Some integrands are a product of two very different functions — xex, xcosx, logx, xsin−1x — where substitution gets you nowhere. Integration by parts is the tool for these. It comes straight from reversing the product rule for differentiation.
Starting from dxd(uv)=uv′+u′v and integrating both sides gives the working formula:
∫udxdvdx=uv−∫vdxdudx.
In words: integral of (first × derivative-of-second) = first × integral-of-second − integral of (derivative-of-first × integral-of-second).
Choosing u: the ILATE rule
The whole game is picking which factor is u (to differentiate) and which is dv (to integrate). Pick u by ILATE — the first type that appears:
The key idea is to simplify the integrand using the given substitution x=atan2θ, which turns the inverse sine into a simple angle. After substitution and integration by parts, the final result is (a+x)tan−1ax−ax+C.
The problem asks for the indefinite integral of sin−1a+xx. The expression inside the inverse sine looks messy, but the hint suggests a clever substitution: x=atan2θ. Why does this work? Because a+xx becomes something like a+atan2θatan2θ=1+tan2θtan2θ=sin2θ=sinθ (assuming θ in a suitable range). Then sin−1(sinθ)=θ, which is much simpler to integrate.
Let’s walk through it step by step.
Substitute x=atan2θ.
We need dx in terms of dθ. Differentiate:
dx=a⋅2tanθ⋅sec2θdθ=2atanθsec2θdθ.
Also, note that a+x=a+atan2θ=a(1+tan2θ)=asec2θ.
Simplify the integrand.
Compute a+xx:
asec2θatan2θ=sec2θtan2θ=sin2θ=sinθ,
taking θ∈[0,π/2) so sinθ≥0.
Hence sin−1a+xx=sin−1(sinθ)=θ.
Rewrite the integral.
The integral becomes:
I=∫θ⋅(2atanθsec2θ)dθ=2a∫θtanθsec2θdθ.
Simplify the trigonometric part.
Notice tanθsec2θ=cos3θsinθ. But a better approach: let t=tanθ, then dt=sec2θdθ, so tanθsec2θdθ=tdt. However, we still have θ in terms of t: θ=tan−1t. So:
I=2a∫θ⋅tdt=2a∫(tan−1t)⋅tdt.
Integrate by parts.
Let u=tan−1t and dv=tdt. Then du=1+t21dt and v=2t2.
Integration by parts gives:
Q.∫logexdx is equal to :
(A) xloge(ex)+c
(B) xloge(ex)+c
(C) xloge(xe)+c
(D) loge(ex)+c
›Reveal solutionSolution
∫ln x dx = x ln x − x + c = x·ln(x/e) + c.
Step 1 — Integration by parts
Take u=lnx, dv=dx, so du=x1dx, v=x:
∫lnxdx=xlnx−∫x⋅x1dx
Step 2 — Complete the integral
=xlnx−∫1dx=xlnx−x+c
Step 3 — Rewrite in the option's form
Factor x and use 1=lne:
x(lnx−1)=x(lnx−lne)=xln(ex)
∫lnxdx=xloge(ex)+c
Why the other options are wrong: (A) x·ln(ex) = x(ln x + 1) has the wrong sign; (C) x·ln(e/x) reverses the ratio; (D) drops the leading x factor. Only (B) matches x ln x − x. …
Q.If ∫{cos−1x−(1−x2)−1/2}Kdx=K⋅cos−1x+C, then K= ______.
(A) ex
(B) −ex
(C) e−x
(D) ecos−1x
›Reveal solutionSolution
[!TLDR] p-Si wafer (∼300μm) to thin n-Si emitter (∼1μm) gives a thickness ratio of about 300.
Concept
A p-n junction silicon solar cell is built on a relatively thick p-type wafer (the base/absorber) with a very thin n-type layer diffused on top (the emitter) so that light reaches the junction. The base is far thicker than the emitter.