Do the Taylor series of $sin x$ and $cos x$ depend on the identity $sin^2 x + cos^2 x =1$?

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I had this crazy idea trying to prove the Pythagorean trigonometric identity;$$sin^2x+cos^2x=1$$by squaring the infinite Taylor series of $sin x$ and $cos x$. But it came out quite beautiful, involving also a combinatorics identitie.
The proof:
$$sin x=fracx1-fracx^33!+fracx^55!-fracx^77!+...=sum_n=0^infty(-1)^nfracx^2n+1(2n+1)!\\sin^2x=x^2-x^4left (frac11!3!+frac13!1!right )+x^6left (frac11!5!+frac13!3!+frac15!1!right )-...\\cos x=1-fracx^22!+fracx^44!-fracx^66!+...=sum_n=0^infty(-1)^nfracx^2n(2n)!\\cos^2x!=!1!-!x^2left(!frac10!2!!+!frac12!0!!right)!+!x^4left(!frac10!4!!+!frac12!2!!+!frac14!0!!right)!-!x^6left(!frac10!6!!+!frac12!4!!+!frac14!2!!+!frac16!0!!right)!+...$$We should have shown that the series for both $sin x$ and $cos x$ converge absolutely (since we changed the arrangement), but it's obvious since the absolute value of all terms of $sin x+cos x$ add up to $e^x$.$$sin^2x+cos^2x=\=1-x^2left(frac10!2!-frac11!1!+frac12!0!right)+x^4left(frac10!4!-frac11!3!+frac12!2!-frac13!1!+frac14!0!right)-x^6left(frac10!6!-frac11!5!+frac12!4!-frac13!3!+frac14!2!-frac15!1!+frac16!0!right)+...=\\=1+sum_n=1^infty(-1)^nx^2nsum_k=0^2nfrac(-1)^kbinom2nk(2n)!$$
Since we can show easily that $sum_i=0^n(-1)^ibinomni=0$ by expanding $(1-1)^n$ using Binom's formula. So:$$sin^2x+cos^2x=1-0+0-0+...=1$$
I think it's beautiful. I just wanted to ask, do Taylor's series of those functions depend on this identity? Because if they do, the proof will be circular.
combinatorics trigonometry power-series taylor-expansion
add a comment |Â
up vote
22
down vote
favorite
I had this crazy idea trying to prove the Pythagorean trigonometric identity;$$sin^2x+cos^2x=1$$by squaring the infinite Taylor series of $sin x$ and $cos x$. But it came out quite beautiful, involving also a combinatorics identitie.
The proof:
$$sin x=fracx1-fracx^33!+fracx^55!-fracx^77!+...=sum_n=0^infty(-1)^nfracx^2n+1(2n+1)!\\sin^2x=x^2-x^4left (frac11!3!+frac13!1!right )+x^6left (frac11!5!+frac13!3!+frac15!1!right )-...\\cos x=1-fracx^22!+fracx^44!-fracx^66!+...=sum_n=0^infty(-1)^nfracx^2n(2n)!\\cos^2x!=!1!-!x^2left(!frac10!2!!+!frac12!0!!right)!+!x^4left(!frac10!4!!+!frac12!2!!+!frac14!0!!right)!-!x^6left(!frac10!6!!+!frac12!4!!+!frac14!2!!+!frac16!0!!right)!+...$$We should have shown that the series for both $sin x$ and $cos x$ converge absolutely (since we changed the arrangement), but it's obvious since the absolute value of all terms of $sin x+cos x$ add up to $e^x$.$$sin^2x+cos^2x=\=1-x^2left(frac10!2!-frac11!1!+frac12!0!right)+x^4left(frac10!4!-frac11!3!+frac12!2!-frac13!1!+frac14!0!right)-x^6left(frac10!6!-frac11!5!+frac12!4!-frac13!3!+frac14!2!-frac15!1!+frac16!0!right)+...=\\=1+sum_n=1^infty(-1)^nx^2nsum_k=0^2nfrac(-1)^kbinom2nk(2n)!$$
Since we can show easily that $sum_i=0^n(-1)^ibinomni=0$ by expanding $(1-1)^n$ using Binom's formula. So:$$sin^2x+cos^2x=1-0+0-0+...=1$$
I think it's beautiful. I just wanted to ask, do Taylor's series of those functions depend on this identity? Because if they do, the proof will be circular.
