Movement on a Sphere: Find Lat & Long of Point P

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The discussion focuses on calculating the latitude and longitude of a point P(\theta,\phi) moving along the shortest path (great circle) between two points P1(\theta1,\phi1) and P2(\theta2,\phi2) on a sphere at a constant speed v. Participants emphasize deriving expressions for the angles as functions of time, utilizing the relationships between angular velocity and linear velocity on a sphere. The conversation highlights the need to adjust the radius for the phi component based on the current latitude, specifically using R cos(θ) for accurate calculations.

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Hi all,

I have a question on the movement of a point on a sphere.

Consider a point P(\theta,\phi) (\theta and\phi are the latitude and the longitude, respectively)moving from a point P_1(\theta_1,\phi_1) to a point P_2(\theta_2,\phi_2) with a constant speed v.

How to find the latitude and the longitude of P(\theta,\phi) (the expression of \theta and \phi) if we suppose that the trajectory is the shortest distance between P_1 and P_2 ?

thanks.
 
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I'm not quite understanding the question. Do you want the angles as a function of time, or one angle as a function of the other?

To start working on the problem, you can find the theta and phi components of the velocity from the known P1, P2 and the radius of the sphere. Then it shouldn't be too bad to write down expressions for the two angles as a function of t , since the speed is constant. The phi equation will take a little more trig than the equation for theta. When you get this far, you should be able to answer your question.
 
thank you for the answer.

I'm not quite understanding the question. Do you want the angles as a function of time, or one angle as a function of the other?

angles as a function of time.

I see how to do it on a circle but on a sphere I don't arrive to visualize the movement.

Just to be sure, on a circle of radius R we have that d \theta=\frac{v}{R} dt, so by integrating we have \theta(t)=\frac{v}{R} t + \theta_1 ?
 
You have the circle approach correct. The same approach will work for the theta component on the sphere. For phi, R will have to be replaced by R cos(theta), but the approach is otherwise the same. You will still have to figure out how to set up the two components of v (theta and phi) to go along a great circle from the initial to the final point.
 
thanks. I still don't see how things work. Any other help ?

I have that x=R \cos(\theta) \cos(\phi), \\ y=R \sin(\theta) \cos(\phi), \\ z=R \sin(\phi)

and \frac{dr}{dt}=v

what am I missing ?. Is \tan(\theta)=\frac{r}{R} ?
 
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