The other day I was looking at series and noticed that cos(i)
would actually be a real number, and the series for cos(ix) would
be a part of ex. Is there a function which has the
required series for the missing terms (i.e. x + x3/3! +
...) to make up ex, besides [sin(ix)]/i?
Also - is there a way to derive the series of cos-1 and
sin-1 (if such series exist) from the series for cos and
sin?
I hope the above makes sense - I haven't actually studied imaginary
numbers yet and am just treating them as ordinary numbers.
Thanks,
Olof.
Your observations are excellent. A few
points:
cos(i) is a real number. However I very much doubt it is rational -
it is actually equal to (e + 1/e)/2 (we'll see why a bit later). To
prove that it is irrational I would have thought you could do a
similar trick to the one in the proof that e is irrational. I'll
try this a bit later. Do you know the proof that e is irrational by
the way? I could write it out, or if you have STEP Maths III, 1997,
Q7 proves it (this is how I know the proof!).
Alternatively you can use the fact that e is transcendental. This
means it is not the root of any polynomial equation with integer
coefficients. I must confess I can't prove this, but it is known
that e (and also pi) are transcendental. Then note that if (e +
e-1)/2 is rational we can write
(e + e-1)/2 = a/b
for integers a,b which gives:
b e2 + b = 2ae
be2 - 2ae + b = 0
so e is a root of a polynomial equation which then contradicts the
fact that e is transcendental. Therefore (e + e-1)/2 is
irrational.
Secondly you are right that cos(ix) has part of the series for
ex, and you are also right that sin(ix)/i has the
"missing bit". If you put these two together you get:
cos(ix) + sin(ix)/i = ex
Now there is a far more usual way of writing this - let x =
it:
cos(-t) + sin(-t)/i = eit
So:
eit = cos(t) + i sin(t)
This is an extremely useful (and well known) formula, called
Euler's theorem. One particularly interesting consequence is that
if you set t = pi:
eip = -1.
Richard Feynman was especially entralled by this result.
If you take Euler's theorem and replace t by -t you get:
e-it = cos t - i sin t
And if you add this to eit = cos t + i sin t you
get:
cos t = [eit + e-it]/2
(you can now see why cos(i) = (e + 1/e)/2
If you subtract one equation from the other:
sin t = [eit - e-it]/2i
These two formulae can be very useful. One application (though by
no means the most important) is you can now work out things
like:
sin x + sin 2x + sin 3x + ... + sin nx
Simply rewrite the sum in terms of exponentials then arrange it to
get two geometric progressions, which you know how to sum.
Also you ask whether x + x3/3! + x5/5! + ...
has another name. The answer is yes - it is called sinh(x)
(pronounced as shine x). This is a hyperbolic function - two others
are cosh x (pronounced as spelt) and tanh x (I'm not really sure
how this is pronounced!). They are highly analogous to the normal
trigonometric functions. They satisfy:
cosh(x) = cos(ix)
sinh(x) = -isin(ix)
tanh(x) = sinh(x) / cosh(x)
and are reasonably useful. You can write them very simply in terms
of exponentials:
cosh(x) = (ex + e-x)/2
sinh(x) = (ex - e-x)/2
tanh(x) = (e2x - 1)/(e2x + 1)
Also they obey very similar identities to sin,cos and tan. For
instance:
sinh(2x) = 2sinh(x)cosh(x)
This of course is no co-incidence! You can show it is equivalent to
sin(2x) = 2sin(x)cos(x) by making a very simple substitution.
Hope this helps slightly,
Michael
By the way, you might like to have a think
about other ways of showing that
eix = cos x + i sin x
Here is one way.
Let y = cos x + i sin x
Now y'' + y = 0
where y'' = second derivative of y wrt x.
You can rewrite this as:
y'' + iy' - iy' + y = 0
which then becomes:
(y' + iy)' - i(y' + iy) = 0
So z = y' + iy satisfies:
z' - iz = 0
Now you can solve this for z in terms of exponentials (applying
initial conditions). Then solve for y (again with initial
conditions). You should find y = eix, thus proving
eix = cos x + i sin x.
