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Kumar Rohan

Physics and Mathematics

Mass and Density of Earth

1. Concept Overview

The mass and density of Earth are fundamental parameters in understanding gravitational attraction, planetary motion, and satellite dynamics.
By combining Newton’s Law of Gravitation with the concept of gravitational acceleration, we can derive the Earth’s mass and determine its average density.


2. Explanation and Mathematical Derivation

Let:

  • Mass of Earth = [M]
  • Radius of Earth = [R]
  • Acceleration due to gravity on the surface = [g]
  • Gravitational constant = [G]

According to Newton’s Law of Gravitation, the gravitational force exerted by the Earth on an object of mass [m] at its surface is:

[ F = \dfrac{G M m}{R^2} ]

But, the same force can also be expressed as:

[ F = m g ]

Equating both expressions of force:

[
m g = \dfrac{G M m}{R^2}
]

Canceling [m] from both sides:

[
g = \dfrac{G M}{R^2}
]

From this, we can find the mass of the Earth as:

[
M = \dfrac{g R^2}{G}
]

$ \displaystyle \because G=6.67\times {{10}^{{-11}}}\text{ N}{{\text{m}}^{\text{2}}}\text{k}{{\text{g}}^{{\text{-2}}}}$ and $\displaystyle g=9.8\text{ m}{{\text{s}}^{{\text{-2}}}}$ and $\displaystyle R=6.4\times {{10}^{5}}\text{ m}$

$\displaystyle \begin{array}{l}\therefore M=\dfrac{{9.8\times {{{\left( {6.4\times {{{10}}^{5}}} \right)}}^{2}}}}{{6.67\times {{{10}}^{{-11}}}}}\\\Rightarrow M=6.018\times {{10}^{{24}}}\text{ kg}\end{array}$

Now, the density of Earth ([\rho]) is defined as:

[
\rho = \dfrac{\text{Mass}}{\text{Volume}} = \dfrac{M}{\dfrac{4}{3} \pi R^3}
]

Substituting the value of [M]:

[
\rho = \dfrac{\dfrac{g R^2}{G}}{\dfrac{4}{3} \pi R^3} = \dfrac{3 g}{4 \pi G R}
]

Thus, the average density of Earth is:

[
\rho = \dfrac{3 g}{4 \pi G R}
]


3. Dimensions and Units

Quantity Symbol Formula Dimensions SI Unit
Mass of Earth [M] [M = \dfrac{g R^2}{G}] [M^1] kg
Density of Earth [\rho] [\rho = \dfrac{3 g}{4 \pi G R}] [M L^{-3}] kg/m³
Gravitational Constant [G] — [M^{-1} L^3 T^{-2}] N·m²/kg²

4. Key Features

  1. The mass of the Earth is determined indirectly using [g], [R], and [G].
  2. The value of [g] varies slightly across the surface due to rotation and shape of Earth.
  3. Earth is not a perfect sphere — its density is not uniform. It increases toward the core.
  4. Average density gives an idea of Earth’s internal structure (mantle, core, crust).
  5. Density is independent of the object’s mass but depends on the Earth’s radius and gravity.

5. Important Formulas to Remember

Concept Formula Remark
Mass of Earth [M = \dfrac{g R^2}{G}] Derived from Newton’s Law of Gravitation
Density of Earth [\rho = \dfrac{3 g}{4 \pi G R}] Derived using volume of a sphere
Relation between [M] and [\rho] [M = \dfrac{4}{3} \pi R^3 \rho] Basic definition of density

6. Conceptual Questions with Solutions

1. How is the mass of the Earth calculated if we cannot measure it directly?

By equating gravitational and weight forces, [M = \dfrac{g R^2}{G}] is obtained. Using known values of [g], [R], and [G], we can compute Earth’s mass.

2. Why does the density of Earth vary with depth?

Earth’s interior has varying composition — lighter materials at the crust and denser metals like iron and nickel near the core.

3. What is the relation between [g] and Earth’s mass?

[g] is directly proportional to [M] and inversely proportional to [R^2]; [g = \dfrac{G M}{R^2}].

