One obtains a Maxwell-like structure of gravitation by applying the weak-field approximation to the well accepted theory of general relativity or by extending Newton's laws to time-dependent systems. This splits gravity in two parts, namely a gravitoelectric and gravitomagnetic (or cogravitational) one. Both solutions differ usually only in the definition of the speed of propagation, the lorentz force law and the expression of the gravitomagnetic potential energy. However, only by extending Newton's laws we obtain a set of Maxwell-like equations which are perfectly isomorphic to electromagnetism. Applying this theory to explain the measured advance of the mercury perihelion we obtain exactly the same prediction as starting from general relativity theory. This is not possible using the weak-field approximation approach. Due to the obtained similar structure between gravitation and electromagnetism, one can express one field by the other one using a coupling constant depending on the mass to charge ratio of the field source. This leads to equations e.g. of how to obtain non-Newtonian gravitational fields by time-varying magnetic fields. Unfortunately the coupling constant is so small that using present day technology engineering applications for gravitation using electromagnetic fields are very difficult. Calculations of induced gravitational fields using state-of-the-art fusion plasmas reach only accelerator threshold values for laboratory testing. Possible amplification mechanisms are mentioned in the literature and need to be explored. We review work by Henry Wallace suggesting a very high gravitomagnetic susceptibility of nuclear half-spin material as well as coupling of charge and * Research Scientist, Space Propulsion,