\tan^3(x) into an integrable form. Remember: when dealing with odd powers of tangent, always factor out one tan⁡(x)\tan(x) and convert the remaining even power using tan⁡2(x)=sec⁡2(x)−1\tan^2(x) = \sec^2(x) - 1.
  8. Which of the following represents the correct approach to evaluate ∫tan⁡5xsec⁡3x dx\int \tan^5 x \sec^3 x \, dx?
    Answer: Use substitution u=sec⁡xu = \sec x and rewrite tan⁡5x=(sec⁡2x−1)2⋅tan⁡x\tan^5 x = (\sec^2 x - 1)^2 \cdot \tan x For ∫tan⁡5xsec⁡3x dx\int \tan^5 x \sec^3 x \, dx, we have an odd power of tangent and an odd power of secant. The standard approach is to use u=sec⁡xu = \sec x, du=sec⁡xtan⁡x dxdu = \sec x \tan x \, dx. We need to factor out sec⁡xtan⁡x\sec x \tan x and express the remaining tan⁡4xsec⁡2x\tan^4 x \sec^2 x in terms of secant: tan⁡4x=(sec⁡2x−1)2\tan^4 x = (\sec^2 x - 1)^2. Choice A won't work because we can't easily express sec⁡3x\sec^3 x in terms of tangent. Choice C is unnecessarily complicated. Choice D converts to sine/cosine but isn't the most efficient method for this integral type.
  9. Evaluate the integral ∫tan⁡4(x) dx\int \tan^4(x) \, dx.
    Answer: 13tan⁡3(x)−tan⁡(x)+x+C\frac{1}{3}\tan^3(x) - \tan(x) + x + C Rewrite tan⁡4(x)\tan^4(x) as tan⁡2(x)tan⁡2(x)\tan^2(x) \tan^2(x) and substitute tan⁡2(x)=sec⁡2(x)−1\tan^2(x) = \sec^2(x) - 1 for one of the factors. This gives ∫tan⁡2(x)(sec⁡2(x)−1) dx=∫(tan⁡2(x)sec⁡2(x)−tan⁡2(x)) dx\int \tan^2(x)(\sec^2(x) - 1) \, dx = \int (\tan^2(x)\sec^2(x) - \tan^2(x)) \, dx. The integral separates into ∫tan⁡2(x)sec⁡2(x) dx−∫tan⁡2(x) dx\int \tan^2(x)\sec^2(x)\,dx - \int \tan^2(x)\,dx. For the first part, let u=tan⁡(x)u = \tan(x) to get ∫u2 du=u33=13tan⁡3(x)\int u^2\,du = \frac{u^3}{3} = \frac{1}{3}\tan^3(x). For the second part, ∫tan⁡2(x) dx=∫(sec⁡2(x)−1) dx=tan⁡(x)−x\int \tan^2(x)\,dx = \int (\sec^2(x) - 1)\,dx = \tan(x) - x. Combining these results gives 13tan⁡3(x)−(tan⁡(x)−x)+C=13tan⁡3(x)−tan⁡(x)+x+C\frac{1}{3}\tan^3(x) - (\tan(x) - x) + C = \frac{1}{3}\tan^3(x) - \tan(x) + x + C.
  10. Find the particular solution to the differential equation dydx=tan⁡3(x)\frac{dy}{dx} = \tan^3(x) given the initial condition y(0)=1y(0) = 1.
