Trig Substitution: Let's do a trig substitution because that x2+1 looks like the hypotenuse of a right triangle if x was one of the other sides. So, we set x=tan(θ), which means dx=sec2(θ)dθ.
Integral Simplification: Now we substitute x with tan(θ) in the integral. The integral becomes ∫(tan2(θ)+1⋅sec2(θ),dθ).
Integration by Parts: We know that tan2(θ)+1 is just sec(θ), so the integral simplifies to ∫(sec3(θ),dθ).
Simplifying Integral: This integral is a bit tricky, but we can use integration by parts. Let's set u=sec(θ) and dv=sec2(θ)dθ. Then du=sec(θ)tan(θ)dθ and v=tan(θ).
Splitting Integral: Using integration by parts, we get sec(θ)tan(θ)−∫(tan2(θ)sec(θ),dθ).
Integral of sec(θ): We can simplify the integral further by using the identity tan2(θ)=sec2(θ)−1. So the integral becomes ∫(sec3(θ)−sec(θ),dθ).
Solution in terms of θ: Now we split the integral into two parts: ∫(sec3(θ),dθ)−∫(sec(θ),dθ).
Conversion to x: The integral of sec(θ) is ln∣sec(θ)+tan(θ)∣. So we have that part of the solution.
Finding Antiderivative: The integral of sec3(θ) is a bit more complex, and we might need to use a reduction formula or other methods to solve it. But let's say we somehow find the antiderivative of sec3(θ), which we'll call I for now.
Final Solution: So our solution in terms of θ is I−ln∣sec(θ)+tan(θ)∣+C.
Correction: We need to convert back to x. Since x=tan(θ), we have sec(θ)=x2+1. So our solution in terms of x is I−ln∣x2+1+x∣+C.
Correction: We need to convert back to x. Since x=tan(θ), we have sec(θ)=x2+1. So our solution in terms of x is I−ln∣x2+1+x∣+C.But wait, we didn't actually find the antiderivative of sec3(θ), we just called it I. That's not right, we need to actually calculate it or look it up. This is a mistake, we can't just name it I and move on.
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