The first way I came across how to find Euler's theorem, was when
we were set an integration question - integrate
1/(x2+1). Not knowing about the derivative of arctan, I
tried writing it as:
1/(x2+1) = 1/[(x+i)(x-i)]
Then split the right hand expression into partial fractions (using
normal rules of algebra) and integrate! If you equate the result to
arctan x you can derive the result:
arctan x = i/2 ln((i+x)/(i-x))
from which you can get Euler's formula after a lot of tedious
manipulation.
It's funny that you should mention STEP III '97 - I just got
ahold of this paper yesterday! I'll have a look at Question 7
tonight, thanks for telling me about it.
I had an inkling that this would lead to eip = -1, and I must agree with Mr. Feynman
that this is a beautiful result! I love the way Mathematics can
fill you with amazement like this.
I've always wondered what sinh and cosh were, and always forgotten
to find out. It's nice the way that all these sets of functions are
inter-related.
As for other ways of deriving eix = cos x + i sin x, you
mention z' - iz = 0 (which is fine), but I'm not familiar with "you
can solve this for z in terms of exponentials (applying initial
conditions)". Could you please explain what this means?
Thanks,
Olof.
epi
= -1 is certainly amazing. After all what has the base of natural
growth got to do with the ratio between the circumference and
diameter of a circle, and the square root of -1!? I've heard people
even use this to argue the existence of God! (Let's not get
side-tracked by that though!) It generally tends to surprise
non-mathematicians more than mathematicians.
This is perhaps because, if you think about it for a while, you
realise that epi = -1 is
actually little more than a tautology, in thick disguise. But to
realise why you need to know a bit about the geometry of complex
numbers. Have you heard of the Argand diagram?
Next... z' - iz = 0 is a first order differential equation. Another
way of writing it is:
dz/dx = iz
Have you learnt how to solve equations of this type yet? Here is
one way of getting z in terms of x:
1/z dz/dx = i
Notice that by the chain rule:
d(ln z)/dx = 1/z dz/dx
So our equation:
d(ln z)/dx = i
In other words the gradient of ln z is i everywhere. This means
that ln z is a straight line:
ln z = ix + C
where C is just some constant.
z = eix + C = eix eC =
Aeix
where A is another constant (=eC).
We really want to get rid of that constant A, as it is unknown at
the moment. So what do we know? Well we know that when x = 0, z =
2i. How do we know this? Well y = cos x + i sin x = 1 (when x = 0)
and y' = -sin x + i cos x = i (when x = 0). So z = i + i = 2i when
x = 0 (this is called an initial condition).
Also we know z = Aeix, so substituting x = 0:
2i = Ae0, so A = 2i
z = 2ieix
Therefore the differential equation for y is:
y' + iy = 2ieix
I'll show you how to solve this for y if you like, but you'll
probably work it out for yourself first! There are actually two
approaches, and I'll give a hint for each one:
Approach 1: Multiply the equation by eix. See if you can
do anything with the result.
Approach 2: Start by finding any old solution to the equation. Then
use this to find all solutions.
Yours,
Michael
I had heard about eip = -1
before: my teacher keeps saying that it's the most beautiful
sentence in the English language. However, I had never seen a proof
of it, and never realised that such a seemingly abstract concept
could be so accessible!
I can imagine that it has been brought into the never-ending
existence-of-God debate, and I best not comment on that (I've read
the debate on God's existence in another discussion, and people
seem to feel quite strongly about it)!
I think I've seen something about the Argand plane in a past STEP
question (which I left out), but that's as far as my knowledge of
the subject extends unfortunately. Now that I mention STEP - I like
the proof that e is irrational in STEP III '97; it's a nice
method.
I haven't really come across differential equations yet (we'll be
doing it in a few weeks I believe), nor have we studied the chain
rule yet, but I asked about some of the calculus rules (chain,
product, integration by parts) here on NRICH, so I know about and
understand them now. Cheers NRICH!