    Answer: y=12tan⁡2(x)+ln⁡∣cos⁡(x)∣+1y = \frac{1}{2}\tan^2(x) + \ln|\cos(x)| + 1 When you encounter a differential equation like dydx=tan⁡3(x)\frac{dy}{dx} = \tan^3(x), you need to integrate the right side and then apply the initial condition to find the particular solution. To integrate tan⁡3(x)\tan^3(x), use the identity tan⁡2(x)=sec⁡2(x)−1\tan^2(x) = \sec^2(x) - 1 to rewrite it as: tan⁡3(x)=tan⁡(x)⋅tan⁡2(x)=tan⁡(x)(sec⁡2(x)−1)=tan⁡(x)sec⁡2(x)−tan⁡(x)\tan^3(x) = \tan(x) \cdot \tan^2(x) = \tan(x)(\sec^2(x) - 1) = \tan(x)\sec^2(x) - \tan(x) Now integrate term by term: - ∫tan⁡(x)sec⁡2(x)dx=12tan⁡2(x)\int \tan(x)\sec^2(x) dx = \frac{1}{2}\tan^2(x) (using substitution u=tan⁡(x)u = \tan(x), du=sec⁡2(x)dxdu = \sec^2(x)dx) - ∫tan⁡(x)dx=ln⁡∣sec⁡(x)∣=−ln⁡∣cos⁡(x)∣\int \tan(x) dx = \ln|\sec(x)| = -\ln|\cos(x)| So y=12tan⁡2(x)−(−ln⁡∣cos⁡(x)∣)+C=12tan⁡2(x)+ln⁡∣cos⁡(x)∣+Cy = \frac{1}{2}\tan^2(x) - (-\ln|\cos(x)|) + C = \frac{1}{2}\tan^2(x) + \ln|\cos(x)| + C Apply the initial condition y(0)=1y(0) = 1: Since tan⁡(0)=0\tan(0) = 0 and cos⁡(0)=1\cos(0) = 1, we get 1=0+ln⁡(1)+C=C1 = 0 + \ln(1) + C = C. Therefore, the particular solution is y=12tan⁡2(x)+ln⁡∣cos⁡(x)∣+1y = \frac{1}{2}\tan^2(x) + \ln|\cos(x)| + 1, which is choice D. Choice A uses sec⁡2(x)\sec^2(x) instead of 12tan⁡2(x)\frac{1}{2}\tan^2(x) and has the wrong sign on the logarithm. Choice B has the correct 12tan⁡2(x)\frac{1}{2}\tan^2(x) term but uses −ln⁡∣sec⁡(x)∣-\ln|\sec(x)| instead of +ln⁡∣cos⁡(x)∣+\ln|\cos(x)|. Choice C completely misses the tan⁡(x)\tan(x) integration, showing only the tan⁡(x)sec⁡2(x)\tan(x)\sec^2(x) result. Remember: when integrating powers of tangent, break them down using tan⁡2(x)=sec⁡2(x)−1\tan^2(x) = \sec^2(x) - 1 to create manageable integrals.
  11. Evaluate ∫tan⁡3xsec⁡4x dx\int \tan^3 x \sec^4 x \, dx using an appropriate substitution technique.
    Answer: 14tan⁡4x+16tan⁡6x+C\frac{1}{4}\tan^4 x + \frac{1}{6}\tan^6 x + C Since we have an even power of secant, we can use the substitution u=tan⁡xu = \tan x, so du=sec⁡2x dxdu = \sec^2 x \, dx. We rewrite sec⁡4x=sec⁡2x⋅sec⁡2x=sec⁡2x(1+tan⁡2x)=sec⁡2x(1+u2)\sec^4 x = \sec^2 x \cdot \sec^2 x = \sec^2 x(1 + \tan^2 x) = \sec^2 x(1 + u^2). The integral becomes ∫u3(1+u2) du=∫(u3+u5) du=u44+u66+C=14tan⁡4x+16tan⁡6x+C\int u^3(1 + u^2) \, du = \int (u^3 + u^5) \, du = \frac{u^4}{4} + \frac{u^6}{6} + C = \frac{1}{4}\tan^4 x + \frac{1}{6}\tan^6 x + C. Choice B uses incorrect powers (missing the squared term expansion). Choice C incorrectly substitutes for secant instead of tangent. Choice D uses wrong exponents from integration errors.
  12. Consider the integral ∫sec⁡5(x) dx\int \sec^5(x) \, dx. Using the reduction formula In=1n−1sec⁡n−2(x)tan⁡(x)+n−2n−1In−2I_n = \frac{1}{n-1}\sec^{n-2}(x)\tan(x) + \frac{n-2}{n-1}I_{n-2}, where In=∫sec⁡n(x) dxI_n = \int \sec^n(x)\,dx, what is the integral I5I_5?