combinatorics trigonometry power-series taylor-expansion
add a comment |Â
up vote
22
down vote
favorite
up vote
22
down vote
favorite
I had this crazy idea trying to prove the Pythagorean trigonometric identity;$$sin^2x+cos^2x=1$$by squaring the infinite Taylor series of $sin x$ and $cos x$. But it came out quite beautiful, involving also a combinatorics identitie.
The proof:
$$sin x=fracx1-fracx^33!+fracx^55!-fracx^77!+...=sum_n=0^infty(-1)^nfracx^2n+1(2n+1)!\\sin^2x=x^2-x^4left (frac11!3!+frac13!1!right )+x^6left (frac11!5!+frac13!3!+frac15!1!right )-...\\cos x=1-fracx^22!+fracx^44!-fracx^66!+...=sum_n=0^infty(-1)^nfracx^2n(2n)!\\cos^2x!=!1!-!x^2left(!frac10!2!!+!frac12!0!!right)!+!x^4left(!frac10!4!!+!frac12!2!!+!frac14!0!!right)!-!x^6left(!frac10!6!!+!frac12!4!!+!frac14!2!!+!frac16!0!!right)!+...$$We should have shown that the series for both $sin x$ and $cos x$ converge absolutely (since we changed the arrangement), but it's obvious since the absolute value of all terms of $sin x+cos x$ add up to $e^x$.$$sin^2x+cos^2x=\=1-x^2left(frac10!2!-frac11!1!+frac12!0!right)+x^4left(frac10!4!-frac11!3!+frac12!2!-frac13!1!+frac14!0!right)-x^6left(frac10!6!-frac11!5!+frac12!4!-frac13!3!+frac14!2!-frac15!1!+frac16!0!right)+...=\\=1+sum_n=1^infty(-1)^nx^2nsum_k=0^2nfrac(-1)^kbinom2nk(2n)!$$
Since we can show easily that $sum_i=0^n(-1)^ibinomni=0$ by expanding $(1-1)^n$ using Binom's formula. So:$$sin^2x+cos^2x=1-0+0-0+...=1$$
I think it's beautiful. I just wanted to ask, do Taylor's series of those functions depend on this identity? Because if they do, the proof will be circular.
combinatorics trigonometry power-series taylor-expansion
I had this crazy idea trying to prove the Pythagorean trigonometric identity;$$sin^2x+cos^2x=1$$by squaring the infinite Taylor series of $sin x$ and $cos x$. But it came out quite beautiful, involving also a combinatorics identitie.
The proof:
$$sin x=fracx1-fracx^33!+fracx^55!-fracx^77!+...=sum_n=0^infty(-1)^nfracx^2n+1(2n+1)!\\sin^2x=x^2-x^4left (frac11!3!+frac13!1!right )+x^6left (frac11!5!+frac13!3!+frac15!1!right )-...\\cos x=1-fracx^22!+fracx^44!-fracx^66!+...=sum_n=0^infty(-1)^nfracx^2n(2n)!\\cos^2x!=!1!-!x^2left(!frac10!2!!+!frac12!0!!right)!+!x^4left(!frac10!4!!+!frac12!2!!+!frac14!0!!right)!-!x^6left(!frac10!6!!+!frac12!4!!+!frac14!2!!+!frac16!0!!right)!+...$$We should have shown that the series for both $sin x$ and $cos x$ converge absolutely (since we changed the arrangement), but it's obvious since the absolute value of all terms of $sin x+cos x$ add up to $e^x$.$$sin^2x+cos^2x=\=1-x^2left(frac10!2!-frac11!1!+frac12!0!right)+x^4left(frac10!4!-frac11!3!+frac12!2!-frac13!1!+frac14!0!right)-x^6left(frac10!6!-frac11!5!+frac12!4!-frac13!3!+frac14!2!-frac15!1!+frac16!0!right)+...=\\=1+sum_n=1^infty(-1)^nx^2nsum_k=0^2nfrac(-1)^kbinom2nk(2n)!$$
Since we can show easily that $sum_i=0^n(-1)^ibinomni=0$ by expanding $(1-1)^n$ using Binom's formula. So:$$sin^2x+cos^2x=1-0+0-0+...=1$$
I think it's beautiful. I just wanted to ask, do Taylor's series of those functions depend on this identity? Because if they do, the proof will be circular.