I see what you've done in solving z' = iz now.
As for y' + iy = 2ieix, it's quite easy to see 'by
inspection' that y = eix (especially if you multiplay
everything by eix first), and that's pretty much the
only way I've been able to solve it! I'd be grateful if you could
show me a method.
Yours,
Olof.
Well done for getting STEP 1997, Q7 so
quickly. I remember struggling with the third part of Q7 for a long
time for some reason, when I first tried the paper about 1-2 years
ago. Euler was the first to prove that e is irrational in the 1730s
I think. I'm not sure whether that was his method or not (but I'd
guess so).
For y' + iy = 2ieix then if you multiply by
eix:
eixy' + eixiy = 2ie2ix
This can now be written:
(eixy)' = 2ie2ix
(you can check the left hand side using the product rule)
Now you can integrate:
eixy = e2ix + C
Because 2ie2ix integrates to e2ix. To check
this you can differentiate e2ix by the chain rule. Is
this bit OK? If so we then have:
y = eix + Ce-ix
where C is an arbitrary constant. So in fact we can't yet conclude
y = eix; that is only one possibility. To show that C =
0 we need more information.
Remembering the definition of y as cos x + i sin x, you can apply
the condition y = 1 when x = 0:
1 = e0 + C
So C = 0, and we get:
y = eix
But y = cos x + i sin x so:
eix = cos x + i sin x as we were hoping!
Now there is another method for solving:
y' + iy = 2ieix
You have already spotted one solution is y = eix. (If
you hadn't spotted this you could "guess" a solution of the form
Aeix and see if it works for any A.) Once you've got one
possible solution, the problem becomes easier.
Suppose there are two different functions y1(x) and
y2(x) that both satisfied the given equation.
Well
y1' + iy1 = 2ie2ix
y2' + iy2 = 2ie2ix
Subtracting:
(y1 - y2)' + i(y1 - y2)
= 0
So q = y1 - y2 satisfies:
q' + iq = 0
So:
1/q q' = -i
(ln q)' = -i
ln q = -ix + C
q = e-ix + C
q = Ae-ix
And this means that any two solutions to the equation
satisfy:
y1 - y2 = Ae-ix
It therefore follows that if y2(x) = eix then
for all y1 satisfying the equation:
y1 = eix + Ae-ix
which is the same solution as before. Once again you can show A = 0
for this particular problem - sometimes you can't determine A, and
have to leave it as a final result.
In this case you wouldn't need to bother with any of this, because
you had already found y = eix and this happens to be the
solution with the correct value at x = 0. For simple 1st order
differential equations (i.e. ones not involving y'', y''', y'''')
it is always true that if you find a function that satisfies the
equation, and it has the correct value at x = 0 (or indeed anywhere
else) then this function gives the correct values
everywhere.
By the way, I've just noticed you asked
about the series for cos-1x and sin-1x. These
can't really be derived from the series from sin and cos (or at
least I can't!) The problem is:
sin x = x - x3/3! + x5/5! - ...
Now if you replace x by sin-1x:
x = sin-1x - (sin-1x)3/3! +
...
Unfortunately this gives us a polynomial equation of infinite order
to solve for sin-1x, which is not easy. It might just be
possible though if we assume sin-1x to have a series
solution, then plug in to get a recurrence relationship for the
coefficients. I can't quite make this work at the moment, but it is
certainly a good idea.
An easier way to get sin-1x (and you can apply an
identical method for cos-1x) is to look at its
derivative.
If y = sin-1x
Then:
x = sin y
Differentiate wrt y:
dx/dy = cos y
So dy/dx = 1/cos y
Now we try to get this in terms of x:
dy/dx = 1/sqrt(1-sin2y) = 1/sqrt(1-x2)
Strictly you should check to make sure you take the positive root,
but it should be clear why this is so, given that sin-1x
returns principle values.
