Trigonometric Integrals Lecture Notes

Strategies for Integrating Powers of Sine and Cosine

  • General Context: The focus is on evaluating integrals of the form sinK(x)cosJ(x)dx\int \sin^K(x) \cos^J(x) \, dx. The strategy depends primarily on whether the powers of sine (KK) or cosine (JJ) are odd or even.

  • Case 1: The Power of Sine (KK) is Odd

    • Procedure: Reduce the power of sine by one (sinK1(x)\sin^{K-1}(x)), so there is a single sin(x)\sin(x) factor left over to act as the derivative for substitution.

    • Substitution: Let u=cos(x)u = \cos(x). Then du=sin(x)dxdu = -\sin(x) \, dx.

    • Identity: Convert the remaining even powers of sine into terms of cosine using the Pythagorean identity: sin2(x)=1cos2(x)\sin^2(x) = 1 - \cos^2(x).

  • Case 2: The Power of Cosine (JJ) is Odd

    • Procedure: Reduce the power of cosine by one (cosJ1(x)\cos^{J-1}(x)), peeling off one cos(x)\cos(x) to serve as the derivative for substitution.

    • Substitution: Let u=sin(x)u = \sin(x). Then du=cos(x)dxdu = \cos(x) \, dx.

    • Identity: Convert the remaining even powers of cosine into terms of sine using the Pythagorean identity: cos2(x)=1sin2(x)\cos^2(x) = 1 - \sin^2(x).

Basic Example: Odd Power of Sine

  • Problem: sin(x)cos4(x)dx\int \sin(x) \cos^4(x) \, dx

  • Analysis: Sine is to the power of 1, which is odd. Since there is only one sine, there is no need to reduce the power or apply identities.

  • Execution:

    • Let u=cos(x)u = \cos(x).

    • Then du=sin(x)dxdu = -\sin(x) \, dx, which implies du=sin(x)dx-du = \sin(x) \, dx.

    • Rewrite the integral: u4du\int -u^4 \, du.

    • Antiderivative: u55+C- \frac{u^5}{5} + C.

  • Final Substitution: cos5(x)5+C- \frac{\cos^5(x)}{5} + C.

Advanced Example: Odd Power of Cosine

  • Problem: sin2(x)cos3(x)dx\int \sin^2(x) \cos^3(x) \, dx

  • Analysis: Cosine has the odd power (33). We peel off one cosine factor.

  • Execution:

    • Rewrite: sin2(x)cos2(x)cos(x)dx\int \sin^2(x) \cos^2(x) \cos(x) \, dx.

    • Convert cos2(x)\cos^2(x): sin2(x)(1sin2(x))cos(x)dx\int \sin^2(x) (1 - \sin^2(x)) \cos(x) \, dx.

    • Let u=sin(x)u = \sin(x). Then du=cos(x)dxdu = \cos(x) \, dx.

    • Substitute: u2(1u2)du=(u2u4)du\int u^2 (1 - u^2) \, du = \int (u^2 - u^4) \, du.

    • Integrate: u33u55+C\frac{u^3}{3} - \frac{u^5}{5} + C.

  • Final Substitution: sin3(x)3sin5(x)5+C\frac{\sin^3(x)}{3} - \frac{\sin^5(x)}{5} + C.

  • Verification Note: If you check the work by taking the derivative, the result may look different from the original integrand. You must apply trigonometric identities (like factoring out sin2(x)\sin^2(x) and converting (1sin2(x))(1 - \sin^2(x)) back to cos2(x)\cos^2(x)) to match the starting function.

Strategies for Even Powers (Double Angle Formulas)

  • Context: When both sine and cosine have even powers, u-u substitution is not immediately possible because no single sin(x)\sin(x) or cos(x)\cos(x) is available for dudu. We must use power-reduction/double-angle identities.

  • Core Identities:

    • sin2(x)=1cos(2x)2\sin^2(x) = \frac{1 - \cos(2x)}{2}

    • cos2(x)=1+cos(2x)2\cos^2(x) = \frac{1 + \cos(2x)}{2}

  • Example: Integrating sin2(x)\sin^2(x):

    • sin2(x)dx=1cos(2x)2dx=(12cos(2x)2)dx\int \sin^2(x) \, dx = \int \frac{1 - \cos(2x)}{2} \, dx = \int (\frac{1}{2} - \frac{\cos(2x)}{2}) \, dx.

    • Integration: 12xsin(2x)4+C\frac{1}{2}x - \frac{\sin(2x)}{4} + C.

