- #1
Leo Authersh
Where is my simplification wrong?
I wrote it based on the general formula for real numbers that ##((a)^b)^c = a^{bc}##BvU said:Do I distinguish a ##(-1)^{1/2} = -{1\over 2} ## in the first step ?
##(((64)^{1/2})^{-4})^ {1/2} = (64^{1/2})^{-4/2} = 1/64##mfb said:That formula is (a) problematic for complex numbers and (b) doesn't lead to -1/2 even if you apply it.
Hi,jbriggs444 said:When you replaced ##i^i## with ##{((-1)^{(1/2)})}^{((-1)^{(1/2)})}##, you forgot the parentheses around the "i" in the exponent.
Exponentiation is not associative. ##(a^b)^c## is not, in general, equal to ##a^{(b^c)}##.
jbriggs444 said:When you replaced ##i^i## with ##{((-1)^{(1/2)})}^{((-1)^{(1/2)})}##, you forgot the parentheses around the "i" in the exponent.
Exponentiation is not associative.
jbriggs444 said:All of which is irrelevant because your calculation does not have that form.
You misunderstand. It's not the -1 that's the problem. It's the parentheses.Leo Authersh said:And that is my question. Why the general formula becomes irrelevant when 4096 is replaced with -1.
Thank you. Now I understood why exponentials are not left associative. But since apparently they are all right associative, I'm confused because my simplification gives me the deception of being right associative.jbriggs444 said:You misunderstand. It's not the -1 that's the problem. It's the parentheses.
Edit:
##{(a^b)}^c## is equal to ##a^{(bc)}##
But obviously,
##a^{(b^c)}## is not equal to ##a^{(bc)}## [unless ##b^c## just happens to equal ##b \times c## or a just happens to be equal to 1]
Personally, I can never remember whether a tower of exponents is supposed to be evaluated from left to right or from right to left. I'm pretty sure that I've seen it both ways over the years. But it does not matter. If you are the one writing down the formula, you can use parentheses to be absolutely sure that it evaluates the way you want it to.Leo Authersh said:Thank you. Now I understood why exponentials are not left associative. But since apparently they are all right associative, I'm confused because my simplification gives me the deception of being right associative.
Now, I have understood. Thank you for your answers.mfb said:Where do you see something of the type of ##(a^b)^c## in ##(-1)^{1/2}##? What would a,b, and c be?
Conclusion -- When dealing with complex exponents, consider the complex exponential function.Svein said:Messing around with complex numbers - let's see: [itex] i=e^{i\frac{\pi}{2}}[/itex], so [itex]i^{i}=(e^{i\frac{\pi}{2}})^{i}=e^{i\frac{\pi}{2}\cdot i}=e^{i \cdot i\frac{\pi}{2}}=e^{-\frac{\pi}{2}} [/itex].
Svein said:Messing around with complex numbers - let's see: [itex] i=e^{i\frac{\pi}{2}}[/itex], so [itex]i^{i}=(e^{i\frac{\pi}{2}})^{i}=e^{i\frac{\pi}{2}\cdot i}=e^{i \cdot i\frac{\pi}{2}}=e^{-\frac{\pi}{2}} [/itex].
Good point. It's true that you need to define a branch of the logarithm. The principle branch being the most standard. So there are more than one answer to the question. But the answer given is definitely one possible answer.Infrared said:It's a little bit tricker than this: ##i=e^{\frac{5\pi}{2}i}## is also true and, following your steps, ##i^i=(e^{\frac{5\pi}{2}i})^i=e^{-\frac{5\pi}{2}}##. The issue is that it's hard to define exponentiation for complex numbers. We want to say ##z^w=\exp(w\log(z))## (for ##z\neq 0## of course), but how to define the complex logarithm? For ##z=re^{i\theta}##, we can't have ##\log(z)=\log(r)+i\theta## since ##\theta## is only defined up to a multiple of ##2\pi##, unless we restrict our allowed ##\theta##, say to be in ##[0,2\pi)##. But this makes ##\log## discontinuous and causes exponent rules to fail, as seen above.
Alternatively, you can just give up on ##\log## being a function, and instead have it be defined only up to multiples of ##2\pi i##. But then our exponential ##z^w=\exp(w\log(z))## becomes defined only up to factors of ##\exp(2\pi iw)##. With ##w=i##, we get back to the original problem.
This sort of problem leads to the theory of Riemann surfaces.
Yes, of course. But I just wanted to show that a purely imaginary exponent of a purely imaginary number has a real value. What you have done is to show that it has several real values, which is true for a rather large class of complex functions.Infrared said:It's a little bit tricker than this: ##i=e^{\frac{5\pi}{2}i}## is also true and, following your steps, ##i^i=(e^{\frac{5\pi}{2}i})^i=e^{-\frac{5\pi}{2}}##. The issue is that it's hard to define exponentiation for complex numbers. We want to say ##z^w=\exp(w\log(z))## (for ##z\neq 0## of course), but how to define the complex logarithm? For ##z=re^{i\theta}##, we can't have ##\log(z)=\log(r)+i\theta## since ##\theta## is only defined up to a multiple of ##2\pi##, unless we restrict our allowed ##\theta##, say to be in ##[0,2\pi)##. But this makes ##\log## discontinuous and causes exponent rules to fail, as seen above.
Alternatively, you can just give up on ##\log## being a function, and instead have it be defined only up to multiples of ##2\pi i##. But then our exponential ##z^w=\exp(w\log(z))## becomes defined only up to factors of ##\exp(2\pi iw)##. With ##w=i##, we get back to the original problem.
This sort of problem leads to the theory of Riemann surfaces.
A simplified imaginary unit to the power of imaginary unit is a mathematical expression of the form i^i, where i represents the imaginary unit (√-1). It is a complex number that has both a real and imaginary component.
To simplify i^i, we can use Euler's formula, e^(iπ/2), which converts the imaginary unit to a complex exponential. This can then be simplified further using logarithms to get a real number answer.
The value of i^i is approximately equal to 0.2079. This is the simplified form of the complex exponential e^(iπ/2).
Yes, an imaginary unit can be raised to an imaginary power. This results in a complex number with both real and imaginary components.
Simplified imaginary unit to the power of imaginary unit has various applications in mathematics, physics, and engineering. It is used in solving differential equations, analyzing electrical circuits, and understanding quantum mechanics.