combinatorics trigonometry power-series taylor-expansion
combinatorics trigonometry power-series taylor-expansion
edited Aug 30 at 22:51
asked Sep 20 '16 at 21:11
76david76
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982214
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2 Answers
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up vote
6
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Nice proof! To address your question,
Do Taylor's series of those functions depend on this identity? Because if they do, the proof will be circular.
You are right to be worried about circularity! However, which concepts or theorems depend on which others is a matter of certain flexibility. Often, we take one thing to be the definition of a concept, and then have to prove the other properties as theorems -- but we could alternately have used some other property as a definition, and then the original definition would have to be a theorem.
Specific to your case, I have seen definitions of $sin$ and $cos$ where we start by defining $sin$ using arclength, then we define $cos x$ to satisfy $cos^2 x + sin^2 x = 1$. If we take this approach, certainly, there is nothing to prove. However, this is not the only possible approach! It is also common to define $sin$ and $cos$ using their Taylor series. Under this approach, you have given a very nice proof that $sin^2 x + cos^2 x = 1$.
Your proof could also be valid if we define $sin$ and $cos$ to be a basis of functions satisfying $f''(x) = -f(x)$.
In summary, it depends on what you define $sin$ and $cos$ to be; however, your proof is not necessarily circular. And it is a nice example of deriving a result about some functions from their Taylor series.
1
Thanks for this answer, but what about the usual definition of $sin$ and $cos$, as the proportion of sides of a triangle, that of course also doesn't depend on $sin^2x+cos^2x=1$, am I right?
â 76david76
Sep 20 '16 at 22:17
3
@76david76: Are $sin$ and $cos$ usually defined that way? That's often the way they're introduced, but then what is $sin 3pi/2$?
â Brian Tung
Sep 20 '16 at 22:31
1
It can be an expansion of the first definition. Is there really no way to define these functions out of the unit circle?
â 76david76
Sep 20 '16 at 22:49
2
@76david76 Most functions in analysis are not defined using geometry because we would first need a rigorous definition of points, lines, and so on. It is much easier to define them using taylor series. However, yes, you can develop these functions using the unit circle. When I said "we start by defining sinsin using arclength", that is referring to how we let $sin theta$ be the $y$-coordinate of the point on the unit circle such that the arc length from $(1,0)$ is $2 pi y$. If you define them using the unit circle, $cos^2 theta + sin62 theta$ is immediate like I said.
â 6005
Sep 20 '16 at 23:11
add a comment |Â
up vote
2
down vote
You are just showing that the Pythagorean theorem is a consequence of some property of the (complex) exponential function, there is no circularity in such argument. For instance, we may define, for any $zinmathbbC$,
$$ f(z)=e^z=sum_ngeq 0fracz^nn! tag1$$
and prove through a combinatorial argument that such a function fulfills $e^zcdot e^w=e^z+w$.
Since the Taylor coefficients at $0$ of such analytic function are real, we have $f(barz)=overlinef(z)$,
hence for any $rhoinmathbbR$
$$ left| e^irhoright| = e^irhocdot e^-irho = e^0 = 1. tag2$$
If we define $cos(rho)$ and $sin(rho)$ as the real/imaginary part of $e^irho$, we get that
$$ sin(rho)=sum_ngeq 0frac(-1)^n rho^2n+1(2n+1)!,qquad cos(rho)=sum_ngeq 0frac(-1)^n rho^2n(2n)!tag3 $$
and $(2)$ can be read as:
$$ sin^2(rho)+cos^2(rho) = 1.tag4$$
add a comment |Â
2 Answers
2
active
oldest
votes
2 Answers
2
active
oldest
votes
active
oldest
votes
active
oldest
votes
up vote
6
down vote
accepted
Nice proof! To address your question,
Do Taylor's series of those functions depend on this identity? Because if they do, the proof will be circular.