    Answer: 14sec⁡3(x)tan⁡(x)+38sec⁡(x)tan⁡(x)+38ln⁡∣sec⁡(x)+tan⁡(x)∣+C\frac{1}{4}\sec^3(x)\tan(x) + \frac{3}{8}\sec(x)\tan(x) + \frac{3}{8}\ln|\sec(x)+\tan(x)| + C When you encounter integrals of powers of secant, reduction formulas are your best tool because direct integration becomes extremely complex for higher powers. The key is applying the formula systematically and knowing the base cases. Starting with the given reduction formula for I5=∫sec⁡5(x) dxI_5 = \int \sec^5(x) \, dx, substitute n=5n = 5: I5=15−1sec⁡5−2(x)tan⁡(x)+5−25−1I5−2=14sec⁡3(x)tan⁡(x)+34I3I_5 = \frac{1}{5-1}\sec^{5-2}(x)\tan(x) + \frac{5-2}{5-1}I_{5-2} = \frac{1}{4}\sec^3(x)\tan(x) + \frac{3}{4}I_3 Now you need I3=∫sec⁡3(x) dxI_3 = \int \sec^3(x) \, dx. Apply the formula again with n=3n = 3: I3=13−1sec⁡3−2(x)tan⁡(x)+3−23−1I3−2=12sec⁡(x)tan⁡(x)+12I1I_3 = \frac{1}{3-1}\sec^{3-2}(x)\tan(x) + \frac{3-2}{3-1}I_{3-2} = \frac{1}{2}\sec(x)\tan(x) + \frac{1}{2}I_1 The base case is I1=∫sec⁡(x) dx=ln⁡∣sec⁡(x)+tan⁡(x)∣+CI_1 = \int \sec(x) \, dx = \ln|\sec(x) + \tan(x)| + C. Substituting back: I3=12sec⁡(x)tan⁡(x)+12ln⁡∣sec⁡(x)+tan⁡(x)∣+CI_3 = \frac{1}{2}\sec(x)\tan(x) + \frac{1}{2}\ln|\sec(x) + \tan(x)| + C Therefore: I5=14sec⁡3(x)tan⁡(x)+34⋅[12sec⁡(x)tan⁡(x)+12ln⁡∣sec⁡(x)+tan⁡(x)∣]+CI_5 = \frac{1}{4}\sec^3(x)\tan(x) + \frac{3}{4} \cdot \left[\frac{1}{2}\sec(x)\tan(x) + \frac{1}{2}\ln|\sec(x) + \tan(x)|\right] + C =14sec⁡3(x)tan⁡(x)+38sec⁡(x)tan⁡(x)+38ln⁡∣sec⁡(x)+tan⁡(x)∣+C= \frac{1}{4}\sec^3(x)\tan(x) + \frac{3}{8}\sec(x)\tan(x) + \frac{3}{8}\ln|\sec(x) + \tan(x)| + C This matches answer C. Answer A stops at the first reduction step without continuing to I3I_3. Answer B incorrectly computes the coefficients in the reduction. Answer D has incorrect signs, likely from algebraic errors during substitution. Always work reduction formulas step-by-step down to known base cases, and double-check your arithmetic at each substitution.
  13. Evaluate the definite integral ∫0π/8sec⁡4(2x)tan⁡(2x) dx\int_0^{\pi/8} \sec^4(2x) \tan(2x) \, dx.
    Answer: 38\frac{3}{8} Let w=2xw = 2x, so dw=2dxdw = 2dx or dx=12dwdx = \frac{1}{2}dw. The integral becomes 12∫0π/4sec⁡4(w)tan⁡(w) dw\frac{1}{2}\int_{0}^{\pi/4} \sec^4(w) \tan(w) \, dw. This fits both standard cases. Let's use u=sec⁡(w)u=\sec(w), so du=sec⁡(w)tan⁡(w) dwdu = \sec(w)\tan(w)\,dw. The integral is 12∫sec⁡3(w)(sec⁡(w)tan⁡(w)) dw\frac{1}{2}\int \sec^3(w) (\sec(w)\tan(w))\,dw. In terms of uu, this is 12∫u3 du=12u44=18u4=18sec⁡4(w)\frac{1}{2} \int u^3\,du = \frac{1}{2} \frac{u^4}{4} = \frac{1}{8}u^4 = \frac{1}{8}\sec^4(w). Evaluating from w=0w=0 to w=π/4w=\pi/4: [18sec⁡4(w)]0π/4=18(sec⁡4(π/4)−sec⁡4(0))=18((2)4−14)=18(4−1)=38[\frac{1}{8}\sec^4(w)]_0^{\pi/4} = \frac{1}{8}(\sec^4(\pi/4) - \sec^4(0)) = \frac{1}{8}((\sqrt{2})^4 - 1^4) = \frac{1}{8}(4 - 1) = \frac{3}{8}.
