> For the complete documentation index, see [llms.txt](https://space-axolotls.gitbook.io/space-axolotls-docs/llms.txt). Markdown versions of documentation pages are available by appending `.md` to page URLs; this page is available as [Markdown](https://space-axolotls.gitbook.io/space-axolotls-docs/math/physics-of-asteroid-impacts-and-crater-formation.md).

# Meteor Impact Calculations

#### Asteroid Impact with the Ground

The kinetic energy of the asteroid is:

<figure><img src="/files/uBaY6uFz5AYHlEckG6Ng" alt=""><figcaption></figcaption></figure>

Where $$D\_a​$$, $$ρ\_a$$, $$V\_a$$, ρma are the diameter, density, velocity, and mass of the asteroid. This energy is what excavates, melts, vaporizes, and launches the ground material.

The density of the ground is

$$ρ\_s​$$, and the energy transfer depends on the ratio:

<figure><img src="/files/wKM5P48JMPZL29tRxX9R" alt="" width="64"><figcaption></figcaption></figure>

Through dimensional analysis, the asteroid's variables can be related to g, which affects the crater's size:

<figure><img src="/files/urYXrz9CmRlt1gsautak" alt=""><figcaption></figcaption></figure>

This $$π\_2​$$ is known as a "pi-group".

The initial crater diameter, Dc, is calculated with an empirical law from experiments:

<figure><img src="/files/fMjWZOXNFohdzfUk3gCi" alt=""><figcaption></figcaption></figure>

The typical experimental constants for impacts against the Earth are

$$K\_1​≈1,μ≈0.55,v≈0.17$$.

Craters tend to collapse and obtain a final diameter $$D\_f$$.

$$D\_f​≈1.25D\_c​$$

The amount of excavated mass will be the excavated volume multiplied by the ground's density $$(x = exc)$$.&#x20;

#### Ejected Mass and Velocity Formulas

The excavated mass is calculated as:

<figure><img src="/files/sR4uwZRFIYsDxFAbk5Z6" alt=""><figcaption></figcaption></figure>

Regarding the ejection velocity, according to experimental data, it can range from a minimum velocity:![](/files/ezFJNFnsc6pjN0UMhUSI)

&#x20;to a maximum ($$v\_M​$$): ![](/files/R1k4fM6werQmiN7Zi04M)

Where $$c=0.5$$.

Height of Ejected Material

The mass that achieves a velocity greater than a certain ejection velocity ($$vy​ = eyection$$) is given by:

<figure><img src="/files/eiINGor4jJiUf2AHUZz9" alt=""><figcaption></figcaption></figure>

Where b≈ 2 to 3 and $$v\_y​$$ ranges from $$v\_m​$$ to $$v\_M​$$.

The fraction of mass that could reach the stratosphere must achieve a velocity $$v\_s(s =  est)$$.

<figure><img src="/files/RkRDuy4yq5CNug6uiKys" alt=""><figcaption></figcaption></figure>

Where $$h\_s​$$ is the height of the stratosphere. That fraction is:

<figure><img src="/files/VOG9lv5CdphBzDERFLTU" alt=""><figcaption></figcaption></figure>

For the fraction of mass that reaches orbit, the same logic is applied but with the escape velocity

$$v\_e​=11,200 m/s​$$.  Where e = escape.

<figure><img src="/files/SHnC9VKCwgCBI3ibJrVn" alt=""><figcaption></figcaption></figure>

#### Page 3: Mass Ejected to the Atmosphere and Space

These mass fractions are multiplied by the excavated mass to determine how much remains suspended in the atmosphere, reaches the stratosphere, and how much reaches orbit.

* What remains suspended in the atmosphere (Mass reaching the stratosphere):

  <figure><img src="/files/V3g0Cx6a5oS8awkCAjox" alt=""><figcaption></figcaption></figure>
* What goes out into space (Mass reaching orbit):

  <figure><img src="/files/97YEWUOZnaeJFytti7zx" alt=""><figcaption></figcaption></figure>

### &#x20;Air Geometry and Mass

Geometry and Mass Formulas.

<figure><img src="/files/vR3wBdxQkQZVywx75EZ7" alt=""><figcaption></figcaption></figure>

### International Standard Atmosphere (ISA)

#### General Temperature Formula

<figure><img src="/files/lWpKEpNipHqQjFuL3tLs" alt=""><figcaption></figcaption></figure>

#### Detailed Atmospheric Pressure and Density Formulas

**Temperature at altitude**

<figure><img src="/files/bXQRcrijkA0L9vzpKWGT" alt=""><figcaption></figcaption></figure>

**Pressure at altitude**

<figure><img src="/files/dW1SubKfh9TqOB2D23La" alt=""><figcaption></figcaption></figure>

**Density at altitude**

<figure><img src="/files/QZCpSjnccc6Xfcw6sEMX" alt=""><figcaption></figcaption></figure>

**Sea-level extrapolation for negative altitudes**

<figure><img src="/files/1oipPp7UdTAzD506Qo34" alt=""><figcaption></figcaption></figure>

### Meteor Atmospheric Entry

#### Geometry and Energy

<figure><img src="/files/R8Ohh1RvCo7R5NZyquzh" alt=""><figcaption></figcaption></figure>

#### Velocity (Step Integration)

<figure><img src="/files/0lRuz24ikUuu6KWjWIDv" alt=""><figcaption></figcaption></figure>

### Impact Crater Calculations

#### Crater

<figure><img src="/files/lyjUAD5TNlxyEPS5HHFX" alt=""><figcaption></figcaption></figure>

#### Ejecta

Minimun Ejection Velocity $$(Vmin)$$

<figure><img src="/files/s4aqXpbpdcd65lkEAWIP" alt=""><figcaption></figcaption></figure>

Ejection Percentage $$(P\_v)$$

<figure><img src="/files/mYKO6CTMqkn21mLnh2nC" alt=""><figcaption></figcaption></figure>

### Gravitation and Entry Velocity

**Gravitational Acceleration by Altitude**

<figure><img src="/files/sDuoG1fLO32T36omweDn" alt=""><figcaption></figcaption></figure>

#### Atmospheric Entry Velocity

<figure><img src="/files/EnPVkUORJuVQIspn3yJt" alt=""><figcaption></figcaption></figure>

### Water Impact (Tsunamis)

<figure><img src="/files/S1awN7JVR7JmRJQws81M" alt=""><figcaption></figcaption></figure>


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