You are right to be worried about circularity! However, which concepts or theorems depend on which others is a matter of certain flexibility. Often, we take one thing to be the definition of a concept, and then have to prove the other properties as theorems -- but we could alternately have used some other property as a definition, and then the original definition would have to be a theorem.
Specific to your case, I have seen definitions of $sin$ and $cos$ where we start by defining $sin$ using arclength, then we define $cos x$ to satisfy $cos^2 x + sin^2 x = 1$. If we take this approach, certainly, there is nothing to prove. However, this is not the only possible approach! It is also common to define $sin$ and $cos$ using their Taylor series. Under this approach, you have given a very nice proof that $sin^2 x + cos^2 x = 1$.
Your proof could also be valid if we define $sin$ and $cos$ to be a basis of functions satisfying $f''(x) = -f(x)$.
In summary, it depends on what you define $sin$ and $cos$ to be; however, your proof is not necessarily circular. And it is a nice example of deriving a result about some functions from their Taylor series.
1
Thanks for this answer, but what about the usual definition of $sin$ and $cos$, as the proportion of sides of a triangle, that of course also doesn't depend on $sin^2x+cos^2x=1$, am I right?
â 76david76
Sep 20 '16 at 22:17
3
@76david76: Are $sin$ and $cos$ usually defined that way? That's often the way they're introduced, but then what is $sin 3pi/2$?
â Brian Tung
Sep 20 '16 at 22:31
1
It can be an expansion of the first definition. Is there really no way to define these functions out of the unit circle?
â 76david76
Sep 20 '16 at 22:49
2
@76david76 Most functions in analysis are not defined using geometry because we would first need a rigorous definition of points, lines, and so on. It is much easier to define them using taylor series. However, yes, you can develop these functions using the unit circle. When I said "we start by defining sinsin using arclength", that is referring to how we let $sin theta$ be the $y$-coordinate of the point on the unit circle such that the arc length from $(1,0)$ is $2 pi y$. If you define them using the unit circle, $cos^2 theta + sin62 theta$ is immediate like I said.
â 6005
Sep 20 '16 at 23:11
add a comment |Â
up vote
6
down vote
accepted
Nice proof! To address your question,
Do Taylor's series of those functions depend on this identity? Because if they do, the proof will be circular.
You are right to be worried about circularity! However, which concepts or theorems depend on which others is a matter of certain flexibility. Often, we take one thing to be the definition of a concept, and then have to prove the other properties as theorems -- but we could alternately have used some other property as a definition, and then the original definition would have to be a theorem.
Specific to your case, I have seen definitions of $sin$ and $cos$ where we start by defining $sin$ using arclength, then we define $cos x$ to satisfy $cos^2 x + sin^2 x = 1$. If we take this approach, certainly, there is nothing to prove. However, this is not the only possible approach! It is also common to define $sin$ and $cos$ using their Taylor series. Under this approach, you have given a very nice proof that $sin^2 x + cos^2 x = 1$.
Your proof could also be valid if we define $sin$ and $cos$ to be a basis of functions satisfying $f''(x) = -f(x)$.
In summary, it depends on what you define $sin$ and $cos$ to be; however, your proof is not necessarily circular. And it is a nice example of deriving a result about some functions from their Taylor series.
1
Thanks for this answer, but what about the usual definition of $sin$ and $cos$, as the proportion of sides of a triangle, that of course also doesn't depend on $sin^2x+cos^2x=1$, am I right?
â 76david76
Sep 20 '16 at 22:17
3
@76david76: Are $sin$ and $cos$ usually defined that way? That's often the way they're introduced, but then what is $sin 3pi/2$?
