Why is ##x = r \sin{\phi} \cos{\theta}## in spherical coordinates?

AI Thread Summary
The discussion centers on the conversion between spherical and Cartesian coordinates, specifically the equation x = r sin(φ) cos(θ). Participants clarify that φ is the angle between the position vector and the z-axis, while θ is the angle in the xy-plane. The confusion arises over the concept of negative lengths in projections, with some arguing that projecting a negative length is meaningless, while others suggest it can represent direction. The consensus is that r (or ρ) is always positive, and thus the expression x = r sin(φ) cos(θ) does not require absolute values. Ultimately, the conversation emphasizes the importance of defining angles and distances correctly in spherical coordinates.
PFuser1232
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My question is really about converting between spherical coordinates and cartesian coordinates.
Suppose that ##\phi## and ##\theta## are defined as follows:
##\phi## is the angle between the position vector of a point and the ##z##-axis. ##\theta## is the angle between the projection of that vector onto the ##xy##-plane and the ##x##-axis.
Why exactly do we write ##x = r \sin{\phi} \cos{\theta}##?
I know that we first project the position vector onto the ##xy##-plane before projecting that projection onto the ##x##-axis. But if that were the case, shouldn't we write ##x = |r \sin{\phi}| \cos{\theta}##?
I'm confused because the quantity ##r \sin{\phi}## is, on occasion, negative. I thought we're only allowed to project "lengths" or "positive scalars". I am fully aware of the fact that the projection can itself be negative, but the whole notion that the length (not the final projection) which is to be projected can be negative isn't so intuitive.
Take for example a circle of radius ##r## centred at the origin. I'll define ##t## as the angle made with the ##x##-axis. ##x = r \cos{\theta}##. ##x## is allowed to be positive or negative, but ##r## is always positive.
 
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##\phi## is only defined on the domain ##0<\phi<\pi/2## so ##\sin(\phi) \ge 0##
 
Khashishi said:
##\phi## is only defined on the domain ##0<\phi<\pi/2## so ##\sin(\phi) \ge 0##

Isn't the choice of the interval somewhat arbitrary?
When dealing with polar coordinates for instance, we work on either ##(-\pi, \pi]## or ##[0, 2\pi)##.
 
Well, that's the standard convention. You can choose another convention if you want, but you'll have to deal with ##\sin(\phi) < 0## somehow, so the standard convention makes a lot of sense.
 
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Khashishi said:
Well, that's the standard convention. You can choose another convention if you want, but you'll have to deal with ##\sin(\phi) < 0## somehow, so the standard convention makes a lot of sense.

Thanks!
But am I correct in assuming that projecting a "negative length" is meaningless?
Also, I believe the domain you are talking about is ##0 \leq \phi \leq \pi##, not ##0 \leq \phi \leq \frac{\pi}{2}##.
 
MohammedRady97 said:
Also, I believe the domain you are talking about is ##0 \leq \phi \leq \pi##, not ##0 \leq \phi \leq \frac{\pi}{2}##.
Oops!

In some situations, you can interpret a negative length as a length in the opposite direction.
 
Khashishi said:
Oops!

In some situations, you can interpret a negative length as a length in the opposite direction.

Well, yeah. But not in this particular example, right?
 
Given the spherical coordinates as you say, the z coordinate is easy. If we draw a line from the given point perpendicular to the z-axis, \phi is the angle in a right triangle having the straight line from the origin to the point, of length \rho, as hypotenuse and the height above the xy-plane as "near side": so z= \rho cos(\phi).

Now consider the projection of that point in the xy-plane, (x, y, 0). The straight line from the origin to (x, y, 0) is the "opposite side" to \phi of a right triangle having \rho as hypotenuse- its length is \rho sin(\phi). And that line is the hypotenuse of a right triangle in the xy-plane with angle \theta and "near side" of length x, "opposite side" of length y. x/r= cos(\theta) so x= r cos(\theta)= \rho sin(\phi) cos(\theta) and y/r= sin(\theta) so y= r sin(\theta)= \rho sin(\phi)sin(\theta).
 
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HallsofIvy said:
Given the spherical coordinates as you say, the z coordinate is easy. If we draw a line from the given point perpendicular to the z-axis, \phi is the angle in a right triangle having the straight line from the origin to the point, of length \rho, as hypotenuse and the height above the xy-plane as "near side": so z= \rho cos(\phi).

Now consider the projection of that point in the xy-plane, (x, y, 0). The straight line from the origin to (x, y, 0) is the "opposite side" to \phi of a right triangle having \rho as hypotenuse- its length is \rho sin(\phi). And that line is the hypotenuse of a right triangle in the xy-plane with angle \theta and "near side" of length x, "opposite side" of length y. x/r= cos(\theta) so x= r cos(\theta)= \rho sin(\phi) cos(\theta) and y/r= sin(\theta) so y= r sin(\theta)= \rho sin(\phi)sin(\theta).

And the length ##\rho \sin{\phi}## is always positive, right?
 
