∫(sin x + cos x) dx = ? — −cos x + sin x + C.∫sin x = −cos x; ∫cos x = sin x. Total: −cos x + sin x + C.
The indefinite integral ∫f(x) dx represents: — A family of functions (all antiderivatives).∫f(x) dx = F(x) + C — the entire family of antiderivatives, parameterized by the constant C.
∫sec²x dx = ? — tan x + C.∫sec²x dx = tan x + C. (Verify: d/dx[tan x] = sec²x. ✓)
Initial condition problem: if F'(x) = 2x and F(0) = 3, then F(x) = ? — x² + 3.∫2x dx = x² + C. Apply F(0) = 3: 0 + C = 3 → C = 3. F(x) = x² + 3.
FTC Part 1 states: d/dx ∫_a^x f(t) dt = ? — f(x).FTC Part 1: the derivative of the integral with variable upper limit equals the integrand evaluated at x: d/dx ∫_a^x f(t) dt = f(x).
∫_a^b f(x) dx = −∫_b^a f(x) dx. This means: — Swapping limits negates the integral.Swapping the limits of integration changes the sign: ∫_a^b f dx = −∫_b^a f dx.
A Riemann sum approximates ∫_a^b f(x) dx by: — Summing n rectangle areas with width Δx = (b−a)/n.Riemann sum: Σ f(xᵢ*)·Δx. As n→∞, this converges to the exact definite integral.
If f(x) < 0 on [a,b], then ∫_a^b f(x) dx is: — Negative.When f is negative on the entire interval, the net signed area is negative.
The average value of f on [a,b] is: — (1/(b−a))·∫_a^b f(x) dx.Average value = (1/(b−a))·∫_a^b f(x) dx. This divides total area by the length of the interval.
The number that represents the exact signed area between y = x² and the x-axis from 0 to 3 is: — 27/3 = 9.∫₀^3 x² dx = [x³/3]₀^3 = 27/3 − 0 = 9. Options A and D are equivalent.
∫3x²(x³+1)⁴ dx = ? — (x³+1)⁵/5 + C.u = x³+1, du = 3x² dx. ∫u⁴ du = u⁵/5 + C = (x³+1)⁵/5 + C.
∫2xe^(x²) dx = ? — e^(x²) + C.u = x², du = 2x dx. ∫eᵘ du = eᵘ + C = e^(x²) + C.
∫cos(3x) dx = ? — sin(3x)/3 + C.u = 3x, du = 3 dx, so dx = du/3. ∫cos(u)(du/3) = (1/3)sin(u) + C = sin(3x)/3 + C.
∫sin(x²)·2x dx = ? — −cos(x²) + C.u = x², du = 2x dx. ∫sin(u) du = −cos(u) + C = −cos(x²) + C.
The area between f(x) = x and g(x) = x² from 0 to 1 is: — 1/6.f ≥ g on [0,1]. ∫₀^1 (x−x²) dx = [x²/2 − x³/3]₀^1 = 1/2 − 1/3 = 1/6.
To find area between two curves, we need to know where they intersect because: — The limits of integration are the intersection points.The intersection points determine the limits of integration [a,b] over which to compute ∫[f(x)−g(x)] dx.
∫e^(5x) dx = ? — e^(5x)/5 + C.u = 5x, du = 5 dx. ∫eᵘ du/5 = eᵘ/5 + C = e^(5x)/5 + C.
Area between y = sin x and x-axis from 0 to π: — 2.sin x ≥ 0 on [0,π]. ∫₀^π sin x dx = [−cos x]₀^π = −cos π + cos 0 = 1 + 1 = 2.
For definite integrals with u-sub, we can convert limits. For ∫₀^1 2x(x²+1)³ dx with u=x²+1: — New limits: u(0)=1 to u(1)=2.u = x² + 1: when x=0, u=1; when x=1, u=2. New integral: ∫₁^2 u³ du.
Which integral requires a different method than u-substitution? — ∫x·sin(x) dx.∫x sin(x) dx is a product of two unrelated functions — it requires integration by parts, not u-substitution.
∫ 2x/(x²+3) dx = ? — ln(x²+3) + C.u = x²+3, du = 2x dx. ∫du/u = ln|u| + C = ln(x²+3) + C.
∫x eˣ dx: using IBP with u = x, dv = eˣ dx gives: — xeˣ − eˣ + C.u=x, v=eˣ, du=dx. ∫x eˣ dx = x·eˣ − ∫eˣ dx = xeˣ − eˣ + C = eˣ(x−1) + C.
∫x sin x dx: using u=x, dv=sin x dx: — −x cos x + sin x + C.u=x, v=−cos x. ∫x sin x dx = x·(−cos x) − ∫(−cos x) dx = −x cos x + sin x + C.
∫ln x dx: use u = ln x, dv = dx: — x ln x − x + C.u=ln x, v=x. ∫ln x dx = x·ln x − ∫x·(1/x) dx = x ln x − ∫1 dx = x ln x − x + C.
For ∫x²eˣ dx, IBP must be applied: — Twice.Each IBP reduces the polynomial power by 1. x² needs to reach x⁰ (constant), requiring 2 applications.
Integration by parts is derived from the: — Product rule d(uv) = u dv + v du.d(uv) = u dv + v du. Integrate both sides: uv = ∫u dv + ∫v du. Rearrange: ∫u dv = uv − ∫v du.
∫x cos x dx = ? — x sin x + cos x + C.u=x, dv=cos x dx, v=sin x. ∫x cos x dx = x sin x − ∫sin x dx = x sin x + cos x + C.
When should you choose dv = eˣ dx rather than u = eˣ? — When no LIATE option is higher priority than exponential.By LIATE, eˣ is last priority for u. So eˣ becomes dv unless the other factor is also exponential (same priority).
∫ x^n·eˣ dx requires n IBP applications. For n=4: — 4 applications.Each IBP reduces the power of x by 1. For x⁴, we need 4 applications to reach x⁰.
The "cyclic trick" in IBP occurs when: — The second IBP reproduces the original integral.For ∫eˣ sin x dx, two IBP steps return −I, giving I = ∫eˣ sin x dx = eˣ(sin x − cos x)/2 + C.
Which integral can be solved by u-sub alone (no IBP)? — ∫x·e^(x²) dx.∫x·e^(x²) dx: u = x², du = 2x dx. Direct u-sub works. The others need IBP.