  14. To evaluate ∫sec⁡2(x)tan⁡(x) dx\int \frac{\sec^2(x)}{\sqrt{\tan(x)}} \, dx, a u-substitution is performed. What is the resulting integral in terms of uu?
    Answer: ∫u−1/2 du\int u^{-1/2} \, du The integrand can be written as ∫(tan⁡(x))−1/2sec⁡2(x) dx\int (\tan(x))^{-1/2} \sec^2(x) \, dx. The presence of tan⁡(x)\tan(x) and its derivative sec⁡2(x)\sec^2(x) suggests the substitution u=tan⁡(x)u = \tan(x). The differential is du=sec⁡2(x) dxdu = \sec^2(x)\,dx. Substituting uu and dudu into the integral directly yields ∫u−1/2 du\int u^{-1/2} \, du.
  15. Evaluate the integral ∫tan⁡(x)sec⁡(x)−tan⁡(x) dx\int \frac{\tan(x)}{\sec(x) - \tan(x)} \, dx.
    Answer: sec⁡(x)+tan⁡(x)−x+C\sec(x) + \tan(x) - x + C When you encounter integrals involving trigonometric functions like tangent and secant, look for opportunities to use substitution or recognize patterns that simplify through trigonometric identities. To solve ∫tan⁡(x)sec⁡(x)−tan⁡(x) dx\int \frac{\tan(x)}{\sec(x) - \tan(x)} \, dx, multiply both numerator and denominator by (sec⁡(x)+tan⁡(x))(\sec(x) + \tan(x)): tan⁡(x)sec⁡(x)−tan⁡(x)⋅sec⁡(x)+tan⁡(x)sec⁡(x)+tan⁡(x)=tan⁡(x)(sec⁡(x)+tan⁡(x))sec⁡2(x)−tan⁡2(x)\frac{\tan(x)}{\sec(x) - \tan(x)} \cdot \frac{\sec(x) + \tan(x)}{\sec(x) + \tan(x)} = \frac{\tan(x)(\sec(x) + \tan(x))}{\sec^2(x) - \tan^2(x)} Since sec⁡2(x)−tan⁡2(x)=1\sec^2(x) - \tan^2(x) = 1, this becomes: tan⁡(x)(sec⁡(x)+tan⁡(x))=tan⁡(x)sec⁡(x)+tan⁡2(x)\tan(x)(\sec(x) + \tan(x)) = \tan(x)\sec(x) + \tan^2(x) Now integrate each term: - ∫tan⁡(x)sec⁡(x) dx=sec⁡(x)+C1\int \tan(x)\sec(x) \, dx = \sec(x) + C_1 - ∫tan⁡2(x) dx=∫(sec⁡2(x)−1) dx=tan⁡(x)−x+C2\int \tan^2(x) \, dx = \int (\sec^2(x) - 1) \, dx = \tan(x) - x + C_2 Therefore: sec⁡(x)+tan⁡(x)−x+C\sec(x) + \tan(x) - x + C, which is choice C. Choice A incorrectly combines logarithmic and polynomial forms that don't match our integration result. Choice B has the wrong sign on the xx term and suggests sec⁡(x)−tan⁡(x)\sec(x) - \tan(x) instead of sec⁡(x)+tan⁡(x)\sec(x) + \tan(x). Choice D involves ln⁡∣cos⁡(x)∣\ln|\cos(x)| and −sec⁡(x)-\sec(x), which would arise from completely different integral setups. Strategy tip: When dealing with rational trigonometric expressions, try multiplying by the conjugate of the denominator. This often eliminates complex denominators using the identity sec⁡2(x)−tan⁡2(x)=1\sec^2(x) - \tan^2(x) = 1, making integration much more manageable.