So if y = sin-1x, dy/dx = 1/sqrt(1-x2)
Now try writing out the denominator of the RHS using the binomial
expansion. Then integrate to find y (remember you get an arbitrary
constant of integration, which you need to calculate) and then
that's the series expansion for sin-1x!
Hope this helps,
Michael
I didn't quite get the 3rd part of Q7 either, until I wrote out
some more terms of the series, and realised that all terms up to
n!/n! would be integers (which is obvious in retrospect). I don't
like the look of any of the other questions on that paper though
(except Q2, which is similar to a question I once did 'which is
greatest: ep or pe'). It has to be said though, some of
these STEP questions are great (I've been doing quite a few papers
recently), although I wouldn't like to do them under
exam-conditions! I'm not looking forward to that.
Ah, now I see. These differential equations are quite interesting.
I read ahead in the book we're doing at the moment, and I think the
only thing we cover is differential equations of the form y' = ky
(or -ky). I hear that you study them a lot at
University-level?
We have only covered series briefly: we were doing Taylor
approximations in a book called "Numerical Methods", and it
mentions the series for sin x, cos x and ex. We had just
been discussing what order we should do the next couple of modules
in, which got me thinking about complex numbers (which we are going
to study soon I think). Then later on that night the thought
occured to me that x4 = 1 has 3 solutions (1, -1, i,
providing there are no special rules for imaginary numbers?), and
that i4n will always be 1, and i4n-2 will
always be -1 (for integer n). This result practically begged to be
put into the series of cos x, to completely change the function. So
it was really completely due to chance that cos ix + (sin ix)/i =
ex popped into my head.
You'll be happy to know we did the chain and product rule at school
today. I was given a nice function to differentiate on the board:
(26x2 + e3^x)2(cos
x3+4sin x). Great fun that was.
That's a great way of finding the series for sin-1x!
Thanks for that. I've tried programming the series into my
calculator, and it gets the first few values right, but after 6 or
so iterations it starts diverging (perhaps because of its limited
memory capabilities). Are there many other series that can be used
to find p (besides
cos-1)?
Regards,
Olof.
Don't miss the root -i to the equation
x4=1, since we have
(-i)4=(-1)4(i)4=1, and we have i
and -i distinct. Otherwise, we would have i=-i, which means that i
is identically zero, a contradiction. In general, a polynomial
equation of order n has exactly n roots(not necessarily distint) in
the complex plane.
Another way to find p is via
tan-1 x. The most obvious one is by setting x=1 in the
Maclaurin seies of tan-1 x, which is
x-x3/3+x5/5-...
and multiply by 4. However, this series converges very slowly, and
one can show that you will need about 1 million terms to get to 6
d.p. accuracy. On the other hand, if you play around with
tan(a±p/4)=tan b or various
other equations, you should be able to find a method that will give
p in a reasonable amount of time.
Kerwin
Another way of seeing that x4 =
1 has a root of -i as well as 1,-1,i is the following
theorem:
If x is a solution to a polynomial equation with real coefficients
then x* is also a solution. x* is the complex conjugate of x,
defined as follows:
(a + ib)* = a - ib
where a,b are real.
This theorem is pretty easy to prove if you know the binomial
expansion. Here the theorem tells us that as i is a solution to
x4 = 1, i* is also a solution. And of course i* = (0 +
1i)* = (0 - 1i) = -i. This can be a useful check if you're solving
polynomials in the complex domain.
Out of interest, when you programmed your calculator with the
series for sin-1x and then tested it out, which value of
x did you use? The obvious one to try I think is x = 1/2 as this
returns p/6. If this is what you did
then I don't really see why it didn't converge... It should
converge for all -1 < x < 1.
There are loads of formulae for calculating p. One other is:
p2/6 = 1/12 +
1/22 + ...
Actually that one is extremely important for other reasons. To see
where it comes from, note that sin x has roots at np. Therefore it is conceivable that the sin
function is:
sin x = ...(1 - x/(2p))(1 -
x/p)x(1 + x/p)(1 + x/(2p))...