â Brian Tung
Sep 20 '16 at 22:31
1
It can be an expansion of the first definition. Is there really no way to define these functions out of the unit circle?
â 76david76
Sep 20 '16 at 22:49
2
@76david76 Most functions in analysis are not defined using geometry because we would first need a rigorous definition of points, lines, and so on. It is much easier to define them using taylor series. However, yes, you can develop these functions using the unit circle. When I said "we start by defining sinsin using arclength", that is referring to how we let $sin theta$ be the $y$-coordinate of the point on the unit circle such that the arc length from $(1,0)$ is $2 pi y$. If you define them using the unit circle, $cos^2 theta + sin62 theta$ is immediate like I said.
â 6005
Sep 20 '16 at 23:11
add a comment |Â
up vote
6
down vote
accepted
up vote
6
down vote
accepted
Nice proof! To address your question,
Do Taylor's series of those functions depend on this identity? Because if they do, the proof will be circular.
You are right to be worried about circularity! However, which concepts or theorems depend on which others is a matter of certain flexibility. Often, we take one thing to be the definition of a concept, and then have to prove the other properties as theorems -- but we could alternately have used some other property as a definition, and then the original definition would have to be a theorem.
Specific to your case, I have seen definitions of $sin$ and $cos$ where we start by defining $sin$ using arclength, then we define $cos x$ to satisfy $cos^2 x + sin^2 x = 1$. If we take this approach, certainly, there is nothing to prove. However, this is not the only possible approach! It is also common to define $sin$ and $cos$ using their Taylor series. Under this approach, you have given a very nice proof that $sin^2 x + cos^2 x = 1$.
Your proof could also be valid if we define $sin$ and $cos$ to be a basis of functions satisfying $f''(x) = -f(x)$.
In summary, it depends on what you define $sin$ and $cos$ to be; however, your proof is not necessarily circular. And it is a nice example of deriving a result about some functions from their Taylor series.
Nice proof! To address your question,
Do Taylor's series of those functions depend on this identity? Because if they do, the proof will be circular.
You are right to be worried about circularity! However, which concepts or theorems depend on which others is a matter of certain flexibility. Often, we take one thing to be the definition of a concept, and then have to prove the other properties as theorems -- but we could alternately have used some other property as a definition, and then the original definition would have to be a theorem.
Specific to your case, I have seen definitions of $sin$ and $cos$ where we start by defining $sin$ using arclength, then we define $cos x$ to satisfy $cos^2 x + sin^2 x = 1$. If we take this approach, certainly, there is nothing to prove. However, this is not the only possible approach! It is also common to define $sin$ and $cos$ using their Taylor series. Under this approach, you have given a very nice proof that $sin^2 x + cos^2 x = 1$.
Your proof could also be valid if we define $sin$ and $cos$ to be a basis of functions satisfying $f''(x) = -f(x)$.
In summary, it depends on what you define $sin$ and $cos$ to be; however, your proof is not necessarily circular. And it is a nice example of deriving a result about some functions from their Taylor series.
answered Sep 20 '16 at 21:30
6005
35.1k750124
35.1k750124
1
Thanks for this answer, but what about the usual definition of $sin$ and $cos$, as the proportion of sides of a triangle, that of course also doesn't depend on $sin^2x+cos^2x=1$, am I right?
â 76david76
Sep 20 '16 at 22:17
3
@76david76: Are $sin$ and $cos$ usually defined that way? That's often the way they're introduced, but then what is $sin 3pi/2$?
â Brian Tung
Sep 20 '16 at 22:31
1
It can be an expansion of the first definition. Is there really no way to define these functions out of the unit circle?
â 76david76
Sep 20 '16 at 22:49
2
@76david76 Most functions in analysis are not defined using geometry because we would first need a rigorous definition of points, lines, and so on. It is much easier to define them using taylor series. However, yes, you can develop these functions using the unit circle. When I said "we start by defining sinsin using arclength", that is referring to how we let $sin theta$ be the $y$-coordinate of the point on the unit circle such that the arc length from $(1,0)$ is $2 pi y$. If you define them using the unit circle, $cos^2 theta + sin62 theta$ is immediate like I said.
