Size of fictional planet based on gravity and density

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SUMMARY

The discussion focuses on calculating the size of a fictional planet with a gravitational force of 1.916G and the same density as Earth, while accounting for 57% water coverage. Key equations include Newton's Law of Universal Gravitation and the formula for mass based on density and radius. The participant aims to understand the implications of these calculations for the planet's rotational and orbital periods, as well as its habitability. The conversation highlights the importance of accurate data regarding star classes and the Habitable Zone for the planet's ecological viability.

PREREQUISITES
  • Newton's Law of Universal Gravitation
  • Understanding of gravitational acceleration and its relation to mass
  • Basic knowledge of planetary density calculations
  • Familiarity with the concept of the Habitable Zone
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  • Research the application of Newton's Law of Universal Gravitation in planetary science
  • Learn about calculating planetary density and its effects on mass and size
  • Explore the concept of the Habitable Zone and its implications for different star types
  • Investigate advanced meteorological phenomena relevant to fictional planetary environments
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Writers, astrophysicists, and world-builders interested in creating scientifically plausible fictional planets, as well as educators and students in planetary science and astronomy.

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Given a planet of the same (relative) density as Earth, and a G-force on said planet of 1.916G, what is the procedure to determine the radius and surface area for such a planet, given it having only 57% water coverage?

I will admit that I am working on this for a book series I started in 2002, but my initial calculations obtained a ridiculously large planet size (17x Earth's surface area). Clearly, my own efforts were (at the time) incorrect equations, but I will admit that my math skills may not be up to the task, although much of the data I originally based the calculations on have been lost. Other planets in my series are Earth-type, albeit different due to the stars they orbit being far different from our Sun.

I want to ultimately be able to explain why such a planet would have a rotational period of 100,000 seconds, and an orbital period of 1,000 of those rotations (roughly 3.17 Terran years), yet be habitable.

Bear in mind that I am not requesting that someone do the work, just help me obtain the knowledge needed to do the work myself for this project.
 
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Awesome project. Have you considered issues concerning the Habitable Zone?

The surface area of a planet is given by the radius (to good accuracy at least). Thus you just need the radius which is included in the equation for Newton's[/PLAIN] Law of Gravity:
F_g = G_N\frac{M_p m}{R^2}
Where G_N is Newton's constant; M_p is the mass of the planet, and m is the mass of the secondary object (e.g. a person feeling the force), and finally R is the radius of the planet.
From Newton's second law:
F = F_g = m a
where 'a' is the gravitational acceleration (on Earth this is usually called 'g'; what you called 'G').
You can combine these equations to remove 'm'. Also, you want a = 1.916 g.
The only other thing you need to solve for is the total mass of the planet, which is determined by its density and size:
M_p = \frac{4\pi}{3} \rho R^3
where \rho is the density (which you can look up on wikipedia for the earth---the amount of surface water won't make any noticeable difference).
 
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zhermes said:
Awesome project. Have you considered issues concerning the Habitable Zone?
Yes, I have, but finding correct data on the different star classes (or an actually-working visual calculator!) has been interesting.
zhermes said:
The surface area of a planet is given by the radius (to good accuracy at least). Thus you just need the radius which is included in the equation for Newton's Law of Gravity:
F_g = G_N\frac{M_p m}{R^2}
Where G_N is Newton's constant; M_p is the mass of the planet, and m is the mass of the secondary object (e.g. a person feeling the force), and finally R is the radius of the planet.
From Newton's second law:
F = F_g = m a
where 'a' is the gravitational acceleration (on Earth this is usually called 'g'; what you called 'G').
You can combine these equations to remove 'm'. Also, you want a = 1.916 g.
The only other thing you need to solve for is the total mass of the planet, which is determined by its density and size:
M_p = \frac{4\pi}{3} \rho R^3
where \rho is the density (which you can look up on wikipedia for the earth---the amount of surface water won't make any noticeable difference).
Okay, that does make sense, insofar as I actually understand what you've mentioned. I would be incorrect if I said I understood all of this. :-) And I acknowledge your near-rebuke regarding g and my incorrect use of the uppercase G for it. LOL
 
The only Habitable Zone "calculator" I've seen at all is useless for what I need; it only shows three very-general star types (basically, small, medium, super-huge) and is leaving me totally unable to figure out other critical data in re: the star classes of these star systems. Based on what I know (the orbital year of two of the planets), I expect one of the stars is a close cousin (so to speak) of the star we ourselves orbit. The one for Regelis, on the other hand, appears to be much hotter, as the HZ is obviously much further out from the star.

Based on the apparent ecology and temperature spreads I have created for Regelis (and the fact that their hurricane classification system has 10(!) steps, not 5, as ours does) I expect that Regelis is closer to the inner edge of its system's HZ than Earth is.

Worst directly-referenced hurricane (in the novels) has been a Class 7, although class 10s have been indirectly referred to, largely in historical context. (Either one would be intensely dangerous, probably destructive beyond anything we have concept of, to be honest.) Closest I can figure for the Class 7 is somewhere around 2000km across, with wind speeds exceeding 250mph, although meterology is decidedly not my strong suit. Been trying to research certain data from well-known storms now for several hours, to little effect. :-\
 

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