High School Newton's Constant in Higher Dim. Spacetimes, Velocity of Light=1

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Setting the velocity of light to unity, the discussion explores the implications of Newton's constant in higher-dimensional spacetimes. It highlights that while the curvature scalar's dimension remains constant, the matter Lagrangian's dimension changes with the number of dimensions, leading to a different dimension for Newton's constant in non-four-dimensional spaces. The modified form of Newton's Law of Gravity in d-dimensional space is presented, showing how it relates to Laplace-Poisson's equation. By equating gravitational force with Newton's Second Law, the derived dimension of G in MKS units is discussed. The conversation references relevant literature for further exploration of these concepts.
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In our spacetime, Newtons constant has dimension length/energy (the velocity of light set unity). How is this in a different number of dimensions?
In the following, I set the velocity of light unity.
I refer to theories of gravities in higher-dimensional spacetimes.

Newton` s constant converts the curvature scalar with dimension ##lenght^{-2}## into the matter Lagrangian with dimension ##energy/length^3##. So its dimension is ##length/energy##. But in ##d##-dimensional spacetime the dimension of the curvature scalar would remain unchanged, whereas the matter Lagrangian would have dimension ##energy/length^{d-1}##. So, for ##d \ne 4##, Newtons constant would have a different dimension. Is this correct?
 
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In d-dimensional space, Newton's Law of Gravity would be F_g=\displaystyle G\frac{m_1m_2}{r^{d-1}}
(which follows from Laplace-Poisson's equation in d-dimensions).
By equating that with Newton's Second Law, which is taken to be dimensionally-independent,
we get
in MKS units, for d-dimensional space, [G]=\displaystyle \frac{1}{kg} m^d s^{-2}.

https://en.wikipedia.org/wiki/Gravitational_constant

See: J.D. Barrow's
(1983) Dimensionality
Philosophical Transactions of the Royal Society of London.
Series A, Mathematical and Physical Sciences 310: 337–346 http://doi.org/10.1098/rsta.1983.0095
(See also https://www.jstor.org/stable/37418 )

It seems this following blog summarizes some of the details:
https://thespectrumofriemannium.wordpress.com/2012/11/18/log054-barrow-units/
 
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MOVING CLOCKS In this section, we show that clocks moving at high speeds run slowly. We construct a clock, called a light clock, using a stick of proper lenght ##L_0##, and two mirrors. The two mirrors face each other, and a pulse of light bounces back and forth betweem them. Each time the light pulse strikes one of the mirrors, say the lower mirror, the clock is said to tick. Between successive ticks the light pulse travels a distance ##2L_0## in the proper reference of frame of the clock...

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