∫du=u+C
∫undu=un+1n+1+C,n≠−1
∫duu=ln|u|+C
∫eudu=eu+C
∫audu=aulna+C
∫sinudu=−cosu+C
∫cosudu=sinu+C
∫tanudu=−ln|cosu|+C
∫cotudu=ln|sinu|+C
∫secudu=ln|secu+tanu|+C
∫cscudu=−ln|cscu+cotu|+C
∫du√a2−u2=sin−1ua+C
∫dua2+u2=1atan−1ua+C
∫duu√u2−a2=1asec−1|ua|+C
A **Riemann Sum** is a rectangular approximation method where you DO NOT EVALUATE THE INTEGRAL, but sum the areas of the rectangles.
For uneven intervals, calculate one trapezoid at a time:
Atrap=12h(b1+b2)
For even intervals:
∫baf(x)dx=b−a2n[y0+2y1+2y2+⋯+2yn−1+yn]
If f(x) is continuous on [a,b], then there exists a number x=c such that:
favg=1b−a∫baf(x)dx
This value f(c) represents the **average value** of the function on [a,b].
x(t) = position function
v(t) = velocity function
a(t) = acceleration function
The derivative of position is velocity: v(t)=x′(t).
The derivative of velocity is acceleration: a(t)=v′(t).
Displacement:
∫tft0v(t)dt
Distance:
∫final timeinitial time|v(t)|dt
Average Velocity:
Average Velocity=Final position−Initial positionTotal time=ΔxΔt
The total amount F(x) at any time x is given by:
F(x)=f(a)+∫xaf′(t)dt
∫baf(x)dx=F(b)−F(a)
Where F′(x)=f(x).
ddx∫g(u)af(t)dt=f(g(u))dudx