Ya resolvimos la ecuación de calor en un anillo unidimensional donde utilizamos las series de Fourier. Sin embargo, otro caso importante es aquel donde el espacio es ilimitado de -infinito a infnito. En este caso se tiene que utilizar la transformada de Fourier para resolver la ecuación. Su definición y sus propiedades, las pueden encontrar en las siguientes notas actualizadas. Notas actualizadas
Hola todos, aquí les tengo la liga para una nueva versión de nuestros notas de curso. Incluyen un breve resumen sobre la teoría del grupo simétrico -- mas o menos hasta donde lo necesitarémos para trabajar con el cubo de Rubik: Lecture Notes (pág. 24-26). Leanlo, e intentan contestar las preguntas y hacer los ejercisios.
a) z'=z_1*z_2
ResponderBorrarz'=(x_1 + i y_1)*(x_2+iy_2)
z'=x_1*x_2 +i(x_1*y_2) +i(x_2*y_1) + i^2*y_1*y_2
z'=(x_1*x_2 - y_1*y_2) + i(x_1*y_2 +x_2*y_1)
Bien!
Borrarb) z'= z_1/z_2
ResponderBorrarz'= x_1+iy_1/(x_2+iy_2)
z'= (x_1+iy_1)/(x_2+iy_2)*[(x_2 -iy_2)/(x_2-iy_2)]
z'= (x_1*x_2 +y_1*y_2 + i(x_2*y_1 - x_1*y_2))/(x_2^2 + y_2^2)
z'=[(x_1*x_2 + y_1*y_2)/(x_2^2 + y_2^2)] +i[(x_2*y_1 - x_1*y_2)/(x_2^2 + y_2^2)]
Bien!
Borrarc) |z|=sqrt(x^2+y^2) ; \theta= arctan(y/x)
ResponderBorrarz_1=1 + i
|z_1|= sqrt(1+1)= sqrt(2)
\theta_1= arctan(1)= pi/4
z_1= sqrt(2)*exp(i*pi/4)= sqrt(2)*(cos(pi/4) + isen(pi/4))
z_2= -1 + i
|z_2|=sqrt(2)
\theta_2 = pi - arctan(1) = pi - pi/4 = 3pi/4
z_2= sqrt(2)*exp(i*3pi/4)= sqrt(2)*(cos(3pi/4) +isen(3pi/4))
z_3= - 1 - i
|z_3|=sqrt(2)
\theta_3= pi + arctan(1)= pi + pi/4= 5pi/4
z_3=sqrt(2)*exp(i*5pi/4)=sqrt(2)*(cos(5pi/4) + isen(5pi/4))
z_4= 1 + isqrt(3)
|z_4|= sqrt(4)= 2
\theta_4= arctan(sqrt(3)) = pi/3
z_4= 2*exp(i*pi/3)=2*(cos(pi/3) + isen(pi/3))
z_5= -1 -isqrt(3)
|z_5|=2
\theta_5= pi + arctan(sqrt(3))= pi + pi/3 = 4pi/3
z_5= 2*exp(i*4pi/3)=2*(cos(4pi/3) + isen(4pi/3))
z_6= sqrt(3) - i
|z_6|=2
\theta_6= 2pi- arctan(1/sqrt(3))= 2pi - pi/6= 11pi/6
z_6= 2*exp(i*11pi/6)= 2*(cos(11pi/6) + isen(pi/6))
z_7= 2 + sqrt(3) + i
|z_7|=sqrt( (2+sqrt(3))^2 +1)= sqrt(4+3+4*sqrt(3) +1)=sqrt(8 +4*sqrt(3))= 2*sqrt(2+sqrt(3))
\theta_7= arctan(1/(2 + sqrt(3)))= arctan([1/(2+sqrt(3)]*[(2-sqrt(3))/(2-sqrt(3))])=arctan(2-sqrt(3))
z_7=2*sqrt(2+sqrt(3))*exp(i*arctan(2-sqrt(3))=2*sqrt(2+sqrt(3))*(cos(arctan(2-sqrt(3)) + isen(arctan(2-sqrt(3))
Caracoles
BorrarMadre de cristo no vi que esto era de tarea!