â 6005
Sep 20 '16 at 23:11
add a comment |Â
1
Thanks for this answer, but what about the usual definition of $sin$ and $cos$, as the proportion of sides of a triangle, that of course also doesn't depend on $sin^2x+cos^2x=1$, am I right?
â 76david76
Sep 20 '16 at 22:17
3
@76david76: Are $sin$ and $cos$ usually defined that way? That's often the way they're introduced, but then what is $sin 3pi/2$?
â Brian Tung
Sep 20 '16 at 22:31
1
It can be an expansion of the first definition. Is there really no way to define these functions out of the unit circle?
â 76david76
Sep 20 '16 at 22:49
2
@76david76 Most functions in analysis are not defined using geometry because we would first need a rigorous definition of points, lines, and so on. It is much easier to define them using taylor series. However, yes, you can develop these functions using the unit circle. When I said "we start by defining sinsin using arclength", that is referring to how we let $sin theta$ be the $y$-coordinate of the point on the unit circle such that the arc length from $(1,0)$ is $2 pi y$. If you define them using the unit circle, $cos^2 theta + sin62 theta$ is immediate like I said.
â 6005
Sep 20 '16 at 23:11
1
1
Thanks for this answer, but what about the usual definition of $sin$ and $cos$, as the proportion of sides of a triangle, that of course also doesn't depend on $sin^2x+cos^2x=1$, am I right?
â 76david76
Sep 20 '16 at 22:17
Thanks for this answer, but what about the usual definition of $sin$ and $cos$, as the proportion of sides of a triangle, that of course also doesn't depend on $sin^2x+cos^2x=1$, am I right?
â 76david76
Sep 20 '16 at 22:17
3
3
@76david76: Are $sin$ and $cos$ usually defined that way? That's often the way they're introduced, but then what is $sin 3pi/2$?
â Brian Tung
Sep 20 '16 at 22:31
@76david76: Are $sin$ and $cos$ usually defined that way? That's often the way they're introduced, but then what is $sin 3pi/2$?
â Brian Tung
Sep 20 '16 at 22:31
1
1
It can be an expansion of the first definition. Is there really no way to define these functions out of the unit circle?
â 76david76
Sep 20 '16 at 22:49
It can be an expansion of the first definition. Is there really no way to define these functions out of the unit circle?
â 76david76
Sep 20 '16 at 22:49
2
2
@76david76 Most functions in analysis are not defined using geometry because we would first need a rigorous definition of points, lines, and so on. It is much easier to define them using taylor series. However, yes, you can develop these functions using the unit circle. When I said "we start by defining sinsin using arclength", that is referring to how we let $sin theta$ be the $y$-coordinate of the point on the unit circle such that the arc length from $(1,0)$ is $2 pi y$. If you define them using the unit circle, $cos^2 theta + sin62 theta$ is immediate like I said.
â 6005
Sep 20 '16 at 23:11
@76david76 Most functions in analysis are not defined using geometry because we would first need a rigorous definition of points, lines, and so on. It is much easier to define them using taylor series. However, yes, you can develop these functions using the unit circle. When I said "we start by defining sinsin using arclength", that is referring to how we let $sin theta$ be the $y$-coordinate of the point on the unit circle such that the arc length from $(1,0)$ is $2 pi y$. If you define them using the unit circle, $cos^2 theta + sin62 theta$ is immediate like I said.
â 6005
Sep 20 '16 at 23:11
add a comment |Â
up vote
2
down vote
You are just showing that the Pythagorean theorem is a consequence of some property of the (complex) exponential function, there is no circularity in such argument. For instance, we may define, for any $zinmathbbC$,
$$ f(z)=e^z=sum_ngeq 0fracz^nn! tag1$$
and prove through a combinatorial argument that such a function fulfills $e^zcdot e^w=e^z+w$.
