Calculus II: Power Reduction and Integration by Parts Flashcards
Algorithmic Power Reduction for Secant and Tangent
The lecture introduces an algorithmic approach to finding the integrals of high-powered trigonometric functions, specifically secant and tangent, using power reduction formulas.
This method is more efficient than the manual method of turning powers of secant into tangents (or vice versa) repeatedly, especially as the exponent n increases. It is described as the logic a computer program would follow to solve these integrals.
Power Reduction Formula for Secant:
The formula for a power of secant (n) is: ∫secn(x)dx=n−11secn−2(x)tan(x)+n−1n−2∫secn−2(x)dx
This formula reduces the power of the integral by 2 in each iteration until the remaining integral is either the integral of sec(x) (if n is odd) or sec0(x)=1 (if n is even).
Example: Evaluating ∫sec3(x)dx:
Identify n=3.
Applying the formula: 3−11sec3−2(x)tan(x)+3−13−2∫sec3−2(x)dx
Simplified: 21sec(x)tan(x)+21∫sec(x)dx
Result: The anti-derivative of sec(x) is ln∣sec(x)+tan(x)∣.
Final Solution: 21sec(x)tan(x)+21ln∣sec(x)+tan(x)∣+C
Example: Evaluating ∫sec5(x)dx:
Identify n=5.
First reduction: 41sec3(x)tan(x)+43∫sec3(x)dx
We then substitute the previously found value for ∫sec3(x)dx into this expression: 41sec3(x)tan(x)+43(21sec(x)tan(x)+21ln∣sec(x)+tan(x)∣)+C
Final simplified form (distributing the coefficient): 41sec3(x)tan(x)+83sec(x)tan(x)+83ln∣sec(x)+tan(x)∣+C
Power Reduction Formula for Tangent:
This formula contains a subtraction rather than an addition between terms because converting tangents to secants (via tan2(x)=sec2(x)−1) introduces a negative sign.
The formula is: ∫tann(x)dx=n−1tann−1(x)−∫tann−2(x)dx
This formula works for all n as long as the functions are defined on their domain; it is applied repeatedly until the remaining integral becomes ∫tan(x)dx or ∫1dx.
Example: Evaluating ∫tan4(x)dx:
Identify n=4.
First reduction: 31tan3(x)−∫tan2(x)dx
Apply formula again for n=2: 31tan3(x)−(1tan1(x)−∫tan0(x)dx) 31tan3(x)−tan(x)+∫1dx
Final Result: 31tan3(x)−tan(x)+x+C
Integration by Parts (IBP) Foundations
The IBP Formula: ∫udv=uv−∫vdu
Strategy for Choosing u and dv:
Choose u such that its derivative dxdu is simpler than u itself.
Choose dv such that its anti-derivative v is easy to calculate.
The lecturer notes that for polynomials multiplied by exponentials (e.g., x4ex), the polynomial is nearly always chosen as u to eventually reduce the power to zero through repeated integration.
Example: Integration of ∫x4exdx:
Let u=x4, du=4x3dx.
Let dv=exdx, v=ex.
Applying IBP: x4ex−∫4x3exdx
This requires doing integration by parts three more times (total of four iterations) to fully evaluate until the power of x becomes 0.
Example: Integration with Nested Logarithms ∫(ln(x))4dx:
Note: The exponent 4 is outside the natural log, meaning it cannot be brought to the front as a coefficient.
Let u=(ln(x))4. Use the chain rule for the derivative: du=4(ln(x))3×x1dx.
Let dv=dx, so v=x.
Result of first step: x(ln(x))4−∫x(x4(ln(x))3)dx=x(ln(x))4−∫4(ln(x))3dx
This process must be repeated until the the logarithm factor is eliminated.
Advanced Integration by Parts Techniques
Linear Arguments in Logs (∫ln(3r−4)dr):
Direct IBP: Set u=ln(3r−4) and dv=dr. This leads to a complicated algebraic integral ∫3r−43rdr. This requires an algebraic trick: rewrite 3r as (3r−4)+4 to split the fraction into 1+3r−44.
Initial U-Substitution (Recommended): Let w=3r−4, then dw=3dr or dr=31dw. The integral becomes 31∫ln(w)dw, which is a standard IBP setup (u=ln(w), dv=dw).
Cyclical Integrals (∫exsin(x)dx):
Neither a derivative of ex nor sin(x) ever reaches zero.
First IBP step: Choose u=sin(x), dv=exdx. Result: exsin(x)−∫excos(x)dx.
Second IBP step: Perform IBP on ∫excos(x)dx. Choose u=cos(x), dv=exdx. Result: excos(x)−∫ex(−sin(x))dx.
Algebraic solve: Substitute back to get I=exsin(x)−(excos(x)+I), where I is the original integral.
Combine terms: 2I=exsin(x)−excos(x).
Result: ∫exsin(x)dx=21(exsin(x)−excos(x))+C.
Definite Integrals with Integration by Parts
Definite Integral Example: ∫24t3ln(5t)dt:
In this case, choose u=ln(5t) because the derivative makes the log part disappear: du=5t5dt=t1dt.
Let dv=t3dt, so v=4t4.
IBP evaluation: [4t4ln(5t)]24−∫244t4×t1dt
[4t4ln(5t)]24−∫244t3dt=[4t4ln(5t)−16t4]24
Plug in upper bound (t=4): 4256ln(20)−16256=64ln(20)−16
Plug in lower bound (t=2): 416ln(10)−1616=4ln(10)−1
Subtracting bounds: (64ln(20)−16)−(4ln(10)−1)=64ln(20)−4ln(10)−15
Definite Integral Example: ∫1e4t2ln(t)dt:
Pull out the constant: 4∫1et2ln(t)dt.
Set u=ln(t), du=t1dt.
Set dv=t2dt, v=3t3.
Evaluating: 4([3t3ln(t)]1e−∫1e3t2dt)=4[3t3ln(t)−9t3]1e
Evaluate at e: 34e3ln(e)−94e3=34e3−94e3.
Evaluate at 1: 34(1)3ln(1)−94(1)3=0−94.
Result: 912e3−94e3−(−94)=98e3+4.
Inverse Trigonometric Integrals
Questions & Discussion
Q: Does tan0(x) simplify to 1?
A: Yes, anything raised to the power of zero is 1. While 00 is technically undefined, for the purposes of these integrals (power reduction), the function behaves as a constant 1 across the valid domain.
Q: When do we use these formulas vs. standard U-sub?
A: For something like tan6(x), these formulas are significantly faster. For combinations of secant and tangent where powers are mixed, one must still check the rules for even/odd powers to decide on the best strategy.
Q: Are there formulas for combined secant and tangent?
Q: How to provide answers on tests?