To finalize one even more interesting finding:
Here is probably well known feature, anyway interesting value of W:
W( -ln( ((e^I)/I) ^ (I/(e^I))) = ((pi/2)-1)*I = lnI - I=lnI-ln(e^-I)=ln(I*e^I)
W(-ln(((I*e^-I)^(1/(I*e^-I) = -((pi/2)-1)*I = (1-pi/2)*I = -lnI+I= -lnI+ln(e^I)= ln((e^I)/I)
correspondingly:
h( ((e^I)/I) ^ (I/(e^I))) = -I* e^I = sin1-I*cos1
h((I*(e^-I)^(1/I*(e^-I))= I*e^-I = -sin(-1)+I*cos1
and also :
-I*e^I= e^((-pi/2)I+I)= e^(1-pi/2)*I
I*e^-I=e^((pi/2)*I-I)=e^(pi/2-1)*I
are rather specific rotations in complex plane.
Ivars
Here is probably well known feature, anyway interesting value of W:
W( -ln( ((e^I)/I) ^ (I/(e^I))) = ((pi/2)-1)*I = lnI - I=lnI-ln(e^-I)=ln(I*e^I)
W(-ln(((I*e^-I)^(1/(I*e^-I) = -((pi/2)-1)*I = (1-pi/2)*I = -lnI+I= -lnI+ln(e^I)= ln((e^I)/I)
correspondingly:
h( ((e^I)/I) ^ (I/(e^I))) = -I* e^I = sin1-I*cos1
h((I*(e^-I)^(1/I*(e^-I))= I*e^-I = -sin(-1)+I*cos1
and also :
-I*e^I= e^((-pi/2)I+I)= e^(1-pi/2)*I
I*e^-I=e^((pi/2)*I-I)=e^(pi/2-1)*I
are rather specific rotations in complex plane.
Ivars

