Deriving an Expression of an Object in Free-Fall on Mars

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SUMMARY

This discussion focuses on deriving the velocity expression for an object in free fall on Mars, considering the drag force and gravitational acceleration. The drag force is defined by the equation $$F_d = \frac{C_d A \rho_M v^2}{2}$$, where $$C_d$$ is the drag coefficient, $$A$$ is the reference area, and $$\rho_M$$ is the air density on Mars. The derived velocity function is $$v(m,t,r) = \frac{15.083}{r} \sqrt m \text{ tanh} \frac{0.285211r (C-t)}{\sqrt m}$$, but complications arise when attempting to solve for the constant C under specific conditions, leading to questions about the validity of the integration approach.

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  • Understanding of classical mechanics, particularly free fall dynamics.
  • Familiarity with calculus, especially integration techniques.
  • Knowledge of fluid dynamics concepts, including drag force.
  • Basic understanding of Martian environmental conditions, such as gravity and air density.
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  • Study the derivation of drag force equations in different atmospheric conditions.
  • Learn about variable mass systems and their impact on motion equations.
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lithium123
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Hi everyone. I'm trying to derive an expression of the velocity of an object in free fall on Mars, and I am having trouble. Here is what I've done so far:

Drag on Mars can be expressed as
$$F_d = \frac{C_d A \rho_M v^2}{2}, $$ where C_d denotes the drag coefficient, A the reference area, and rho_M the air density on Mars. Let $$k = \frac{C_d A \rho_M}{2}$$.

Suppose the lander is in free-fall. Considering its two main forces, the lander hence has an equation of motion
\begin{align*}
F_d - mg &= m \hspace{1mm}\frac{dv}{dt} \\
\frac{k}{m}v^2 - g &= \frac{dv}{dt} \\
\int {dt} &= \int{\frac{dv}{\frac{k}{m}v^2 - g}}
\end{align*}
Applying the substitution $$v = u \sqrt{\strut\frac{gm}{k}}$$, the equation can then be written as

\begin{align*}
t &= \int \frac{1}{\left(u^2-1\right)\sqrt{\frac{gk}{m}}} du \\
&= -{\sqrt{\frac{m}{gk}}}\int \frac{1}{-u^2+1} \hspace{1mm} du \\
&= -{\sqrt{\frac{m}{gk}}} \hspace{1mm} \text{arctanh} \hspace{1mm} u
\end{align*}
And substituting back, $$u = v \sqrt{\strut\frac{gm}{k}}$$ and expressing this as a function $v(t)$ gives us $$v(t) = \sqrt{\frac{gm}{k}} \hspace{1mm} \text{tanh} \hspace{1mm} ( \hspace{0.5mm}\sqrt{\frac{gk}{m}} (C-t)).$$ Now, we must find the values of the constants in our above expression.

From information about our object, we have $$ k = \big(\frac{1}{2}\big) (0.67)(\pi r^2)(0.0155) \approx 0.0163 r^2 \hspace{1mm} \frac{\text{kg}}{\text{m}}.$$
The force of $g$ on Mars is expressed as $$g = 3.711 \frac{\text {m}}{\text{s}^2}.$$
Note m and r are not constants and vary. Our velocity expression can then be written as $$v(m,t,r) = \frac{15.083}{r} \sqrt m \hspace{1mm}\text{ tanh} \hspace{1mm}\frac{0.285211r (C-t)}{\sqrt m}.$$ We can determine the constant C by noting that our object has a mass of 600 kg, begins the landing phase at $t = 0$ at a speed of 250 m/s with a cross sectional area of 81pi, or $$v(600, 0, 9) = 250$$.

I have run into a problem here. If I use v(600, 0, 9) = 250, the C value turns out to not be real. Why is this, and is it still possible to get an expression for v(m,t,r) with this special condition?
 
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Hi @lithium123:

I don't think I can offer much help, but I think the integration of
t = ∫... du is flawed. You assumed that m is independent of u, and I don't think that is correct. Both m and u are functions of t.

If I am wrong about this, I apologize.

ADDED

I am not sure why you said
Note m and r are not constants and vary.​
m might vary if some fuel is used to control attitude while falling.
I think you intended r to be ρ.

In any case, gk/m is a function of t, so the integral with respect to t should have an integrand of
√m/gk

Regards,
Buzz
 
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