  • #10
\rho itself is a distance so always positive. \phi is between 0 and \pi so sin(\phi) is positive. Yes, their product, the product of positive numbers, is positive.
 
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  • #11
HallsofIvy said:
\rho itself is a distance so always positive.
Per wikipedia, "always" is too strong.
It is also convenient, in many contexts, to allow negative radial distances, with the convention that (−r, θ, φ) is equivalent to (r, θ + 180°, φ) for any r, θ, and φ.
-- https://en.wikipedia.org/wiki/Spherical_coordinate_system

Note that for some reason they are using r instead of ##\rho##, which is more commonly used in spherical coordinates.
HallsofIvy said:
\phi is between 0 and \pi so sin(\phi) is positive. Yes, their product, the product of positive numbers, is positive.
 
  • #12
HallsofIvy said:
\rho itself is a distance so always positive. \phi is between 0 and \pi so sin(\phi) is positive. Yes, their product, the product of positive numbers, is positive.

So unlike polar coordinates, ##\phi## is always restricted to be between 0 and ##\pi##.
 
  • #13
MohammedRady97 said:
So unlike polar coordinates, ##\phi## is always restricted to be between 0 and ##\pi##.
Not according to the same article whose link I posted earlier.
If it is necessary to define a unique set of spherical coordinates for each point, one may restrict their ranges. A common choice is:

r ≥ 0
0° ≤ θ ≤ 180° (π rad)
0° ≤ φ < 360° (2π rad)
However, the azimuth φ is often restricted to the interval (−180°, +180°], or (−π, +π] in radians, instead of [0, 360°). This is the standard convention for geographic longitude.
 
  • #14
Mark44 said:
Not according to the same article whose link I posted earlier.
Mark44 said:
Not according to the same article whose link I posted earlier.

Which brings me to my initial question; how can we project a "negative length" onto a plane?
 
  • #15
You can project a positive length onto a plane, right? The projection of a "negative length" would be just as long but would point in the opposite direction.
 
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  • #16
Mark44 said:
You can project a positive length onto a plane, right? The projection of a "negative length" would be just as long but would point in the opposite direction.
So, is it wrong to write ##x = |\rho \sin{\phi}| \cos{\theta}## (where ##\phi## is the angle between the position vector of a point and the ##z##-axis)?
 
  • #17
Yes, it is. What is correct is that x= \rho sin(\phi) cos(\theta). There should be no absolute value since x, which is a coordinate, not a distance, can be negative.
 
  • #18
HallsofIvy said:
Yes, it is. What is correct is that x= \rho sin(\phi) cos(\theta). There should be no absolute value since x, which is a coordinate, not a distance, can be negative.
It could still be negative if ##x = |\rho \sin{\phi}| \cos{θ}##; there are no absolute value bars around ##\cos{θ}##.
 
  • #19
Right. I should have said that the absolute value bars are not necessary here. \rho, a distance, is always positive and since \phi lies between 0 and \pi, sin(\phi) is always positive \rho sin(\phi) cannot be negative..
 
  • #20
HallsofIvy said:
Right. I should have said that the absolute value bars are not necessary here. \rho, a distance, is always positive and since \phi lies between 0 and \pi, sin(\phi) is always positive \rho sin(\phi) cannot be negative..
For what it's worth, and to repeat what I said in post #11, wikipedia disagrees that ##\rho## is always positive -- https://en.wikipedia.org/wiki/Spherical_coordinate_system
 
  • #21
Mark44 said:
For what it's worth, and to repeat what I said in post #11, wikipedia disagrees that ##\rho## is always positive -- https://en.wikipedia.org/wiki/Spherical_coordinate_system
How do we define ##\phi## anyway? I thought the concept of "positive - counterclockwise, negative - clockwise" only makes sense in a plane, not in three dimensional space.
 
  • #22
MohammedRady97 said:
How do we define ##\phi## anyway? I thought the concept of "positive - counterclockwise, negative - clockwise" only makes sense in a plane, not in three dimensional space.
##\phi## is the angle between the z-axis and the ray along which you measure ##\rho##. The z-axis and the ray define a plane.
 
  • #23
Mark44 said:
##\phi## is the angle between the z-axis and the ray along which you measure ##\rho##. The z-axis and the ray define a plane.
How do we define negative angles in that case?
 
  • #24
In this specific case, we don't. \phi is always between 0 and \pi. It is never negative.
 
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  • #25
HallsofIvy said:
In this specific case, we don't. \phi is always between 0 and \pi. It is never negative.
Is the Wikipedia article posted earlier by @Mark44 wrong about ##\rho## being negative in some cases?
 
  • #26
MohammedRady97 said:
Is the Wikipedia article posted earlier by @Mark44 wrong about ##\rho## being negative in some cases?
It's not always positive, it could be zero.
 
  • #27
The point is you can use any system for spherical coordinates as long as it is well defined. For instance every time you get in an aircraft you rely on a system which uses ±90° latitude, ±180° longitude and height above (or below, in which case you are in trouble) an approximately equipotential geoid.
 
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