First integral: (\int \sqrt9-y^2, dy) is a standard semicircle area formula. From (y=-3) to (0), it’s a quarter circle of radius 3. Area of quarter circle = (\frac14\pi (3^2) = \frac9\pi4). So (3 \times \frac9\pi4 = \frac27\pi4).
Rico remembered Ricardo Asin’s golden rule: “For work problems, slice it, find the force on each slice, multiply by the distance that slice travels, then integrate.”
Second integral: Let (u = 9-y^2), (du = -2y,dy), so (y,dy = -\frac12du). [ \int_-3^0 y\sqrt9-y^2,dy = \int_y=-3^0 \sqrtu \left(-\frac12 du\right) = -\frac12 \int_u=0^9 u^1/2 du = -\frac12 \cdot \frac23 u^3/2 \Big| 0^9 = -\frac13 (27) = -9. ] But careful with limits: actually (y=-3 \to u=0), (y=0 \to u=9), so (\int 0^9 \sqrtu (-\frac12 du) = -\frac12 \cdot \frac23 [27-0] = -9). Yes. Integral Calculus Reviewer By Ricardo Asin Pdf 54
Therefore: [ W = 196000 \left( \frac27\pi4 + 9 \right) \quad \textJoules. ]
Rico told the foreman, “About 5.9 megajoules.” The foreman nodded, and the pump worked perfectly—thanks to a slice, a distance, and an integral from page 54 of Ricardo Asin’s reviewer. First integral: (\int \sqrt9-y^2, dy) is a standard
Thus: [ \int_-3^0 y\sqrt9-y^2,dy = -9. ] So minus that term: ( -\int_-3^0 y\sqrt9-y^2 , dy = -(-9) = +9).
Each slice’s thickness = (dy). Width of the slice = (2x = 2\sqrt9 - y^2). Volume of the slice = length × width × thickness = (10 \cdot 2\sqrt9 - y^2 \cdot dy = 20\sqrt9-y^2 , dy). So (3 \times \frac9\pi4 = \frac27\pi4)
So bracket = (\frac27\pi4 + 9).