BorrarAquí van:
A) z' = z_1*z_2 = (x_1+iy_1)(x_2+iy_2) = (x_1x_2 - y_1y_2) + i(x_1y_2 + x_2y_1)
B) z' = z_1 / z_2 = (x_1+iy_1) / (x_2+iy_2) = (x_1+iy_1) / [(x_2+iy_2) * (x_2-iy_2)] =
[(x_1+iy_1) * (x_2-iy_2)] / (x_2 ^2 + y_2 ^2) =
[x_1x_2+ y_1y_2 + i(x_2y_1 - x_1y_2)] / (x_2 ^2 + y_2 ^2)
C)
1) |z| = sqrt(1^2+1^2) = sqrt(2), phi = tan^-1 (1) = pi/4 -> sqrt(2) e^i(pi/4)
2) |z| = sqrt((-1)^2+1^2) = sqrt(2), phi = pi - tan^-1 (1) = 3pi/4 -> sqrt(2) e^i(3pi/4)
3) |z| = sqrt((-1)^2+(-1)^2) = sqrt(2), phi = pi + tan^-1 (1) = 5pi/4 -> sqrt(2) e^i(5pi/4)
4) |z| = sqrt(1^2+sqrt(3)^2) = 2, phi = tan^-1 (sqrt (3)) = pi/3 -> 2*e^i(pi/3)
5) |z| = sqrt((-1)^2+(-sqrt(3))^2) = 2, phi = pi + tan^-1 (sqrt (3)) = 4pi/3 -> 2*e^i(4pi/3)
6) |z| = sqrt((-1)^2+sqrt(3)^2) = 2, phi = 2pi - tan^-1 (1/sqrt (3)) = 2pi - pi/6 = 11pi/6
-> 2*e^i(11pi/6)
7) |z| = sqrt(1^2+sqrt(2+sqrt(3)) ^2) = 2sqrt (2+sqrt(3)),
phi = tan^-1 (1/ sqrt(2+sqrt(3))) = 5pi/12 -> 2sqrt (2+sqrt(3))*e^i(5pi/12)
a)
ResponderBorrarz_1 z_2 = (x_1 + iy_1)(x_2 + iy_2)
z_1 z_2 = (x_1 x_2 - y_1 y_2) + i(x_1 y_2 + x_2 y_1)
b)
\frac{z_1}{z_2} = \frac{(x_1 + iy_1)}{(x_2 + iy_2)}
\frac{z_1}{z_2} = \frac{(x_1 + iy_1)(x_2 - iy_2)} {(x_2 + iy_2)(x_2 - iy_2)}
\frac{z_1}{z_2} = \frac{(x_1 x_2 + y_1 y_2) + i(x_1 y_2 + x_2 y_2)} {(x_2^2 + y_2^2)}
c)
1. \sqrt{2} e^{i\frac{\pi}{4}}
2. \sqrt{2} e^{i\frac{3 \pi}{4}}
3. \sqrt{2} e^{i\frac{5 \pi}{4}}
4. 2 e^{i \arctan{\sqrt{3}}}
5. 2 e^{i (\pi + \arctan{\sqrt{3}} ) }
6. 2 e^{i (\frac{3 \pi}{2} + \arctan{\sqrt{3}} ) }
7. \sqrt{8+4\sqrt{3}} e^{i \arctan{\sqrt{2 + \sqrt{3}}}}
a) z' = z_1 * z_2
ResponderBorrar= (x_1 + i y_1) * (x_2 + i y_2)
= (x_1*x_2 - y_1*y_2) + i ( x_1*y_2 + x_2*y_1)
b) z' = z_1/z_2
= ((x_1 + i y_1) / (x_2 + i y_2)) * (x_2 - i y_2) / (x_2 - i y_2)
= (x_1 * x_2 + y_1 * y_2)/(x_2^2 + y_2^2) + i (y_1 * x_2 - x_1 * y_2)/(x_2^2 + y_2^2)
c)
1) 1 + i = sqrt(2) * exp(i * pi/4)
2) -1 + i = sqrt(2) * exp(i *3pi/4 )
3) -1- i = sqrt(2)* exp(i * 5pi/4)
4) 1 + i*sqrt(3) = 2 * exp(i * pi/3)
5) -1 - i*sqrt(3) = 2 * exp(i * 4pi/3)
6) sqrt(3) - i = 2 * exp(i * 11pi/6)
7) 2 + sqrt(3) + i = 2 * sqrt (2 + sqrt(3)) * exp(i * pi/6)
PUBLICACIÓN ATRASADA:
ResponderBorrar(a)
z'=z1*z2=(x1+iy1)*(x2+iy2)=x1*x2+ix1*y2+ix2*y1-y1*y2
=(x1x2-y1y2)+i(x1y2+x2y1)
(b)
z'=(x1+iy1)/(x2+iy2)=((x1+iy1)/(x2+iy2))*((x2-iy2)/(x2-iy2))=(x1x2-ix1y2+ix2y1+y1y2)/(x2^2-ix2y2+ix2y2+y2^2)