Since the Taylor coefficients at $0$ of such analytic function are real, we have $f(barz)=overlinef(z)$,
hence for any $rhoinmathbbR$
$$ left| e^irhoright| = e^irhocdot e^-irho = e^0 = 1. tag2$$
If we define $cos(rho)$ and $sin(rho)$ as the real/imaginary part of $e^irho$, we get that
$$ sin(rho)=sum_ngeq 0frac(-1)^n rho^2n+1(2n+1)!,qquad cos(rho)=sum_ngeq 0frac(-1)^n rho^2n(2n)!tag3 $$
and $(2)$ can be read as:
$$ sin^2(rho)+cos^2(rho) = 1.tag4$$
add a comment |Â
up vote
2
down vote
You are just showing that the Pythagorean theorem is a consequence of some property of the (complex) exponential function, there is no circularity in such argument. For instance, we may define, for any $zinmathbbC$,
$$ f(z)=e^z=sum_ngeq 0fracz^nn! tag1$$
and prove through a combinatorial argument that such a function fulfills $e^zcdot e^w=e^z+w$.
Since the Taylor coefficients at $0$ of such analytic function are real, we have $f(barz)=overlinef(z)$,
hence for any $rhoinmathbbR$
$$ left| e^irhoright| = e^irhocdot e^-irho = e^0 = 1. tag2$$
If we define $cos(rho)$ and $sin(rho)$ as the real/imaginary part of $e^irho$, we get that
$$ sin(rho)=sum_ngeq 0frac(-1)^n rho^2n+1(2n+1)!,qquad cos(rho)=sum_ngeq 0frac(-1)^n rho^2n(2n)!tag3 $$
and $(2)$ can be read as:
$$ sin^2(rho)+cos^2(rho) = 1.tag4$$
add a comment |Â
up vote
2
down vote
up vote
2
down vote
You are just showing that the Pythagorean theorem is a consequence of some property of the (complex) exponential function, there is no circularity in such argument. For instance, we may define, for any $zinmathbbC$,
$$ f(z)=e^z=sum_ngeq 0fracz^nn! tag1$$
and prove through a combinatorial argument that such a function fulfills $e^zcdot e^w=e^z+w$.
Since the Taylor coefficients at $0$ of such analytic function are real, we have $f(barz)=overlinef(z)$,
hence for any $rhoinmathbbR$
$$ left| e^irhoright| = e^irhocdot e^-irho = e^0 = 1. tag2$$
If we define $cos(rho)$ and $sin(rho)$ as the real/imaginary part of $e^irho$, we get that
$$ sin(rho)=sum_ngeq 0frac(-1)^n rho^2n+1(2n+1)!,qquad cos(rho)=sum_ngeq 0frac(-1)^n rho^2n(2n)!tag3 $$
and $(2)$ can be read as:
$$ sin^2(rho)+cos^2(rho) = 1.tag4$$
You are just showing that the Pythagorean theorem is a consequence of some property of the (complex) exponential function, there is no circularity in such argument. For instance, we may define, for any $zinmathbbC$,
$$ f(z)=e^z=sum_ngeq 0fracz^nn! tag1$$
and prove through a combinatorial argument that such a function fulfills $e^zcdot e^w=e^z+w$.
Since the Taylor coefficients at $0$ of such analytic function are real, we have $f(barz)=overlinef(z)$,
hence for any $rhoinmathbbR$
$$ left| e^irhoright| = e^irhocdot e^-irho = e^0 = 1. tag2$$
If we define $cos(rho)$ and $sin(rho)$ as the real/imaginary part of $e^irho$, we get that
$$ sin(rho)=sum_ngeq 0frac(-1)^n rho^2n+1(2n+1)!,qquad cos(rho)=sum_ngeq 0frac(-1)^n rho^2n(2n)!tag3 $$
and $(2)$ can be read as:
$$ sin^2(rho)+cos^2(rho) = 1.tag4$$
answered Sep 20 '16 at 22:28
Jack D'Aurizioâ¦
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