TheNextFeliks
Veteran
Ok thanks.
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Solve for real values of x.
\( log_2(2^{x-1}+3^{x+1})=2x-log_2(3^x)
\)
It is... there's an answer. I know it but it requires fudging so im still trying to solve it properlywulfram says its not possible symbolically
wulfram says its not possible symbolically
this thread makes me feel like such an *****. lol
edit: seriously, i d i o t is censored? wow.
hear's my question for somepony two solve
pruf that \( \int_{-\infty}^{\infty} e^{\frac{-x^2}{2}}dx=\sqrt{2\pi} \)
Lol. I have proof:
Given circle with points (-1,0) and (1,0)
Prove that equation of circle is x^2-2yk+y^2=1 with center (0,k)
I know k must be 0 but I can't figure out how to prove it.
i dont know if youll like this ben:
d/dx erf(x)=2*Pi^(-0.5)*e^(-x^2)
d/dx erf(2^(-0.5)*x)=(2/Pi)^(0.5)*e^(-0.5*x^2)
erf(2^(-0.5)*t)=(2/Pi)^(0.5)* integral (0,t) [e^(-0.5*x^2)]dx
2*sqrt(Pi/2)* erf(2^(-0.5)*t)=2* integral (0,t) [e^(-0.5*x^2)]dx
sqrt(2*Pi)* erf(inf)=2* integral (0,inf) [e^(-0.5*x^2)]dx
sqrt(2*Pi)=integral (-inf,inf) [e^(-0.5*x^2)]dx
I am too lazy to try to type a complete proof on SS because mine is a bit long so I will skip obvious steps. Anyway, the easiest way to solve some problems it to think of a similar problem in an extra demension. In this case, z=e^(-x^2-y^2). If you find the volume under that surface at the verticies (±b,±b). it is
int([-b,b] e^(-x^2)dx)*int([-b,b] e^(-y^2)dy)=4*(int([0,b] e^(-x^2) dx))^2
V over the whole xy plane is V=lim(b->∞) 4(int([0,b] e^(-x^2) dx)^2= 4(int([0,∞] e^(-x^2) dx)^2
this can also be found in polar coordinates as V=lim(a->∞) int[0,2pi]int[0,a] (e^(-r^2)*r dr*dθ)=lim(a->∞) pi*(1-e^(-a^2))=pi
so 4(int([0,∞] e^(-x^2) dx)^2=pi
int([0,∞] e^(-x^2) dx=sqrt(pi)/2
int([-∞,∞] e^(-x^2) dx=sqrt(pi)
now u substitute u=x/sqrt(2) so
\( \int_{-\infty}^{\infty} e^{\frac{-x^2}{2}}dx=\sqrt{2\pi} \)
btw, how did you type your integral on SS. I'm curious.
(-1,0) and (1,0) centre (0,k) => radius = 1
x² + y² - 2yk = 1
x² + (y-k)² - k² = 1
x² + (y-k)² = 1+k²
1+k² = 1 => k = 0
what is this showing?