  16. Evaluate the indefinite integral ∫sec⁡4(x)tan⁡2(x) dx\int \frac{\sec^4(x)}{\tan^2(x)} \, dx.
    Answer: −cot⁡(x)+tan⁡(x)+C-\cot(x) + \tan(x) + C When you encounter integrals involving powers of trigonometric functions, look for opportunities to rewrite them using fundamental identities and algebraic manipulation before attempting substitution or integration by parts. Start by rewriting this integral using the identity sec⁡2(x)=1+tan⁡2(x)\sec^2(x) = 1 + \tan^2(x): ∫sec⁡4(x)tan⁡2(x) dx=∫sec⁡2(x)⋅sec⁡2(x)tan⁡2(x) dx=∫(1+tan⁡2(x))sec⁡2(x)tan⁡2(x) dx\int \frac{\sec^4(x)}{\tan^2(x)} \, dx = \int \frac{\sec^2(x) \cdot \sec^2(x)}{\tan^2(x)} \, dx = \int \frac{(1 + \tan^2(x)) \sec^2(x)}{\tan^2(x)} \, dx Split this into two separate integrals: ∫sec⁡2(x)tan⁡2(x) dx+∫tan⁡2(x)sec⁡2(x)tan⁡2(x) dx=∫sec⁡2(x)tan⁡2(x) dx+∫sec⁡2(x) dx\int \frac{\sec^2(x)}{\tan^2(x)} \, dx + \int \frac{\tan^2(x) \sec^2(x)}{\tan^2(x)} \, dx = \int \frac{\sec^2(x)}{\tan^2(x)} \, dx + \int \sec^2(x) \, dx The second integral is straightforward: ∫sec⁡2(x) dx=tan⁡(x)\int \sec^2(x) \, dx = \tan(x) For the first integral, use the identity sec⁡2(x)tan⁡2(x)=1sin⁡2(x)=csc⁡2(x)\frac{\sec^2(x)}{\tan^2(x)} = \frac{1}{\sin^2(x)} = \csc^2(x) Therefore: ∫csc⁡2(x) dx=−cot⁡(x)\int \csc^2(x) \, dx = -\cot(x) Combining both parts: −cot⁡(x)+tan⁡(x)+C-\cot(x) + \tan(x) + C, which is answer C. Answer A incorrectly involves secant and cosecant functions that don't appear in the correct antiderivative. Answer B has the wrong sign on the cotangent term. Answer D suggests a logarithmic form that would only arise from a rational function in tangent, not from this particular combination. Strategy tip: When dealing with quotients of trigonometric powers, always try rewriting using Pythagorean identities first. This often transforms complex expressions into recognizable standard forms.
  17. The integral ∫xsec⁡(x)tan⁡(x) dx\int x \sec(x) \tan(x) \, dx is best evaluated using which technique?
    Answer: Integration by parts with u=xu = x and dv=sec⁡(x)tan⁡(x) dxdv = \sec(x)\tan(x)\,dx. The integral contains a product of an algebraic function (xx) and a trigonometric function (sec⁡(x)tan⁡(x)\sec(x)\tan(x)). This structure suggests integration by parts. The choice of uu and dvdv is guided by the LIATE rule (Log, Inverse, Algebraic, Trig, Exponential). We choose the algebraic term u=xu=x, as its derivative simplifies to du=dxdu=dx. The remaining part, dv=sec⁡(x)tan⁡(x) dxdv = \sec(x)\tan(x)\,dx, is a standard derivative, and its integral is v=sec⁡(x)v=\sec(x). This choice leads to a simpler integral to solve. The alternative choice in B would lead to a more complex integral.
  18. Evaluate ∫sin⁡3(x)cos⁡6(x) dx\int \frac{\sin^3(x)}{\cos^6(x)} \, dx.
    Answer: 15sec⁡5(x)−13sec⁡3(x)+C\frac{1}{5}\sec^5(x) - \frac{1}{3}\sec^3(x) + C First, rewrite the integrand in terms of tangent and secant: ∫sin⁡3(x)cos⁡3(x)⋅1cos⁡3(x) dx=∫tan⁡3(x)sec⁡3(x) dx\int \frac{\sin^3(x)}{\cos^3(x)} \cdot \frac{1}{\cos^3(x)} \, dx = \int \tan^3(x) \sec^3(x) \, dx. Since the power of tangent is odd, save a sec⁡(x)tan⁡(x)\sec(x)\tan(x) factor and let u=sec⁡(x)u = \sec(x). The integral becomes ∫tan⁡2(x)sec⁡2(x)(sec⁡(x)tan⁡(x)) dx\int \tan^2(x)\sec^2(x)(\sec(x)\tan(x))\,dx. Substitute tan⁡2(x)=sec⁡2(x)−1\tan^2(x) = \sec^2(x) - 1 to get ∫(sec⁡2(x)−1)sec⁡2(x)(sec⁡(x)tan⁡(x)) dx\int (\sec^2(x)-1)\sec^2(x)(\sec(x)\tan(x))\,dx. With u=sec⁡(x)u = \sec(x) and du=sec⁡(x)tan⁡(x) dxdu = \sec(x)\tan(x)\,dx, this becomes ∫(u2−1)u2 du=∫(u4−u2) du=u55−u33+C\int (u^2-1)u^2\,du = \int (u^4 - u^2)\,du = \frac{u^5}{5} - \frac{u^3}{3} + C. Substituting back gives 15sec⁡5(x)−13sec⁡3(x)+C\frac{1}{5}\sec^5(x) - \frac{1}{3}\sec^3(x) + C.