4. If the radius of Earth increases, what happens to its density (keeping mass constant)?

Density decreases since [\rho = \dfrac{M}{\dfrac{4}{3}\pi R^3}].

5. How can we conclude that Earth’s core is denser?

The average density (~5.5 g/cm³) is higher than the surface rock density (~2.6 g/cm³), implying denser core materials.

6. What is the unit of gravitational constant [G]?

[N·m²/kg²].

7. On what quantities does [M] depend?

[M] depends on [g], [R], and [G].

8. Does [G] vary with location on Earth?

No, [G] is universal and constant everywhere.

9. How does the concept of density relate to buoyancy in Earth’s layers?

Denser materials sink, while lighter materials float, explaining crust and mantle separation.

10. What is the dimensional formula of [G]?

[M^{-1} L^3 T^{-2}].

11. If [G] were doubled, what happens to [M] for a given [g] and [R]?

[M] becomes half, since [M = \dfrac{g R^2}{G}].

12. What is the significance of average density in astronomy?

It helps compare planets and infer their composition and internal structure.

13. Why is [g] not the same everywhere on Earth?

Due to Earth’s rotation and oblateness, [g] is slightly less at the equator and greater at the poles.

14. Can we calculate the density of Earth using only measurable quantities?

Yes, using [g], [R], and [G] which are all experimentally measurable.

15. How does the derivation involve concepts of differentiation?

Differentiation is used while deriving [g] variation with height and depth. (Refer to topic: **Differentiation**)


7. FAQ / Common Misconceptions

1. Is the Earth’s mass the same everywhere?

Yes, but its *gravitational effect* varies with distance due to [R] and [g].

2. Does Earth’s rotation change its mass?

No, rotation affects effective gravity but not the total mass.

3. Is the gravitational constant [G] affected by altitude?

No, [G] is constant everywhere.

4. Does mass depend on gravity?

No, mass is intrinsic to matter. Weight depends on gravity, not mass.

5. Is density the same as mass?

No, density is mass per unit volume.

6. Why is average density lower than core density?

Because the surface is made of lighter materials.

7. Is the formula [M = \dfrac{g R^2}{G}] applicable to other planets?

Yes, it applies universally for any spherical body.

8. Can [G] be derived mathematically?

No, [G] is determined experimentally (by Cavendish experiment).

9. Does higher density mean stronger gravity?

Not necessarily. Gravity depends on total mass and radius, not just density.

10. Does the derivation assume uniform density?

Yes, for simplicity, the derivation assumes uniform Earth density.


8. Practice Questions (with Step-by-Step Solutions)

Q1. Find the mass of the Earth given [g = 9.8 m/s^2], [R = 6.37 \times 10^6 m], and [G = 6.67 \times 10^{-11} N·m^2/kg^2].

Solution:
[M = \dfrac{g R^2}{G}] [= \dfrac{9.8 \times (6.37 \times 10^6)^2}{6.67 \times 10^{-11}}] [= 5.97 \times 10^{24} kg]


Q2. Calculate the mean density of the Earth using the same data.

Solution:
[\rho = \dfrac{3 g}{4 \pi G R}] [= \dfrac{3 \times 9.8}{4 \pi \times 6.67 \times 10^{-11} \times 6.37 \times 10^6}] [= 5.5 g/cm^3]


Q3. If Earth’s radius were doubled but mass remained the same, what would happen to density?

Solution:
[\rho’ = \dfrac{M}{\dfrac{4}{3} \pi (2R)^3}] [= \dfrac{\rho}{8}]
Hence, density becomes one-eighth.


Q4. Derive the expression for [\rho] in terms of [M] and [R].

Solution:
[\rho = \dfrac{M}{\dfrac{4}{3} \pi R^3}] [= \dfrac{3M}{4 \pi R^3}]


Q5. If [R = 6.4 \times 10^6 m], [M = 5.98 \times 10^{24} kg], find [g] on the surface.

Solution:
[g = \dfrac{G M}{R^2}] [= \dfrac{6.67 \times 10^{-11} \times 5.98 \times 10^{24}}{(6.4 \times 10^6)^2}] [= 9.8 m/s^2]

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