=((x1x2+y1y2)/(x2^2+y2^2))+i((x2y1-x1y2)/(x2^2+y2^2))
(c)
(1) phi=pi/4, |z|=sqrt(2)
z=sqrt(2)*exp(ipi/4)=sqrt(2)*(cos(pi/4)+isin(pi/4))
(2) phi=3*pi/4, |z|=sqrt(2)
z=sqrt(2)*exp(i3pi/4)=sqrt(2)*(cos(3*pi/4)+isin(3*pi/4)
(3) phi=-3*pi/4, |z|=sqrt(2)
z=sqrt(2)*exp(-i3pi/4)=sqrt(2)*(cos(3pi/4)+isin(3pi/4))
(4) phi=pi/3, |z|=2
z=2*exp(ipi/3)=2*(cos(pi/3)+isin(pi/3)
(5) phi=-2pi/3, |z|=2
z=2*exp(-i2pi/3)=2*(cos(2pi/3)-isin(2pi/3)
(6) phi=-pi/6, |z|=2
z=2*exp(-ipi/6)=2*(cos(pi/6)-isin(pi/6)
(7) phi=pi/12, |z|=2*sqrt(2+sqrt(3))
z=2*sqrt(2+sqrt(3))*exp(ipi/12)=2*sqrt(2+sqrt(3))*(cos(pi/12)+isin(pi/12))
a)
ResponderBorrar$z' = z_1 * z_2$\\
$= (x_1 + i y_1)*(x_2 + i y_2)$\\
$= (x_1*x_2 - y_1*y_2) + i ( x_1*y_2 + x_2*y_1)$
b)
$z' = z_1/z_2$\\
$= ((x_1 + i y_1) / (x_2 + i y_2)) * (x_2 - i y_2) / (x_2 - i y_2)$\\
$= (x_1 * x_2 + y_1 * y_2)/(x_2^2 + y_2^2) + i (y_1 * x_2 - x_1 * y_2)/(x_2^2 + y_2^2)$\\
c)
$z_1 = \sqrt{2} * \exp^{(i* \pi/4)}$\\
$z_2 = \sqrt{2} * \exp^{(i *3 \pi/4 )}$\\
$z_3 = \sqrt{2}* \exp^{(i * 5 \pi/4)}$\\
$z_4 = 2 * \exp^{(i * \pi/3)}$\\
$z_5= 2 * \exp^{(i * 4\pi/3)}$\\
$z_6 = 2 * \exp^{(i * 11\pi/6)}$\\
$z_7 =2* \sqrt{(2+\sqrt{3})} * \exp^{(i*\arctan {(2-\sqrt{3})}}$\\
a) z' = z_{1} * z_{2} = (x_{1} + iy_{1}) * (x_{2} + iy_{2})
ResponderBorrar= x_{1} * x_{2} + i( x_{1} * y_{2} + x_{2} * y_{1}) - y_{1} * y_{2}.
b) z' = \frac{ z_{1} }{ z_{2} } = \frac{ x_{1} + iy_{1} }{ x_{2} + iy_{2} }
= (\frac{ x_{1} + iy_{1} }{ x_{2} + iy_{2} } ) * ( \frac{ x_{2} - iy_{2} }{ x_{2} - iy_{2} } )
= \ frac{ x_{1} * x_{2} + y_{1} * y_{2} }{ x_{2}^{2} + y_{2}^{2} }
+ i * \frac{ x_{2} * y_{1} - x_{1} * y_{2} }{ x_{2}^{2} + y_{2}^{2} }
c) En forma polar: , si \theta = arctan \frac{y}{x}
(1) => \sqrt{2} * e^i{\pi/4} = \sqrt{2} * ( \cos{\pi/4} + i * \sin{\pi/4} )
(2) => \sqrt{2} * e^i{3 * \pi/4} = \sqrt{2} * ( \cos{3*\pi/4} + i * \sin{3*\pi/4} )
(3) => \sqrt{2} * e^i{5 * \pi/4} = \sqrt{2} * ( \cos{5*\pi/4} + i * \sin{5*\pi/4} )
(4) => 2 * e^i{\pi/3} = 2 * ( \cos{\pi/3} + i * \sin{\pi/3} )
(5) => 2 * e^i{4 * \pi/3} = 2 * ( \cos{4 * \pi/3} + i * \sin{4 * \pi/3} )
(6) => 2 * e^i{11* \pi/6} = 2 * ( \cos{11 * \pi/6} + i * \sin{11* \pi/6} )
(7) => 2 * \sqrt{ 2 + \sqrt{3} } * e^i{\pi/12} = 2 * \sqrt{ 2 + \sqrt{3} } * ( \cos{ \pi/12} + i * \sin{ \pi/12} )