Problems with the Standard Model

Special relativity unified electricity and magnetism into the electromagnetic force. Glashow, Salam, and Weinberg unified the electromagnetic force and weak force into the electroweak force. Extrapolation of present experimental data predicts that the behavior of the electroweak force and the strong force will become the same around 10^16 GeV .This results in the standard model, successfully incorporating the Lie groups SU(3)xSU(2)xU(1). But where is gravity in all of this? Gravity is expected to play a role at higher energies such as 10^19 GeV; this energy scale is the Planck Mass 3. The problem is, the relationship between these forces is not known. The two theories,
general relativity and the standard model's quantum field theory, are incompatible. The renormalizations that normally occur in the equations are not present 4. For example, the force between gravitons is found to be
infinite, a nonsensical answer 2. This incompatibility can generally be avoided based on the applications of the two theories. General relativity is applied to massive structures such as stars. Quantum mechanics is applied to minute structures such as electrons and quarks.Usually the application of one precludes the application of the other. There are instances where both are required, however. Singularities and the state of the universe before the big bang combine enormous masses with minute distances; thus both theories are needed but only one can be used. One of the major problems occurs with quantum field theory's treatment of particles as points of zero size. In this case, interactions occur at zero distance--a distance at which the math fails to normalize 1.