The main parts of the deduction in this subsection is taken from [Chapter 7]P-80.
As seen in the previous section, the Lagrangian is defined as
where T is the kinetic energy and V is the potential energy. In physical coordinates we have, for one particle,
where 
is the potential. Since we in this treatment are considering
comoving particles, we need to transform equation (3.9) to comoving
coordinates, using equations (2.5) and (2.6):
This expression can be simplified somewhat by adding a function
, which will cancel out some of its terms. This seems like a rather
dubious thing to do, but is justified by Hamilton's principle: The time integral of
the function only depends on the values of its variables at the
end-points, where the variation is zero. Therefore, the function does not contribute to
the time integral of the Lagrangian. The function added in this case is given by
which, by subtracting its time derivate from equation (3.10),
results in the reduced Lagrangian:
The second term in equation (3.13) allows the introduction of a homogeneous mass distribution, which in this case would represent the background universe. The Friedmann equations for a flat, pressureless universe is
where 
is the mean background density. Inserting this equation into
(3.13), prompts
The second term is the result of the coordinate change from physical to
comoving, and can be considered as a correction term to the potential due to the
background universe.
Before looking closer at what the expression for the potential is, we need to include more particles than the one treated so far. The reason for this is that in the approximation considered here, the only potential affecting a particle is the one formed by the gravitational field of the other particles in the system. Hence, the Lagrangian for a system of particles is
The potential energy in equation (3.16) can be derived from Poisson's
equation (which in turn can be derived from the Newtonian approximation to general
relativity). Poisson's equation with p=0 and 
is given as
where the `` 
'' subscript indicates that the gradient is to be taken
with respect to the comoving coordinate . The solution of this equation for one
particle can easily be seen to be
For the point particle picture considered here, where a particle at position
is being affected by the particles 
and where 
, the potential can be written as
By introducing this expression for the potential to equation (3.16), the terms containing the cosmological constant cancels out, and we then have the following resulting expression for the Lagrangian, describing a system of particles in an expanding universe:
