- #36
erobz
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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
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 teh 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}
exponentiate both sides, and move ##u_o## over to the right hand side.silento said:\begin{equation}
\ln\left|\frac{u_f}{u_o}\right| = -\frac{2B}{m}x
\end{equation}
Delimiters? And you can lose the absolute value bars. The RHS is always positive.silento said:am I typing something wrong?
The absolute value bars are no longer necessary. The RHS is always positive. Move ##u_o## over.silento said:\begin{equation}\left| \frac{u_f}{u_o} \right| = e^{-\frac{2B}{m}x}\end{equation}
Now evaluate ##u_f## and ##u_o## using the corresponding ##v_f## and ##v_o##. Make sure you are evaluating ##u##. I repeat ##u## is not ##v##.silento said:\begin{equation}u_f = u_o \cdot e^{-\frac{2B}{m}x}\end{equation}
Oh I just realized you are trying to solve for ##x##, not ##v##. Anyhow just finish it out, the solve for ##x##. I realized this is undoing a few steps. My bad.erobz said:Now evaluate ##u_f## and ##u_o## using the corresponding ##v_f## and ##v_o##. Make sure you are evaluating ##u##. I repeat ##u## is not ##v##.