Equations of motion in a free fall with friction

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SUMMARY

This discussion focuses on the equations of motion for an object in free fall with friction, specifically using Newton's second law to derive acceleration and position. The key equation presented is the first-order linear differential equation $$\dot{v} + \frac{\lambda}{m}v = g$$, which describes the motion of the object under the influence of gravitational force and friction. The fundamental theorem of calculus is applied to interpret the integral of a derivative, clarifying the integration process. The conclusion emphasizes that solving this differential equation is essential for accurately modeling the motion of the object.

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  • Newton's second law of motion
  • Basic calculus, including integration and differentiation
  • Understanding of differential equations
  • Friction and its effects on motion
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Homework Statement
A point mass ##m## is dropped from a hight ##z##. Its motion is subject to gravity force and a friction force ##F_f=-\lambda \dot{z}##.
Write the equations of motion for this system.
Relevant Equations
$$F_f=-\lambda \dot{z}$$
I'm stack at the very beginning. If I use Newton's second law to find acceleration and integrate until I find the position, I must face

$$v(t) = \int_0^t g-\frac{\lambda v}{m} dt'=gt-\frac{\lambda }{m} \int_0^t\frac{\partial z}{\partial t}dt$$

But this last term feels pretty weird. I don't know how to interpret it, even though

$$\frac{\partial z}{\partial t}dt = dz$$

If I extract velocity from friction, we get

$$v(t)=\frac{m}{\lambda}(g-a(t))$$

which once again defines a function by its derivative. Should I be solving a differential equation?

In any case, I face two possible ways and I wonder which one, if any, is the correct one. Thank you in advance for the help.
 
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The simple answer is that yes, this is about solving differential equations. Have you studied these?

Your last equation could better be written:

##\ddot{z} = g - \frac{\lambda}{m}\dot{z}##

Note: this is, by definition, the "equation of motion" for the system.

In the first part of your post you effectively integrated this, using the initial conditions, to get:

##\dot{z} = gt - \frac \lambda m z##

Note that your "weird" integral was just the integral of a derivative, which is given by the fundamental theorem of calculus. Note that the derivative should be an ordinary time derivative, not a partial derivative.
 
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Yes you are called to solve a first order linear differential equation here. The first step is to gather the unknown function and all its derivatives to the same side of the equation and write the equation as $$\dot v+\frac{\lambda}{m}v=g$$.
Now we notice that if we multiply the equation by the factor ##e^{\frac{\lambda}{m}t}## then the LHS becomes the derivative of the product ##e^{\frac{\lambda}{m}t}v(t)## so we ll have
$$(e^{\frac{\lambda}{m}t}v(t))'=ge^{\frac{\lambda}{m}t}$$
and from this last equation you can integrate both sides and after some algebraic manipulation you can solve for the unknown function ##v(t)##.
 
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Apart from what has already been said, just a bit of terminology: If there is friction, the object is not in free fall.
 
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