    • Note: The division by 4 comes from the substitution u=2xu = 2x, where du=2dxdu = 2 \, dx, adding another factor of 12\frac{1}{2}.

  • Example: Integrating cos2(x)\cos^2(x):

    • cos2(x)dx=1+cos(2x)2dx=12x+sin(2x)4+C\int \cos^2(x) \, dx = \int \frac{1 + \cos(2x)}{2} \, dx = \frac{1}{2}x + \frac{\sin(2x)}{4} + C.

Scaling Factors in the Argument

  • If the argument of the function is already scaled, such as sin2(7x)\sin^2(7x), the double angle formula doubles that specific argument.

  • Example: sin2(7x)dx\int \sin^2(7x) \, dx

    • Formula: 1cos(2×7x)2=1cos(14x)2\frac{1 - \cos(2 \times 7x)}{2} = \frac{1 - \cos(14x)}{2}.

    • Integration results in: 12xsin(14x)28+C\frac{1}{2}x - \frac{\sin(14x)}{28} + C.

Higher Even Powers: cos4(x)\cos^4(x)

  • Strategy: Treat cos4(x)\cos^4(x) as (cos2(x))2(\cos^2(x))^2.

  • Step-by-Step Procedure:

    1. Apply identity: (1+cos(2x)2)2dx\int (\frac{1 + \cos(2x)}{2})^2 \, dx.

    2. Expand the square: 14(1+2cos(2x)+cos2(2x))dx\int \frac{1}{4}(1 + 2\cos(2x) + \cos^2(2x)) \, dx.

    3. Distribute the constant: (14+12cos(2x)+14cos2(2x))dx\int (\frac{1}{4} + \frac{1}{2}\cos(2x) + \frac{1}{4}\cos^2(2x)) \, dx.

    4. Apply double angle identity again to cos2(2x)\cos^2(2x): cos2(2x)=1+cos(4x)2\cos^2(2x) = \frac{1 + \cos(4x)}{2}.

    5. The third term becomes: 14(1+cos(4x)2)=18+cos(4x)8\frac{1}{4} (\frac{1 + \cos(4x)}{2}) = \frac{1}{8} + \frac{\cos(4x)}{8}.

    6. Combine constants: 14+18=38\frac{1}{4} + \frac{1}{8} = \frac{3}{8}.

    7. Final Antiderivative: 38x+sin(2x)4+sin(4x)32+C\frac{3}{8}x + \frac{\sin(2x)}{4} + \frac{\sin(4x)}{32} + C.

Integrals with Differing Scaling Factors (Product-to-Sum)

  • When the scaling factors inside sine and cosine are different (e.g., sin(mx)cos(nx)\sin(mx)\cos(nx)), use product-to-sum identities derived from sum and difference formulas.

  • Identity 2 (Sine and Cosine): sin(Ax)cos(Bx)=12[sin((AB)x)+sin((A+B)x)]\sin(Ax)\cos(Bx) = \frac{1}{2}[\sin((A-B)x) + \sin((A+B)x)]

  • Example: sin(5x)cos(3x)dx\int \sin(5x)\cos(3x) \, dx

    • Apply identity: 12(sin(2x)+sin(8x))dx\int \frac{1}{2}(\sin(2x) + \sin(8x)) \, dx.

    • Integrate: 12(cos(2x)2cos(8x)8)+C\frac{1}{2}(-\frac{\cos(2x)}{2} - \frac{\cos(8x)}{8}) + C.

Strategies for Secant and Tangent Integrals

  • Standard Integrals to Memorize:

    • sec2(x)dx=tan(x)+C\int \sec^2(x) \, dx = \tan(x) + C

    • sec(x)tan(x)dx=sec(x)+C\int \sec(x)\tan(x) \, dx = \sec(x) + C

    • tan(x)dx=lnsec(x)+C\int \tan(x) \, dx = \ln|\sec(x)| + C

    • sec(x)dx=lnsec(x)+tan(x)+C\int \sec(x) \, dx = \ln|\sec(x) + \tan(x)| + C

  • Pythagorean Identity: tan2(x)+1=sec2(x)\tan^2(x) + 1 = \sec^2(x).

  • Case A: The Power of Secant (JJ) is Even (J2J \ge 2)

    • Goal: Use u=tan(x)u = \tan(x). Peel off a sec2(x)\sec^2(x) for dudu.

