how does the equation

cos(x)= (exp(ix) + exp(-ix))/2     

and the sine equivalent fit into this? Clearly exponentials are not restricted 
to angles ... indicating that x (and by implication angles) have no dimensions.



Marc Schiltz's previously cited Taylor expansion demonstrates this even better:

sin(x) = x/1! - x^3/3! + x^5/5! ..... etc to infinity

If you assume for a moment that x does have a dimension, lets call it [X], then 
the equation is dimensionally unbalanced

[?] = [X]^1 - [X]^3 + [X]^5    ...... etc

and is therefore invalid. It only makes sense if x, and its sine, are 
dimensionless

Pete






On 23 Nov 2009, at 16:42, marc.schi...@epfl.ch wrote:

> Dale Tronrud wrote:
>>    While it is true that angles are defined by ratios which result in
>> their values being independent of the units those lengths were measured,
>> common sense says that a number is an insufficient description of an
>> angle.  If I tell you I measured an angle and its value is "1.5" you
>> cannot perform any useful calculation with that knowledge.
> 
> 
> I disagree: you can, for instance, put this number x = 1.5 (without units) 
> into the series expansion for sin X :
> 
> x - x^3/(3!) + x^5/(5!) - x^7/(7!) + ...
> 
> and compute the value of sin(1.5) to any desired degree of accuracy
> (four terms will be enough to get an accuracy of 0.0001). Note that
> the x in the series expansion is just a real number (no dimension, no
> unit).
> 
> 
> 
> Yes it's
>> true that the confusion does not arise from a mix up of feet and meters.
>> I would have concluded my angle was 1.5 in either case.
>> 
>>    The confusion arises because there are differing conventions for
>> describing that "unitless" angle.  I could be describing my angle as
>> 1.5 radians, 1.5 degrees, or 1.5 cycles (or 1.5 of the mysterious
>> "grad" on my calculator).
> 
> 
> 
> These are just symbols for dimensionless factors :
> 
> 1 rad = 1
> 1 degree = pi/180
> 1 grad = pi/200
> 
> Thus :
> 
> 1.5 rad = 1.5
> 1.5 degree = 0.0268
> 1.5 grad = 0.0236
> 
> and all these numbers (which have no units !!!) can be put into the
> series expansions for trigonometric functions.
> 
> In my opinion, it is actually best not to use the symbol rad. As we can
> see from this discussion, it mostly creates confusion.
> 
> 
> 
> For me to communicate my result to you
>> I would need to also tell you the convention I'm using, and you will
>> have to perform a conversion to transform my value to your favorite
>> convention.  If it looks like a unit, and it quacks like a unit, I
>> think I'm free to call it a unit.
>> 
>>    I think you will agree that if we fail to pass the convention
>> along with it value our space probe will crash on Mars just as hard
>> as if we had confused feet and meters.
>> 
>>    The result of a Sin or Cos calculation can be treated as "unitless"
>> only because there is 100% agreement on how these results should be
>> represented.  Everyone agrees that the Sin of a right angle is 1.
> 
> 
> This is not a simple matter of agreement (or convention), it is
> contained in the very definition of the sine function.
> 
> 
>> If I went off the deep end I could declare that the Sin of a right
>> angle is 12 and I could construct an entirely self-consistent description
>> of physics using that convention.
> 
> 
> I challenge you to draw a right triangle on paper where the length of
> one of the sides measures 12 times the length of the hypotenuse.
> 
> Of course, you can say that your "crazy Tronrud Sin" is defined
> differently, but then we are really speaking about something else. You
> can define whatever crazy quantity you want. But the need for a function
> which describes the ratio of the length of a side of a right triangle
> to the length of its hypotenuse will inevitably arise at some point in
> physics and mathematics. And the "crazy Tronrud Sin" will not do this
> job. So the proper sine and cosine functions will eventually have to
> be invented.
> 
> 
> 
> 
> In that case I would have to be
>> very careful to keep track of when I was working with traditional
>> Sin's and when with "crazy Tronrud Sin's".  When switching between
>> conventions I would have to careful to use the conversion factor of
>> 12 "crazy Tronrud Sin's"/"traditional Sin" and I'd do best if I
>> put a mark next to each value indicating which convention was used
>> for that particular value.  Sounds like units to me.
>> 
>>    Of course no one would create "crazy Tronrud Sin's" because the
>> pain created by the confusion of multiple conventions is not compensated
>> by any gain.  When it comes to angles, however, that ship has sailed.
>> While mathematicians have very good reasons for preferring the radian
>> convention you are never going to convince a physicist to change from
>> Angstrom/cycle to Angstrom/radian when measuring wavelengths.  You
>> will also fail to convince a crystallographer to measure fractional
>> coordinates in radians.  We are going to have to live in a world that
>> has some angular quantities reported in radians and others in cycles.
