silento
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hold on I think I got something
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The discussion focuses on solving a differential equation involving the separation of variables and integration in the context of physics. Participants clarify the relationship between velocity (v), position (x), and forces, specifically addressing the drag force and its non-constant nature. The equation discussed is of the form $$\varphi - \beta v^2 = m v\frac{dv}{dx}$$, with a substitution of $$u = \varphi - \beta v^2$$ to facilitate integration. The final goal is to derive the change in position (∆x) as velocity transitions from 120 m/s to 0 m/s.
PREREQUISITESStudents and professionals in physics, engineering, and mathematics who are working on problems involving differential equations and motion analysis.
I was looking for this:silento said:du= -2Bvdv
look at the RHS of that result, and compare it to the RHS of your original equation. Notice anything?silento said:Alright...that makes sense. Interested to see where we go from here
I meant examine similarities between post 16 and post 32.silento said:looks like we moved that drag force over to the right hand side
luckily, that's just a constant... Quite literally solve for ##v \frac{dv}{dx}## in terms of ##\frac{du}{dx}## in post 32, and plug it into post 16 equation. Don't forget about the ##u## substitution made in 16 either. If you do it correctly, watch the equation transform into a butterfly.silento said:View attachment 340974 . however -2B is in place of the mass
Try again. everything should be in terms of ##u,x##..no more ##v## in the equation.silento said:
in post 16 eqn, substitute on the LHS to get rid of ##v## and the constant... remember I defined ##u = \varphi - \beta v^2##.silento said:From post 32 View attachment 340976 then I plugged that into the answer from post 16 in place of vdv/dx. I don't see where I'm going wrong
Solve for ##u(x)## from the resulting ODE. After you’ve done that you can change back to ##v## and it’s values etc…silento said:correct me in i'm wrong, but we are going to move the du to the LHS. Then we can sub v back in for u. Then velocity would be the only variable on the LHS along with the constants. On the right hand side it would just be 1/-2Bdx which is just constants???
Ordinary differential equation. The equation we just developed. Linear. separable, ODE.silento said:Im sorry but what's ODE?
Integrate ##u## with limits ##u_f, u_o##. You can leave the ##x## the way it is assuming ##x_o=0##. Otherwise good.silento said:\begin{equation}
\ln|u| = -\frac{2B}{m}x
\end{equation}
##u## is not ##v##. Go back and look at what ##u## is…silento said:so let me think about this. u is velocity from 54 m/s to 0 m/s. xf is what I'm solving for. Would I only integrate the LHS?
Now combine the logssilento said:\begin{equation}
\ln|u_f| - \ln|u_o| = -\frac{2B}{m}x
\end{equation}