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d/dx(c)
0
d/dx(cx)
c
d/dx(tan x)
sec²x
d/dx(cot x)
-csc²x
d/dx(xⁿ)
nxⁿ⁻¹
d/dx(sec x)
sec x tan x
d/dx[f(x)g(x)]
f'g +g'f
d/dx(csc x)
-csc x cot x
d/dx(f/g)
(f'g-g'f)/g²
d/dx(sin⁻¹x)
1/√(1-x²)
d/dx(f(g(x))
f'(g(x))g'(x)
d/dx(cos⁻¹x)
-1/√(1-x²)
d/dx(sin x)
cos x
d/dx(cos x)
-sin x
d/dx(tan⁻¹x)
1/(1+x²)
d/dx(cot⁻¹x)
-1/(1+x²)
d/dx(csc⁻¹x)
1/|x|√(x²-1)
d/dx(sec⁻¹x)
-1/|x|√(x²-1)
d/dx(ln x)
1/x
d/dx(logₙx)
1/(ln n)x
d/dx(eˣ)
e^x
d/dx[aˣ]
(ln a)a^x
∫a dx
ax + C
∫xⁿ dx
xⁿ⁺¹/(n+1) +C
Integration by Parts
∫ u dv
uv- ∫v du
∫1/x dx
ln|x| +C
∫eˣ dx
eˣ+c
∫aˣ dx
a^x/(ln a) +c
∫sin x dx
-cos x +c
∫cos x dx
sin x +c
∫tan x dx
ln |sec x| +C
∫cot x dx
ln |sin x| +c
∫sec x dx
ln |sec x + tan x| +c
∫csc x dx
ln |csc x - cot x| + c
∫sec²x dx
tan x +c
∫csc²x dx
-cot x + c
∫sec x tan x dx
sec x + c
∫csc x cot x dx
-csc x + c
∫1/(x²+a²) dx
1/a(tan⁻¹(x/a)) +c
∫1/√(a²-x²) dx
sin⁻¹(x/a) + c
∫1/x√(x²-a²) dx
1/a(sec⁻¹|x/a|) + c
∫ln x dx
x ln x - x +c
√(a²-x²)
x=a sin θ
√(x²+a²)
x = a tan θ
√(x²-a²)
x = a sec θ
(use when power of cosine is odd) cos²x
1-sin²x, u=sin x
(use when power of sine is odd) sin²x
1-cos²x, u=cos x
(if both sin and cos have even powers) sin²x
1/2 -1/2(cos 2x)
(if both sin and cos have even powers) cos²x
1/2 +1/2(sin 2x)
trig identity sin x cos x
1/2 sin 2x
parametric dy/dx
dy/dt / dx/dt
parametric second derivative d²y/dx²
d/dx(dy/dx) / dx/dt
velocity vector v(t)
<x’(t), y’(t)>
acceleration vector a(t)
<x’’(t), y’’(t)>
parametric speed formula
√[(dy/dt)²+(dx/dt)²]
parametric arc length formula
∫ √[(dy/dt)²+(dx/dt)²] dt
Polar area
1/2 ∫r² dθ
polar derivative
dy = r' sin θ +r cos θ
dx = r' cos θ + r sin θ
polar x=
r cos θ
polar y=
r sin θ
r²
x²+y²
polar tan θ
y/x (sin x/cos x)
maclurin series e^x
1+x+ x²/2! + x³/3! + … + xⁿ/n!+…
maclurin series sin x
x- x³/3! +x⁵/5! -x⁷/7! +… + (-1)ⁿx²ⁿ⁺¹/(2n+1)!+…
maclurin series cos x
1- x²/2!+ x⁴/4! - x⁶/6! + … + (-1)ⁿx²ⁿ/(2n)!+…
maclurin series 1/(1-x)
1+x+x²+x³+…+ xⁿ+…
maclurin series ln(x+1)
x-x²/2+ x³/3- x⁴/4 +… + (-1)ⁿxⁿ/(2n)!+…
macurin series tan⁻¹ x
x- x³/3 +x⁵/5 -x⁷/7 +… + (-1)ⁿx²ⁿ⁺¹/(2n+1)+…
geometric series
a+ ar+ ar² +…+ arⁿ+…=∑arⁿ
diverge is |r| >= 1
converge is |r| <1
sum= a₁/(1-r)
harmonic series
∑1/n
always diverges
p-series
∑1/n^p
diverge if p<=1
converge if p>1
Nth Term Test (Divergence Test)
if lim(x→∞) aₙ ≠ 0, the series ∑aₙ diverges
limit= 0 does not mean converge, but keep testing
Telescoping series
Series such as (1- 1/2)+(1/2-1/3)+(1/3-1/4)+…
Collapses to one or the first few terms and this is the sum. Use a partial fraction to break down the telescoping series if necessary.
integral test
if ƒ is decreasing, continuous, and positive for x>=1 AND aₙ = f(x), then ∑aₙ and ∫(1→∞) f(x) dx either both converge or diverge.
