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sin(2t) =
2 sin(t) cos(t)
used to cancel terms in the denominator w/ tan(t) or sec(t)
cos(2t) =
cos2(t) - sin2(t)
2 cos2(t) - 1
1 - 2 sin2(t)
used to rewrite terms before integrating
sin²(t) =
1 - cos(2t) / 2
used when integral has a squared term in it
cos²(t) =
1 + cos(2t) / 2
used when integral has asquared term in it
tan(t) =
sin(t) / cos(t)
sec(t) =
1 / cos(t)
csc(t) =
1 / sin(t)
cot(t) =
cos(t) / sin(t)
cos²(t) + sin²(t) =
1
1 + tan²(t) =
sec²(t)
y
Y
y’
sY - y(0)
y’’
s²Y - sy(0) - y’(0)
f(t) = 1
F(s) = 1 / s
f(t) = t
F(s) = 1 / s²
f(t) = tn
F(s) = n! / sn+1
f(t) = eat
F(s) = 1 / s - a
f(t) = sin(at)
F(s) = a / s2 + a2
f(t) = cos(at)
F(s) = s / s2 + a2
f(t) = eat cos(bt)
F(s) = s - a / (s - a)2 + b2
f(t) = eat sin(bt)
F(s) = b / (s - a)2 + b2
f(t) = tn eat
F(s) = n! / (s - a)n+1
g(t) =
(first rule) + uc(t)(second rule - first rule)
Wronskian =
y1 y’2 - y’1 y2
λ1, λ2 < 0
stable node and asymptotically stable
λ1, λ2 > 0
unstbale node and unstable
λ1 < 0 < λ2
saddle point and unstable
𝛼 = 0, β does not equal 0, λ = 𝛼 +— βi
center and stable but NOT asymptotically
𝛼 > 0, β does not equal 0, λ = 𝛼 + βi
source and unstable
𝛼 < 0, β does not equal 0, λ = 𝛼 + βi
sink and asymptoticlaly stable
λ < 0 (defective)
stable improper node and symptotically stable
λ > 0 (defective)
unstable improper node and unstable