User:Hapoth/Scalar gravitation

A scalar theory of gravitation
The basic field equation of a scalar theory of gravitation from Poth published in 2012/2013 is


 * $$ (1)  \frac{1}{c^2} \frac{\partial^2 \Phi}{\partial t^2}  -\nabla^2 \Phi = \kappa \cdot \rho, $$

wherein $$\Phi$$ is the scalar gravitational potential and $$\rho$$ the proper time density of the mass being the source of the gravitational potential and $$\kappa$$ is a constant incorporating the gravitational constant G. $$\kappa$$ is given by
 * $$ (2) \kappa = 4\pi\frac{h}{c^2}G   , $$

wherein h is Planck's constant and c is the veleocity of light.

The proper time density $$\rho$$ is defined by
 * $$ (3) \rho = \frac{\nu_M}{\Delta V}   , $$

wherein $$\nu_M $$ is the frequency of mass M being regarded as an oscillator according to de Broglie and $$\Delta V$$ is the volume in which that mass is situated. Thus $$\rho$$ is a scalar. Hence, (3) is Lorentz invariant.

Thus, the gravitational interaction becomes essentially an interaction between oscillators or between clocks representing masses. That yields directly the dependency of clock rates on the gravitational potential. And as the frequencies for the masses are velocity dependent, the gravitational interaction becomes dependent on the velocities of the interacting masses.

Thus, the heavy mass $$m_h $$ of an inertial rest mass $$m_0 $$ is given by
 * $$ (4) m_h=m_0 \sqrt{1-\frac{v^2}{c^2}} $$

Usually, that can not be noticed, in particular not under common laboratory conditions for determining the gravitational constant G.

The relativistic action integral for a mass $$m_0 $$ moving at velocity v in the gravitational potential of an other mass M at rest becomes
 * $$ (5) A = -\int \left(m_0\,c^2 - \frac{GM}{r}m_0 \, \sqrt{1-\frac{v^2}{c^2}}\right)\, \sqrt{1-\frac{v^2}{c^2}}\cdot dt, $$

That results eventually in the energy H given by
 * $$ (6) H= \frac {m_0c^2} {\sqrt{1-\displaystyle \frac{v^2}{c^2}}} -\frac{G M m_0}{r} \left(1+\frac{v^2}{c^2}\right), $$

Hence, the gravitational potential has become „velocity dependent“. And that eventually results amongst others in the perihelion precession. The geodesic precision and the frame dragging effect as observed by the Gravity B Probe follow also and more.

If two stars of equal mass M orbit each other at the radius r from their center of mass as in a binary star under essentially nonrelativistic conditions, a gravitational wave is created from their retardation difference as seen from a distant observer. That is not a dipole radiation but corresponds to a quadrupole radiation. The radiant power P of that wave is given up to a factor by
 * $$ (5) P \propto \frac{G}{c^5}\, \omega ^6 \,M^2\,r^4, $$

like in the general theory of relativity. The factor appears to be 3/2 times of that obtained from the general theory of gravitation cf. e.g..

The basic field equation (1) can be derived a corresponding Lagrangian and, hence, also the energy density of the gravitational waves which could be directly quantized. As they are scalar waves, their spin is zero.

Comments
In the scalar theory the field equation simply coincides with the common wave equation. In fact, when being applied it is not so simple. It appears that Feynman had such a scalar model in mind but eventually dismissing it; at that time he had apparently no physical entity in mind providing for the gravitation interaction and being porportional to $$\sqrt{1-v^2/c^2} $$. In particular he didn't consider the proper time of a mass particle $$m $$ as a possible entity, albeit it had been commonly know that the Lagrangian $$L_m $$ of a mass particle is given by

L_m=-mc^2\sqrt{1-v^2/c^2} $$ All the less some kind of spatial density of such an entity had he considered. Nevertheless, the scalar theory can be drafted, at least as such, abeit not every mathematical model has to be implemented by nature.