Then you can combine factors pairwise to get (by difference of two
squares):
sin x = x(1-x2/p2)(1-x2/(4p2))...
Then write sin x using its usual Maclaurin expansion and equate the
coefficients of x3 on each side of the equation, and you
should get:
1/12 + 1/22 + ... = p2/6
This method also allows you to work out 1/14 +
1/24 + ... (simply equate coefficients of x5)
and in fact all the series with even powers, but the result for odd
powers is unknown.
This series does converge more quickly than the arctan one Kerwin
gave, but this is nothing compared to one derived in the 1960s. In
this algorithm you have a simple programming loop (of about 6
lines) which gives an approximation for p each loop. The amazing thing is: the number of
correct digits of p it gives doubles
with each loop!! I haven't got the program on me at the moment
unfortunately, but you can find it in the Penguin Dictionary of
Curious and Interesting Numbers (a very useful reference
book).
I can't remember any of the rest of the 1997 paper (I don't think I
did all the questions, but the prove e is irrational one was too
interesting to miss out!). If you have any specific difficulties
with the paper please post them!
Your teacher was obviously in a very bad mood to make you calculate
that derivative. Out of interest, how did you differentiate
4sin x?
Yours,
Michael
By the way, I should have mentioned
earlier that the standard way of deriving Euler's formula (the one
you'll find in every such textbook without fail) also uses series
expansions:
eix = 1 + ix + (ix)2/2! + (ix)3/3!
+ (ix)4/4! + ...
= (1 - x2/2! + x4/4! - ...) + i(x -
x3/3! + x5/5! - ...) = cos x + i sin x
I used to dislike this method, but then I distrusted series
expansions till quite recently. And anyway it gives no indication
of why the result is true. The best way of seeing why it is true is
to think geometrically. So I'll give a bit of introductory
information about the Argand diagram.
Each complex number is represented as a point on a plane. So the
number x + iy is displayed as the point with co-ordinates
(x,y).
The modulus of a complex number is defined as the length from the
origin to the number in the Argand diagram. So modulus of a + ib =
sqrt(a2 + b2)
The argument of a complex number is the angle between the x axis
and the number. So we can write all complex numbers in
modulus-argument form:
z = r(cos x + i sin x)
where r is the modulus and x is the argument.
Next... can you see what is going to happen when you add two
complex numbers? It is very, very similar to vector addition!
Also we need to know about multiplication. See if you can show that
when you multiply two complex numbers the result has modulus equal
to the product of the moduli of the first two complex numbers,
while the argument of the product is the sum of the arguments of
the original complex numbers. Hint: use the modulus - argument form
of the numbers given above.
I think that not many people would have seen your way of deriving
Euler's formula, because substituting a complex quantity into a
cosine (which is to do with real angles) is not at all
obvious!
Yours,
Michael
I see what you mean about -i satisfying x4 = 1 as
well. Complex numbers open up so many new interesting
possibilities.
Is the series for tan-1x really that slow to converge to
p/4? Is there a way to prove how quickly
a series converges for different values?
I found what the problem was with my program: there was a bracket
missing on one of the lines! It only caused a slight error, but it
was enough to cause the series to diverge after 10 or so terms. I
might have a go at programming it onto my PC, so that I can get
more decimal places (my calculator only does it up to 9 I think),
and compare the efficiencies of all the different methods I can
find for generating p.
The Penguin Dictionary of Curious and Interesting Numbers is a very
good book. They have it at my school's library - I'll get it out on
monday and have a look for the loop you mention - it sounds
amazing! The only problem with the book is that you find so many
things you want to investigate further. I had no idea how to get to
the series for p2/6, which I
first found in this book, so thanks once again for showing me. One
thing - I'm having a little trouble equating the coefficients for
x4 and reducing it all to 1/14 +
1/24.... What is it that I'm missing?
To differentiate y = 4sin x I said:
y = eu,
u = ln4 × sin x,
Then
du/dx = ln4 × cos x,
dy/du = eu,
therefore
dy/dx = ln 4 × cos x × 4sin x. Hope that's
right.
It wasn't actually the teacher who set the question: she told us
students to set each other challenges, and my 'so-called' friend
gave me that :).
Thanks for the information on the Argand diagram - I'll be sure to
have a go at working with complex numbers in the ways you mentioned
(when I'm not this tired).
Regards,
Olof.
[Part of this post was actually from
Kerwin Hui: the correction he pointed out has been inserted! - The
Editor]
Sorry, I'm not sure how to tell how fast a
series converges in general. I think I can explain it in the
specific case of 1/1 - 1/3 + 1/5 - 1/7 + ... but I'll think it over
before writing in as my explanation may be flawed.
Regarding tha 1/14+1/24+ ...,
Actually this is a bit tricky to write out so perhaps a better way
is as follows:
sin x = x(1-x2/p2)(1-x2/(4p2)...
or we can write this:
sin x = ...(1 - x/(2p))(1 -
x/p)x(1 + x/p)(1 + x/(2p))...
Take logs and differentiate:
cos x / sin x = ... + 1/(x + 2p) + 1/(x
+ p) + 1/x + 1/(x - p) + ...
We have to be a bit careful here about convergence. To make sense,
we have to evaluate this infinite sum from the middle outwards. So
we can think of the RHS as the limit of the sequence:
1/x
1/(x + p) + 1/x + 1/(x - p)
1/(x + 2p) + 1/(x + p) + 1/x + 1/(x - p) +
1/(x - 2p)
...
Differentiate the expression again:
cosec2x = ... + 1/(x+p)2 + 1/x2 + 1/(x-p)2 + ...
cosec2 x = S¥ r=-¥(x+rp)
-2
Differentiating once gives
-2 cosec2 x cot x = -2 S¥ r=-¥(x+rp)
-3
Simplify and differentiate again gives
-2 cosec2 x cot2 x - cosec4 x = -3
S¥ r=-¥(x+rp)
-4
Substitute x = p/2 and remember that cot
(p/2) = 0, we have
1=3 S¥ r=-¥(p/2+rp-4=
96/p4 S all positive odd
r r-4
so we have S
all positive odd r
r-4=p4/96
Hence 1/14 + 1/24 + ... = z(4)=S¥ r=1 r-4= p/90
Can you see why this method fails for 1/13 +
1/23 + 1/33 + ... (and indeed all odd
powers)? Whether this number has an analytical form is unknown. In
the 1970s it was proved to be irrational but that is about all we
know!
Yours,
Michael
Just to clarify:
z(n) is the Zeta function, defined
as:
z(n) = 1/1n + 1/2n
+ 1/3n + ...
This function is connected to possibly the most important unsolved
problem in mathematics today - the Riemann hypothesis. This states
that the only complex solutions to the equation:
z(x) = 0
are of the form x = 1/2 + ti where t is real.
So if you're finding your A-Levels a bit easy and have a bit of
spare time, why not give this a crack?
Ah, so that's what the Riemann hypothesis is all about. Looks
like fun.
What are cosec and cot? From my differentiation (which is probably
wrong), cosec x would equal 1/sin x; is that right? I'm not even
going to hazard a guess for cot x (ok go on then, 1/tan x?).
Do they have special derivative connections, or do you have to go
through using product rule and chain rule about 10 times over when
doing all the above?
/Olof
Olof,
Indeed, cosec x = 1/sin x, and cot x = 1/tan x = cos x/sin x.
To find the derivative of cot x, we differentiate the quotient to
get
(-sin2 x - cos2 x)/sin2 x, which
is, of course, -1/sin2 x, otherwise known as
-cosec2 x.
Similarly, we can differentiate cosec x (I'll leave it as an
exercise for you).
Note that in some books, cosec is abbreviated further as csc.
Kerwin
Thanks Kerwin.
y = cosec x
dy/dx = -cot x/sin x?
Does 1/cos x also have another name?
Michael-
I've had a look at what you mentioned about complex arithmetic and
the Argand diagram, and I'm fine with that.