  19. If In=∫sec⁡n(x) dxI_n = \int \sec^n(x) \, dx for n≥2n \ge 2, which of the following gives the reduction formula for InI_n?
    Answer: In=1n−1sec⁡n−2(x)tan⁡(x)+n−2n−1In−2I_n = \frac{1}{n-1}\sec^{n-2}(x)\tan(x) + \frac{n-2}{n-1}I_{n-2} The reduction formula is derived using integration by parts on ∫sec⁡n−2(x)sec⁡2(x) dx\int \sec^{n-2}(x) \sec^2(x) \, dx. Let u=sec⁡n−2(x)u = \sec^{n-2}(x) and dv=sec⁡2(x) dxdv = \sec^2(x)\,dx. Then du=(n−2)sec⁡n−2(x)tan⁡(x) dxdu = (n-2)\sec^{n-2}(x)\tan(x)\,dx and v=tan⁡(x)v = \tan(x). Applying the formula uv−∫v duuv - \int v\,du gives In=sec⁡n−2(x)tan⁡(x)−(n−2)∫sec⁡n−2(x)tan⁡2(x) dxI_n = \sec^{n-2}(x)\tan(x) - (n-2)\int \sec^{n-2}(x)\tan^2(x)\,dx. Using tan⁡2(x)=sec⁡2(x)−1\tan^2(x) = \sec^2(x)-1, we get In=sec⁡n−2(x)tan⁡(x)−(n−2)∫(sec⁡n(x)−sec⁡n−2(x)) dxI_n = \sec^{n-2}(x)\tan(x) - (n-2)\int (\sec^n(x) - \sec^{n-2}(x))\,dx. This becomes In=sec⁡n−2(x)tan⁡(x)−(n−2)In+(n−2)In−2I_n = \sec^{n-2}(x)\tan(x) - (n-2)I_n + (n-2)I_{n-2}. Solving for InI_n yields (n−1)In=sec⁡n−2(x)tan⁡(x)+(n−2)In−2(n-1)I_n = \sec^{n-2}(x)\tan(x) + (n-2)I_{n-2}, which gives the correct formula.
  20. Evaluate the definite integral ∫0π/4tan⁡3(x)sec⁡4(x) dx\int_0^{\pi/4} \tan^3(x) \sec^4(x) \, dx
    Answer: 512\frac{5}{12} The power of secant is even, so we save a sec⁡2(x)\sec^2(x) factor and use the identity sec⁡2(x)=1+tan⁡2(x)\sec^2(x) = 1 + \tan^2(x). The integral becomes ∫0π/4tan⁡3(x)(1+tan⁡2(x))sec⁡2(x) dx\int_0^{\pi/4} \tan^3(x)(1+\tan^2(x))\sec^2(x)\,dx. Let u=tan⁡(x)u = \tan(x), so du=sec⁡2(x) dxdu = \sec^2(x)\,dx. The bounds change: when x=0,u=tan⁡(0)=0x=0, u=\tan(0)=0; when x=π/4,u=tan⁡(π/4)=1x=\pi/4, u=\tan(\pi/4)=1. The integral in uu is ∫01u3(1+u2) du=∫01(u3+u5) du\int_0^1 u^3(1+u^2)\,du = \int_0^1 (u^3+u^5)\,du. Evaluating this gives [u44+u66]01=(14+16)−0=3+212=512[\frac{u^4}{4} + \frac{u^6}{6}]_0^1 = (\frac{1}{4} + \frac{1}{6}) - 0 = \frac{3+2}{12} = \frac{5}{12}.

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