## Appendix A: analytical construction of displacement vectors for Model I
In this section we exemplify how special solutions to (2) can be constructed by using a set of local forms which provide first integrals of the seven Poisson equations (2f-l). Let us consider a simple plane-wave model for the initial peculiar-velocity potential , which was studied earlier by Moutarde et al. (1991): The amplitude plays the role of the perturbation parameter here and is related to the total amplitude of the density contrast as . The amplitudes allow for triaxial deformations of the model; one has to choose in order to keep the r.m.s. amplitude of the same. In this paper we shall use , since different amplitudes give no further information about internal structures of the model. Although the model (A.1a) is simple, it has no symmetries which destroy the generic feature of the singularites formed like plane or spherical symmetry would do. The structure of the cluster formed will only retain reflection and rotational symmetries manifest in the potential (A.1a) for our choice of amplitudes. As, e.g., demonstrated in (Buchert & Ehlers 1993) for a similar two-dimensional model, we have with models like (A.1a) the possibility of studying principal kinematical features of a generic collapse such as the formation of cusped caustics, interconnected network structures, infall of matter onto the cluster. Additionally, internal differentiation of a multi-stream system resulting in a hierarchy of shell-crossings, which are attributed to a generic feature of a gravitational collapse, can be demonstrated nicely with this model. The model has periodic boundary conditions which makes it accessible for numerical treatment. From (A.1a) we have for the first order displacement vector: We now scetch a procedure how to construct the higher-order
potentials from this initial condition. The procedure is based on a
list of
According to The local form (A.2) is constructed such that its divergence agrees with the source term in (2g), its curl is, however, in general non-zero, it only vanishes if (A.2b,c,d) are statisfied. Inserting the potential (A.1a) we immediately obtain the second-order displacement vector: The vector (A.2e) is curl-free as can be easily demonstrated, so it obeys the constraints (A.2b,c,d) necessary to admit a potential. This potential can now be guessed from (A.2e) to be of the form
Similarily, we can ask for a local vector form whose divergence
agrees with the source term in equation (2h). An expression given in
Buchert (1994, has the property where are the subdeterminants of the tensor (a comma always denotes partial derivative with respect to Lagrangian coordinates). The following constraints have to be satisfied in order that be curl-free: Inserting the potential (A.1a) into (A.3a) gives for the displacement vector Again, the vector (A.3e) is found to be curl-free which renders the contraints (A.3b,c,d) satisfied. A potential generating this displacement is again easily found from (A.3e). It reads
The source term in (2i) which describes the longitudinal part of
the interaction of first- and second-order perturbations has a similar
structure as the second-order source term (2g). We are able to
construct a local form by analogy (Buchert & Ehlers 1993,
Here, the linear combination of the two possible integrals as a
general integral has to be taken, where . In
order to satisfy the requirement that the vector (A.4a) be a solution
of the Poisson equation (2i), we have to assure that it is curl-free
which implies (Buchert & Ehlers 1993, As can be seen from (A4), we have to determine the parameters and suitably in order to fulfil the constraints (A.4b,c,d). Although, we can find the two first integrals for the potential (A.1a), the resulting vectors are not curl-free. It is a matter of some algebra until one finds the correct linear combination of the two vectors, which is curl-free. This can be achieved by first guessing the form of the potential from the two vectors. It is clear that, in general, we will not be successful. We obtain , . Thus, the displacement vector reads with
Finally, we ask for a first integral of the transverse part of the
interaction vector (2j,k,l). In (Buchert 1994, has the property We have to assure . In order to satisfy the requirement that the vector components (A.5a,b,c) be solutions of the Poisson equations (2j,k,l), we have to guarantee that the vector field is source-free which implies after using well-known vector identities Again, we find the two integrals after inserting the potential (A.1a) to be not source-free. We have to determine the correct linear combination of the two integrals. As in the longitudinal case we first guess the form of the vector potential from the two integrals. We are successful with the parameters , and , but we have to add another function such that the total displacement is source-free. The potential is given by (This is possible, since the local forms discussed above are only determined up to the gradient of some potential, see Buchert 1994). The vector displacement reads with the vector-potential
For the following discussion we need the explicit expressions of the source terms in the solution (2) for the special model (A.1a). We derive From the generating functions constructed above we infer the following property: except for the longitudinal part of the interaction term, the perturbation potentials obey equations which are typical for bound systems: Recall that the condition (A.7a) implies for an initially irrotational peculiar-velocity field ; , i.e., the motion is initiated to follow the gradient of the density-contrast field. At the third order the evolution model shows that this property of the flow is lost. (The algebraic program we used to compute the perturbation potentials for Model II also reproduces the perturbation potentials derived here.) © European Southern Observatory (ESO) 1997 Online publication: July 8, 1998 |