>> That means we will have to keep track of which is being used and apply
>> the factor of 2 Pi radian/cycle or 1/(2 Pi) cycle/radian when switching
>> between.
>> 
>>    I agree with Ian that the 8 Pi^2 factor in the conversion of
>> <u_x^2> to B looks suspiciously like 2 (2 Pi)^2 and it is likely
>> a conversion of cycle^2 to radian^2.  I can even imagine that the
>> derivation of effect of distortions of the lattice points that lead
>> to these parameters would start with a description of these distortions
>> in cycles, but I also have enough experience with this sort of problem
>> to know that you can only be certain of these "units" after going
>> back to the root definition and tracking the algebra forward.
>> 
>>    In my opinion the Mad Scientist is right.  B and <u_x^2> represent
>> the same quantity reported with different units (or conventions if
>> you will) and the answer will be something like B in A^2 radian^2
>> and <u_x^2> in A^2 cycle^2.  It would be much clearer it someone
>> figured out exactly what those units are and we started properly
>> stating the units of each.  I'm sorry that I don't have the time
>> myself for this project.
>> 
>> Dale Tronrud
>> 
>> P.S. As for your distinction between the "convenience" units used to
>> measure angles and the "absolutely required" units of length and mass:
>> all units are part of the coordinate systems that we humans impose on
>> the universe.  Length and mass are no more fundamental than angles.
>> Feet and meters are units chosen for our convenience and one converts
>> between them using an arbitrary scaling constant.  In fact the whole
>> distinction between length and mass is simply a matter of convenience.
>> In the classic text on general relativity "Gravitation" by Miser,
>> Thorne and Wheeler they have a table in the back of "Some Useful
>> Numbers in Conventional and Geometrized Units" where it lists the
>> mass of the Sun as 147600 cm and and the distance between the Earth
>> and Sun as 499 sec.  Those people in general relativity are great
>> at manipulating coordinate systems!
>> 
>>> -----Original Message-----
>>> From: CCP4 bulletin board [mailto:ccp...@jiscmail.ac.uk] On Behalf Of Ian
>>> Tickle
>>> Sent: Sunday, November 22, 2009 10:57 AM
>>> To: CCP4BB@JISCMAIL.AC.UK
>>> Subject: Re: [ccp4bb] units of the B factor
>>> 
>>>     Back to the original problem: what are the units of B and
>>>> <u_x^2>?  I haven't been able to work that out.  The first
>>>> wack is to say the B occurs in the term
>>>> 
>>>>     Exp( -B (Sin(theta)/lambda)^2)
>>>> 
>>>> and we've learned that the unit of Sin(theta)/lamda is 1/Angstrom
>>>> and the argument of Exp, like Sin, must be radian.  This means
>>>> that the units of B must be A^2 radian.  Since B = 8 Pi^2 <u_x^2>
>>>> the units of 8 Pi^2 <u_x^2> must also be A^2 radian, but the
>>>> units of <u_x^2> are determined by the units of 8 Pi^2.  I
>>>> can't figure out the units of that without understanding the
>>>> defining equation, which is in the OPDXr somewhere.  I suspect
>>>> there are additional, hidden, units in that definition.  The
>>>> basic definition would start with the deviation of scattering
>>>> points from the Miller planes and those deviations are probably
>>>> defined in cycle or radian and later converted to Angstrom so
>>>> there are conversion factors present from the beginning.
>>>> 
>>>>    I'm sure that if the MS sits down with the OPDXr and follows
>>>> all these units through he will uncover the units of B, 8 Pi^2,
>>>> and <u_x^2> and the mystery will be solved.  If he doesn't do
>>>> it, I'll have to sit down with the book myself, and that will
>>>> make my head hurt.
>>> Hi Dale
>>> 
>>> A nice entertaining read for a Sunday afternoon, but I think you can
>>> only get so far with this argument and then it breaks down, as evidenced
>>> by the fact that eventually you got stuck!  I think the problem arises
>>> in your assertion that the argument of 'exp' must be in units of
>>> radians.  IMO it can also be in units of radians^2 (or radians^n where n
>>> is any unitless number, integer or real, including zero for that
>>> matter!) - and this seems to be precisely what happens here.  Having a
>>> function whose argument can apparently have any one of an infinite
>>> number of units is somewhat of an embarrassment! - of course that must
>>> mean that the argument actually has no units.  So in essence I'm saying
>>> that quantities in radians have to be treated as unitless, contrary to
>>> your earlier assertions.
>>> 
>>> So the 'units' (accepting for the moment that the radian is a valid
>>> unit) of B are actually A^2 radian^2, and so the 'units' of 8pi^2 (it
>>> comes from 2(2pi)^2) are radian^2 as expected.  However since I think
>>> I've demonstrated that the radian is not a valid unit, then the units of
>>> B are indeed A^2!
>>> 
>>> Cheers
>>> 
>>> -- Ian
>>> 
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> 
> --
> Marc SCHILTZ      http://lcr.epfl.ch

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