The Pauli principle is not a force b/c it is already present in the free theory w/o any specific interaction; it holds purely algebraically w/o specifying a dynamics i.e. w/o specifying a Hamiltonian.
Suppose you have fermionic creation and annihilation operators [itex]b_i^\dagger[/itex] and [itex]b_i[/itex] with the usual anti-commutators. Here 'i' is a general index containing all relevant numbers specifying a state like momentum, spin, isospin etc.
The relevant identity which follows from the anti-commutators is
[tex]\left(b_i^\dagger\right)^2 = 0[/tex]
It says that you cannot create a two-particle state with two fermions having both the same state 'i'.
Of course you can construct arbitrary complex interaction terms
[tex]\sum_{ijk, \ldots pqr \ldots}h_{ijk, \ldots pqr \ldots} b_i^\dagger b_j^\dagger b_k^\dagger \ldots b_p b_q b_r \ldots[/tex]
but in all those interactions every diagonal term with (e.g.) i=j vanishes
[tex]h_{iik, \ldots pqr \ldots} b_i^\dagger b_i^\dagger b_k^\dagger \ldots b_p b_q b_r \ldots = 0[/tex]
So the Pauli principle eliminates all these terms from the theory w/o requiring a specific interaction; the number hiik...pqr... need not be zero; it's the anti-commutator itself that makes this term vanish.