The value of the integral is not the sum of the series
Alternating series test
if aₙ > 0, then the alternating series ∑(-1)ⁿaₙ converges if both of the both following conditions are satisfied
a) lim (n→∞) aₙ = 0 (Nth term test)
b) {aₙ} is decreasing
common alternators: (-1)ⁿ, (-1)ⁿ⁺¹, cos (πn)
direct comparison test
if aₙ>= 0 and bₙ>=0
a) if ∑bₙ converges and 0<= aₙ <= bₙ, then ∑aₙ converges
b) if ∑aₙ diverges and 0<=aₙ,<=bₙ, then ∑bₙ diverges
limit comparison test
if aₙ>=0 and bₙ>= 0, and lim(n→∞) aₙ/bₙ = L or lim(n→∞) bₙ/aₙ =L, where L is both positive and finite, then the two series ∑aₙ and ∑bₙ, either both converge or diverge
absolute convergence
If the series ∑|aₙ| converges then ∑aₙ also converges. Such a series is called absolutely convergent.
If the series ∑|aₙ| diverges and ∑aₙ converges, the series is conditionally convergent
ratio test
∑aₙ converges if lim(n→∞) |aₙ₊₁/aₙ|
root test
the series ∑aₙ converges if lim(n→∞) ⁿ√|aₙ|
Taylor polynomial Tₙ(x)
f(c) + f'(c)(x-c) + f''(c)/2! (x-c)² + … + fⁿ(c)/n! (x-c)ⁿ
Maclurin Polynomial Mₙ(x)
(Taylor polynomial where c=0)
f(0) + f'(0)x + f''(0)x²/2! + … + fⁿ(0)xⁿ/n!
Lagrange error bound
If a function ƒ is differentiable through order n+ in an interval containing the center x=c, then for each x=a in the interval, there exists a number x=z between and c such that Tₙ(x)= f(c ) +f'(c)(a-c) + f''(c)/2! (a-c)² +…+ fⁿ(c)/n! (a-c)ⁿ + Rₙ(a)
Rₙ(a)<=
<=|maxƒⁿ⁺¹(z)/(n+1)! (a-c)ⁿ⁺¹|
Alternating series error bound
Suppose an alternating series converges and that the series has a sum S, then |Rₙ|=
|S-Sₙ| <= |aₙ₊₁|
Power Series
∑aₙ(x-c)ⁿ is a power series centered at x=c, where c is a constant.
a) The series converges at x=c (ALL POWER SERIES CONVERGE AT THEIR CENTER)
the radius is 0
Power Series
∑aₙ(x-c)ⁿ is a power series centered at x=c, where c is a constant.
b) The series converges for all x
the radius is ∞
Power Series
∑aₙ(x-c)ⁿ is a power series centered at x=c, where c is a constant.
c) there exists an R>0 such that the series converges for |x-c| < R and diverges for |x-c| > R
the corresponding domain [(c-R, c+R)], is called the interval of convergence
Exponential growth
Dy/dx=
Y=
dy/dx= ky
y= Ce^kt
Logistic Models
Dy/dx=
Y=
dy/dx = k/L y(L-y) = ky(1-y/L)
y=L/1+Ce^-kt
Euler's method
x | y | dy/dx|(x,y) | ∆y= m∆x | y new = y+∆y
∆x= (b-a)/n
Separation of variables
put y with dy and x with dx then integrate
area under the curve
∫a→b f(x) dx or ∫a→b f(y) dy
Disk method
π∫a→b R² dx or dy
Washer method
π∫a→b R²-r² dx or dy
arc length
∫a→b √(1+(dy/dx)²) dx
cross section
∫a→b A(x) dx
cross section square
s²
cross section semicircle
1/2 πr²
cross section equilateral triangle
√3/4 s²
cross section isosceles right triangle
1/2 x²