d/dx [∫₀^(x²) sin t dt] = ? (by FTC Part 1 with chain rule) — sin(x²)·2x.FTC Part 1: d/dx[∫₀^u sin t dt] = sin(u). Here u = x², so multiply by du/dx = 2x. Result: 2x sin(x²).
∫ x/√(x²+1) dx = ? — √(x²+1) + C.u = x²+1, du = 2x dx. ∫(1/√u)(du/2) = (1/2)·2√u + C = √(x²+1) + C.
∫ ln(x)/x dx = ? — (ln x)²/2 + C.u = ln x, du = (1/x) dx. ∫u du = u²/2 + C = (ln x)²/2 + C.
Area between y = x² and y = 4 (above x² and below 4): — 32/3.Intersect: x² = 4 → x = ±2. ∫₋₂^2 (4−x²) dx = [4x−x³/3]₋₂^2 = (8−8/3)−(−8+8/3) = 2(8−8/3) = 2·16/3 = 32/3.
∫₁^2 2x(x²+1)³ dx with u=x²+1: the result is: — (5⁴−2⁴)/4 = (625−16)/4.x=1→u=2, x=2→u=5. ∫₂^5 u³ du = [u⁴/4]₂^5 = 625/4 − 16/4 = 609/4.
Area between y = x and y = x³ from −1 to 1 (by symmetry or direct): — 1/2.By symmetry, 2∫₀^1 (x−x³) dx = 2[x²/2 − x⁴/4]₀^1 = 2(1/2 − 1/4) = 2(1/4) = 1/2.
∫ tan x dx = ? — −ln|cos x| + C.∫sin x/cos x dx. u = cos x, du = −sin x dx. −∫du/u = −ln|u| + C = −ln|cos x| + C.
∫ dx/(1+x²) = ? — arctan(x) + C.∫1/(1+x²) dx = arctan(x) + C. This is a standard formula.
Area between y = eˣ and y = e^(−x) from 0 to 1: — e + 1/e − 2.∫₀^1 (eˣ − e^(−x)) dx = [eˣ + e^(−x)]₀^1 = (e + 1/e) − (1 + 1) = e + 1/e − 2.
∫ x·√(x²+1) dx = ? — (x²+1)^(3/2)/3 + C.u = x²+1, du = 2x dx, x dx = du/2. ∫√u · du/2 = (1/2)·(2/3)u^(3/2) + C = u^(3/2)/3 + C = (x²+1)^(3/2)/3 + C.
∫ arctan x dx: u = arctan x, dv = dx: — x arctan x − (1/2)ln(1+x²) + C.u=arctan x, v=x. ∫arctan x dx = x·arctan x − ∫x/(1+x²) dx = x arctan x − (1/2)ln(1+x²) + C.
∫eˣ sin x dx: which technique applies? — IBP applied twice (cyclic).IBP twice on ∫eˣ sin x dx cycles back to the original integral, allowing algebraic solution.
For ∫eˣ cos x dx = I, after two IBP we get I = eˣ sin x + eˣ cos x − I. Solving: — I = eˣ(sin x + cos x)/2 + C.2I = eˣ(sin x + cos x) → I = eˣ(sin x + cos x)/2 + C.
∫ x²·ln x dx (use LIATE: u = ln x): — x³ ln x/3 − x³/9 + C.u=ln x, dv=x² dx, v=x³/3. IBP: (x³/3)ln x − ∫(x³/3)(1/x) dx = (x³/3)ln x − x³/9 + C.
Integration by parts CANNOT be used for: — ∫ sin(x²) dx (requires substitution, not IBP directly).∫sin(x²) dx has no elementary antiderivative from IBP or substitution — it requires special functions.
∫ √x·ln x dx (u = ln x, dv = √x dx): — (2x^(3/2)/3)·ln x − (4x^(3/2)/9) + C.u=ln x, v=2x^(3/2)/3. IBP: (2x^(3/2)/3)ln x − ∫(2x^(3/2)/3)(1/x) dx = (2x^(3/2)/3)ln x − (2/3)∫x^(1/2) dx = (2x^(3/2)/3)ln x − (4x^(3/2)/9) + C.
∫ x³·eˣ dx (generalized): result involves: — 4 terms: x³, x², x, constant times eˣ.Each IBP reduces x power by 1: x³eˣ − 3x²eˣ + 6xeˣ − 6eˣ + C — four eˣ terms.
∫ sec³x dx (a classic IBP problem) equals: — (1/2)(sec x tan x + ln|sec x + tan x|) + C.∫sec³x dx = (1/2)(sec x tan x + ln|sec x + tan x|) + C. This is derived by IBP on ∫sec x·sec²x dx.