Lagrangian in cartesian and polar

In summary, the conversation discussed solving a Lagrangian equation in Cartesian and polar coordinates, and deriving the Lagrange equations of motion in both systems. The solution in Cartesian coordinates was found to be r(t)=1 and θ(t)=t when expressed in polar coordinates, and it was shown that this solution satisfies the polar equations of motion.
  • #1
jameshaley
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0

Homework Statement



Consider the following Lagrangian in Cartesian coordinates:
L(x, y, x', y') = 12 (x^ 2 + y^2) -sqrt(x^2 + y^2)

(a) Write the Lagrange equations of motion, and show that x = cos(t);
y =sin(t) is a solution.

(b) Changing from Cartesian to polar coordinates, x = r cos ; y = r sin ,
show that the Lagrangian becomes

L(r;θ ; r';') = 1/2 (r'^2 + r^2θ^2)- r;

and hence fi nd the Lagrange equations in polar coordinates.

(c) Show that the solution given in Cartesian coordinates in (a) is still a
solution when expressed in polar coordinates.


Homework Equations



d/dt(∂L/∂x')-∂L/∂x
L=T-V


The Attempt at a Solution



d/dt(∂L/∂x')-∂L/∂x=x''-x/sqrt(x^2+y^2)=0
d/dt(∂L/∂y')-∂L/∂y=y''-y/sqrt(x^2+y^2)=0

got both as i think there is 2 degrees of freedom

put in x=cost, y=sint
x'=-sint, x''=-cost
y'=cost y''=-sint

put these it above i get

-cost-cost/sqrt(sint^2+cost^2)=-2cost
-sint-sint/sqrt(sint^2+cost^2)=-2sint

for a this is where i think i get stuck.

b) x=rcosθ,x'=cosθr'-rsinθθ'
y=rsinθ,y'=sinθr'+rcosθθ'

x'^2+y'^2=r'^2+r^2θ'^2
sqrt(x^2+y^2)=r

there for
L(r,θ,r',')=(1/2)(r'^2+r^2θ'^2)-r

and so

d/dt(∂L/∂r')-∂L/∂r=r''-rθ'^2+1
d/dt(∂L/∂θ')-∂L/∂θ=r'^2θ''

and that's where i get stuck. This is a practise exam question, and i want to make sure I am going the right way about it. Any help would be much appropriated
 
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  • #2
d/dt(∂L/∂x')-∂L/∂x=x''-x/sqrt(x^2+y^2)=0
d/dt(∂L/∂y')-∂L/∂y=y''-y/sqrt(x^2+y^2)=0

worked out where I went wrong on this, missed the minus'

d/dt(∂L/∂x')-∂L/∂x=x''+x/sqrt(x^2+y^2)=0
d/dt(∂L/∂y')-∂L/∂y=y''+y/sqrt(x^2+y^2)=0
 
  • #3
jameshaley said:
d/dt(∂L/∂x')-∂L/∂x=x''-x/sqrt(x^2+y^2)=0
d/dt(∂L/∂y')-∂L/∂y=y''-y/sqrt(x^2+y^2)=0

worked out where I went wrong on this, missed the minus'

d/dt(∂L/∂x')-∂L/∂x=x''+x/sqrt(x^2+y^2)=0
d/dt(∂L/∂y')-∂L/∂y=y''+y/sqrt(x^2+y^2)=0

Yes. And you should probably fix your initial Lagrangian up, it's got some confusing typos. You mean L=(1/2)*(x'^2+y'^2)-sqrt(x^2+y^2). Any other questions? Your Cartesian solution is r(t)=1 and θ(t)=t in polars. It should be pretty easy to show that satisfies your polar equations of motion.
 
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  • #4
Thank you for the reply''Your Cartesian solution is r(t)=1 and θ(t)=t in polars.''

I'm struggling a bit to understand why this is.

r(t)=1
=sqrt(x^2+y^2)
=sqrt((cost)^2+)sint)^2)

And for θ(t)=t
I thought arctan(y/x)
 
  • #5
jameshaley said:
Thank you for the reply''Your Cartesian solution is r(t)=1 and θ(t)=t in polars.''

I'm struggling a bit to understand why this is.

r(t)=1
=sqrt(x^2+y^2)
=sqrt((cost)^2+)sint)^2)

And for θ(t)=t
I thought arctan(y/x)

I'm not sure what you are thinking. If you want x=cos(t) and y=sin(t) and x=r(t)cos(θ(t)) and y=r(t)sin(θ(t)) then surely putting r(t)=1 and θ(t)=t will do the job just by inspection. If you want to follow through with your calculation, arctan(y/x)=arctan(sin(t)/cos(t))=arctan(tan(t))=t.
 
Last edited:
  • #6
Yep it's just all clicked!

I understand now. Thank you
 

1. What is a Lagrangian in cartesian and polar coordinates?

The Lagrangian is a mathematical function used in classical mechanics to describe the dynamics of a system. In cartesian coordinates, it is defined as the difference between the kinetic and potential energies of a system. In polar coordinates, it includes an additional term that accounts for the effects of the system's rotation.

2. How is the Lagrangian used in classical mechanics?

The Lagrangian is used to derive the equations of motion for a system, known as the Euler-Lagrange equations. These equations describe the evolution of a system over time and can be used to solve for the positions and velocities of all particles in the system at any given time.

3. Can the Lagrangian be used in other branches of physics?

Yes, the Lagrangian can also be used in other branches of physics, such as quantum mechanics and field theory. In these contexts, it is used to describe the dynamics of particles and fields, respectively, and is an important tool in understanding the behavior of complex physical systems.

4. What advantages does using the Lagrangian have over other methods?

One advantage of using the Lagrangian is that it simplifies the mathematical equations used to describe a system, making it easier to solve for the system's behavior. It also allows for a more intuitive understanding of the physical principles at play, making it a useful tool for both theoretical and experimental physicists.

5. Are there any limitations to using the Lagrangian?

While the Lagrangian is a powerful tool in classical mechanics, it does have some limitations. It is most useful for describing systems with a small number of particles and does not work well for systems with a large number of interacting particles. Additionally, it may not accurately describe systems with complex interactions or systems that are highly nonlinear.

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