Problem with Lagrange first kind equations

[carllacan]

Homework Statement

Two masses move in a plane restricted to concentric circles with radii R1 and R2. They are joined by a solid rod of length B. Use Lagrange first order equations to find the equilibrium point

Homework Equations

Constraint due to the solid bar: B = R1² + R2² -2R1R2cos(θ1 + θ2), where θ1 and θ2 are the polar coordinates of the masses.

The Attempt at a Solution

My Langrangian is as follows: L = (m/2)(R1²ω1²+R2²ω2²)-mg(sinθ1+sinθ2)
By substituing in this expression http://en.wikipedia.org/wiki/Lagrangian_mechanics#Lagrange_equations_of_the_first_kind I find two equations of motion:
-mgcos(θ1)+mR1²+α1 + R1R2sin(θ1 - θ2)λ1 = 0
-mgcos(θ2)+mR2²+α2 - R1R2sin(θ1 - θ2)λ2 = 0
where α1 and α2 are the angular accelerations of the masses, and the λs are the Lagrange multipliers. I can't solve this equations, though. Is there any method of solving them that I cannot find or is it that my whole procedure is wrong?

 

[CompuChip]

Can you show us what your Lagrangian looks like, that you use to derive these equations of motion?
You denoted the constraint by $L$, but I don't think that expression is your Lagrangian because I don't see a kinetic term.

 

[carllacan]

Sorry, its a bit confusing because the length of the bar is L. I'll change it to B and edit the rest.