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r²=
X²+Y²
Slope of polar curves: Dy/Dx=
(dy/dtheta)/(dx/dtheta)
The area of the region between the origin and the curve
A=int AtoB ½ r²dtheta
Area between polar curves
A=int AtoB ½ (r2²-r1²)dtheta
x=?
rcostheta
y=?
rsintheta
Displacement from t=a to t=b
(int AtoB v1(t) dt, int AtoB v2(t)dt)
Total distance traveled?
int AtoB sqrt((v1(t))²+(v2(t))²)dt
Speed of a vector
magnitude of V(t)= sqrt(V1²+v2²)
Arc length of a parametrized curve
int T1toT2 sqrt( (dy/dt)²+(dx/dt)²)dt
d²y/dx²=
(dy’/dt)/(dx/dt)
Remainder estimation theory
|Rn(x)|<=M((r^n+1*|x-a|^n+1)/(n+1)!)
1/(1-x)
series from 0 to infinity, x^n (|x|<1)
1/(1+x)
series from 0 to inf, -1^n x^n (|x|<1)
e^x
series from 0 to inf, (x^n/n!) (all real x)
Sin x
series from 0 to inf, -1^n ((x^(2n+1))/(2n+1)!) for all real x
cos x
series from 0 to inf, -1^n (x^(2n+1)/2n!, all real x
ln(1+x)
series from 1 to inf, -1^n-1 x^n/n (-1<x<=1)
tan^-1(x)
series from 0 to inf, -1^n (x^(2n+1)/2n+1, |x|<=1
what happens when L’hopitale reaches #/0 or 0/#
if numerator function approaches 0 then the limit is 0, if the denominator approaches 0 then the limit is infinity
fluid pressure
p(force per unit area) P=wh h=depth, w=weight density
force on one side
integral from 0 to H, (density)(one side of base)(height)
Hooke’s law
force=constant K(x)
Work(work)=int 0toH (Kx)dx
Length of a smooth curve
Int from AtoB sqrt(1+(dy/dx)²)dx
integrating cylindrical shells
int AtoB 2pi (shellradius)(shell height)dx
radius is the opposite axis we are revolving around
height is (upper curve-lower curve)
Area of a circle
A=piR²
A=pi(outer²-inner²)dx
Volume/washers
int AtoB pi(outer²-inner²) dx
half life
Ln(2)/k
average value over an interval
1/(b-a) int AtoB
revolved around a line y=k
upper and lower radius become k-r
areas between curves
A=int AtoB (f(x)-g(x)) dx
intersection points give limit of integration
right-left
sin(2x)
2sin(x)cos(x)
cos(2x)
cos²(x)-sin²(x)
2cos²(x)-1
1-2sin²(x)
sec²(x)
1+tan²(x)
csc²(x)
1+cot²(x)