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My real life problem is to calculate initial translational and angular velocities of a vehicle in a loss of control to a stop. (The vehicle will translate and rotate about it's center of mass.)

Initial strategy is to use energy-work theorem, therefore:

$K = W$

where $K$ is the initial kinetic energy and $W$ is the work due to friction (F) between the tires and the road surface (assume that's the only external force at play), therefore:

$\frac 1 2 mv^2 + \frac 1 2 I\omega^2 = \int F\,ds + \int \tau\,d\theta$

Assume I know how to calculete the RHS of the equation. The problem with this, is that i have two variables($v$ and $\omega$) with only one equation.

The question is: Is it valid to write two different equations, one for rotation and the othe for translation, as following?

$\frac 1 2 mv^2 = \int F\,ds$

$\frac 1 2 I\omega^2 =\int \tau\,d\theta$

This way i would be able to solve for $v$ and $\omega$, but I am not so sure i can do it without violating some underliying principle..

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  • $\begingroup$ I think it is fine because the total energy is the addition of its two components, which are integrated over their own domain, that is independent of each other. $\endgroup$
    – r13
    May 1 at 15:50
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I would look at it like this

Let's call the friction force of wheel a, Fa

then the contributory effect of this force is two parts one part imparting negative acceleration and the other part which is the negative torque resisting car spin, $T=F_a*da \ $ with "da" being the distance of the tire to the CG of the car.

This will together with the other 3 wheels give a set of four differential equations matrix.

$$F_adt=-(m \alpha+I*da)dt$$

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