Standard from deeper level:

Alternative:

Mass

$M=\frac{\hslash }{\overline{\lambda }}\frac{1}{c}$ (kg)

$M_g=t_p\frac{l_p}{\overline{\lambda }}$ (collision-time mass)

Energy

$E=M{c}^2$ (joule)

$E_g=l_p\frac{l_p}{\overline{\lambda }}$ (gravitational energy)

Gravitational constant

$G=\frac{l_p^2{c}^3}{\hslash }$

$c_g$ m/s

Non observable (contains GMm)

Gravity force

$F=G\frac{Mm}{R^2}$ (kg∙m∙s⁻²)

$F=c_g\frac{E_g{E}_g}{R^2}$ m/s

$F=c_g^3\frac{M_g{m}_g}{R^2}$ m/s

Observable predictions, identical for the two methods: (contains only GM)

Gravity acceleration

$g=\frac{GM}{R^2}=c^2\frac{l_p^2}{\overline{\lambda }{R}^2}$

$g=c_g^2\frac{E_g}{R^2}=c_g^2\frac{l_p^2}{\overline{\lambda }{R}^2}$

Orbital velocity

$v_o=\sqrt{\frac{GM}{R}}=c\sqrt{\frac{l_p^2}{\overline{\lambda }R}}$

$v_o=c_g\sqrt{\frac{E_g}{R}}=c_g\sqrt{\frac{l_p^2}{\overline{\lambda }R}}$

Orbital time

$T=\frac{2\pi R}{\sqrt{\frac{GM}{R}}}=\frac{2\pi R}{c\sqrt{\frac{l_p^2}{\overline{\lambda }R}}}$

$T=\frac{2\pi R}{c_g\sqrt{\frac{E_g}{R}}}=\frac{2\pi R}{c_g\sqrt{\frac{l_p^2}{\overline{\lambda }R}}}$

Velocity ball Newton cradle

$v_{out}=\sqrt{2\frac{GM}{R^2}H}=\frac{c}{R}\sqrt{2\frac{l_p^2}{\overline{\lambda }}H}$

$v_{out}=\frac{c_g}{R}\sqrt{E_{g}H}=\frac{c_g}{R}\sqrt{2\frac{l_p^2}{\overline{\lambda }}H}$

Periodicity Pendulum (clock)

$T=2\pi \sqrt{\frac{L}{g}}=2\pi R\sqrt{\frac{L}{GM}}=\frac{2\pi }{c}R\sqrt{\frac{L\overline{\lambda }}{l_p^2}}$

$T=\frac{2\pi R}{c_g}\sqrt{\frac{L}{E_g}}=\frac{2\pi }{c_g}R\sqrt{\frac{L\overline{\lambda }}{l_p^2}}$

Frequency Newton spring

$f=\frac{1}{2\pi R}\sqrt{\frac{GM}{x}}=\frac{c}{2\pi R}\sqrt{\frac{l_p^2}{\overline{\lambda }x}}$

$f=\frac{c_g}{2\pi R}\sqrt{\frac{E_g}{x}}=\frac{c_g}{2\pi R}\sqrt{\frac{l_p^2}{\overline{\lambda }x}}$

Gravitational red shift

$z=\frac{\sqrt{1-\frac{2GM}{R_1{c}^2}}}{\sqrt{1-\frac{2GM}{R_2{c}^2}}}-1=\frac{\sqrt{1-\frac{2l_p^2}{\overline{\lambda }{R}_1}}}{\sqrt{1-\frac{2l_p^2}{\overline{\lambda }{R}_2}}}-1$

$z=\frac{\sqrt{1-\frac{2E_g}{R_L}}}{\sqrt{1-\frac{2E_g}{R_h}}}-1=\frac{\sqrt{1-\frac{2l_p^2}{\overline{\lambda }{R}_1}}}{\sqrt{1-\frac{2l_p^2}{\overline{\lambda }{R}_2}}}-1$