    • Example: tan6(x)sec4(x)dx\int \tan^6(x) \sec^4(x) \, dx

      • Peel off sec2(x)\sec^2(x): tan6(x)sec2(x)sec2(x)dx\int \tan^6(x) \sec^2(x) \sec^2(x) \, dx.

      • Convert one sec2(x)\sec^2(x) to tan2(x)+1\tan^2(x) + 1.

      • Substitute u=tan(x),du=sec2(x)dxu = \tan(x), du = \sec^2(x) \, dx.

      • Resulting integral: u6(u2+1)du=(u8+u6)du\int u^6 (u^2 + 1) \, du = \int (u^8 + u^6) \, du.

      • Answer: tan9(x)9+tan7(x)7+C\frac{\tan^9(x)}{9} + \frac{\tan^7(x)}{7} + C.

  • Case B: The Power of Tangent (KK) is Odd (K1K \ge 1)

    • Goal: Use u=sec(x)u = \sec(x). Peel off a sec(x)tan(x)\sec(x)\tan(x) for dudu.

    • Example: tan3(x)sec3(x)dx\int \tan^3(x) \sec^3(x) \, dx

      • Peel off: tan2(x)sec2(x)(sec(x)tan(x))dx\int \tan^2(x) \sec^2(x) (\sec(x)\tan(x)) \, dx.

      • Convert tan2(x)\tan^2(x) to sec2(x)1\sec^2(x) - 1.

      • Substitute u=sec(x),du=sec(x)tan(x)dxu = \sec(x), du = \sec(x)\tan(x) \, dx.

      • Integral: (u21)u2du=(u4u2)du\int (u^2 - 1)u^2 \, du = \int (u^4 - u^2) \, du.

      • Answer: sec5(x)5sec3(x)3+C\frac{\sec^5(x)}{5} - \frac{\sec^3(x)}{3} + C.

  • Case C: Pure Power of Tangent (J=0J = 0)

    • Strategy: Separate tan2(x)\tan^2(x) and convert it to sec2(x)1\sec^2(x) - 1. Distribute and repeat the process if necessary.

  • Case D: Pure Power of Secant (Integration by Parts)

    • Example: sec3(x)dx\int \sec^3(x) \, dx:

      • Use Integration by Parts (udv=uvvdu\int u \, dv = uv - \int v \, du).

      • Let u=sec(x)u = \sec(x) and dv=sec2(x)dxdv = \sec^2(x) \, dx.

      • Then du=sec(x)tan(x)dxdu = \sec(x)\tan(x) \, dx and v=tan(x)v = \tan(x).

      • Apply IBP: sec(x)tan(x)tan2(x)sec(x)dx\sec(x)\tan(x) - \int \tan^2(x)\sec(x) \, dx.

      • Convert tan2(x)\tan^2(x): sec(x)tan(x)(sec2(x)1)sec(x)dx\sec(x)\tan(x) - \int (\sec^2(x) - 1)\sec(x) \, dx.

      • This results in: sec(x)tan(x)sec3(x)dx+sec(x)dx\sec(x)\tan(x) - \int \sec^3(x) \, dx + \int \sec(x) \, dx.

      • Recognize the "boomerang": Add sec3(x)dx\int \sec^3(x) \, dx to both sides to get 2sec3(x)dx2 \int \sec^3(x) \, dx.

      • Solve: sec3(x)dx=12[sec(x)tan(x)+lnsec(x)+tan(x)]+C\int \sec^3(x) \, dx = \frac{1}{2} [\sec(x)\tan(x) + \ln|\sec(x) + \tan(x)|] + C.

Questions & Discussion

  • Question: How did you go from sec3(x)\int \sec^3(x) \dots to sec5(x)\sec^5(x) in the explanation?

  • Answer: In the derivation of higher powers, you combine sec3(x)\sec^3(x) and sec2(x)\sec^2(x). sec3(x)×sec2(x)=sec3+2(x)=sec5(x)\sec^3(x) \times \sec^2(x) = \sec^{3+2}(x) = \sec^5(x). (Correction of minor error in verbal transcription regarding power of 6).

  • Discussion on Definite Integrals: Definite trigonometric integrals are evaluated the same way but require an extra step of algebra at the end to plug in bounds (e.g., 00 to π\pi). The instructor notes that these can be very long due to the algebra involved.

  • Future Schedule: Thursday will finish up trig integrals, work on integration by parts from homework, and spend the last 20-25 minutes reviewing. Next week will likely include one trig problem and then definite integrals.