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You've integrated the logarithm. You probably used a trick — integration by parts, flashed past too fast to follow, then dismissed. But look at the answer: x ln x āˆ’ x + C. Why that product? Why the minus? Why exactly x? Every inverse function seems to need its own trick. Or they're all the same trick, and nobody showed you the picture. The Geometry of Integration Watch what happens when you frame two integrals—one of a function f, one of its inverse—against a single curve. The curve crosses an L-shaped region corner to corner. It cuts that L into exactly two pieces. The two integrals are those two pieces. No derivatives. No limits. No calculus tricks at all—just read it straight off the geometry. This is the central identity that connects them all: āˆ«ā‚įµ‡ f(x) dx + āˆ«źœ€įµˆ f⁻¹(y) dy = bd āˆ’ ac With c = f(a) and d = f(b), this single picture explains every integral of an inverse function you've ever seen. What You'll Discover Why integration by parts has that exact form (it's not a trick—it's a picture) How the inverse function and the original function tile a rectangle Why e^x's integral of ln x comes out so cleanly (spoiler: the curve is its own antiderivative) How this theorem goes deeper than calculus: Darboux sums, Stieltjes integration, even holomorphic functions A 120-year-old identity that keeps being rediscovered because it looks like it should already be famous For Curious Minds If you love visual mathematics—if you want to understand why formulas have the shapes they do—this is the geometry hiding inside integration by parts, waiting for somebody to draw the box around it. The philosophy: Understand first. Formalize later.

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