I'm still working on showing Euler's formula geometrically using
this.
Regards,
Olof.
Olof,
That's correct. The derivative of cosec x is -cot x cosec x. 1/cos
x is written as sec x, where sec is the abbreviation of
secant.
Going back to the question of convergence, there is no easy way of
estimating how quickly a series converges. However, for alternating
series that converge, the truncation error is less than or equal to
the first neglected term providing the remaining terms are each
less than the first neglected term in magnitude. Hence, as a crude
approximation, the number of terms needed to get N decimal place
accuracy out of
tan-1(1)=1-3-1+5-1-7-1+...
is when the first neglected term is less than (0.5)10-N,
which means that 10N terms is necessary.
Kerwin
To remember what cot, sec and cosec are
the reciprocal of; just look at their third letter. We similarly
have hyperbolic equivalents:
coth, sech, cosech
Anyway, I've just realised I made a bit of a mess of the geometry -
I used the letter x both as the argument, and as the x co-ordinate.
I think you knew what I meant. Just to re-iterate:
A complex number x + iy is represented by a point (x,y) in the
Argand diagram. And it can also be specified by the length from the
origin (the modulus r), and the angle between the x-axis and the
line joining the origin to the complex number (this is called the
argument and I'll call it q this time).
The angle is measured anti-clockwise, by the way.
So the modulus-argument form of our complex number z = x + iy
is:
z = r(cos q + i sin q)
where r = sqrt(x2 + y2)
and tan q = y/x.
And we know that complex numbers add like vectors and when you
multiply two complex numbers you multiply the moduli and add the
arguments.
To see how to explain Euler's formula with the Argand diagram,
remember what y = emx means. It means the rate of change
of the function y is equal to m times the value of the function
y.
Now if we let m = i, we have a function, the rate of change of
which wrt x is equal to iy. And we recall that in the Argand
diagram iy is perpendicular to y and of the same magnitde.
Now imagine you are walking in the Argand diagram, and your
position after a time t is given by the complex number y =
eit. You know the rate of change of the function (your
position) with respect to time is given by iy. In other words, your
velocity is iy and is perpendicular to the line joining you and the
origin. So what kind of curve are we moving in?
Would you be moving in a circle (radius 1, centre the origin) on
the Argand diagram? I'm not sure if I went about it the right way :
I plotted the complex numbers z, where z = eit.
Sorry for taking so long to get back to you; I have a Physics exam
on Monday so I haven't been on the PC much.
Regards,
Olof.
Sorry, I missed your message! Anyway, your
answer is correct but unfortunately you've had to assume the result
we're trying to prove!
What's happening is that we're moving in such a way that our
velocity is perpendicular to the line joining us and the origin
(see earlier). In other words our distance from the origin isn't
changing. (If our distance from the origin was changing this
would require our velocity had an inward or outward component. And
we know this isn't true.) Therefore we are clearly walking in a
circle, centred on the origin.
But what is the radius of the circle? Well our position is z =
eit. So at t = 0 we are at z = ei*0 = 1. We
start off at a distance one from the origin, and as we're moving in
a circle we stay a distance 1 from the origin.
Therefore eix is a circle (radius 1, centre origin) in
the Argand diagram. The only question is which values of x
correspond to which points on the unit circle. If you're with me so
far, I'll try and explain this next bit...
Good luck in the physics!
Michael
Of course! It's so obvious now!
I missed the key bit about emt meaning that the rate of
change of the function y is equal to m times the value of the
function y, which you mentioned in your previous post. That cleared
it all up.
I kept doing the same thing (assuming the thing you're trying to
prove) when I had a go a proving the fundamental theorem of
arithmetic. Now that was annoying. Got there in the end though,
fortunately.
I had the Physics exam this morning (Materials and Waves). I think
it went OK, but everyone thought it was an easy exam, so the
examiners may not be very kind in their marking. It'll be a while
before we find out what we get anyway, so I'm not going to worry
about it.
Thanks again,
Olof