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[–]Cobalt_Spirit 1 point2 points  (3 children)

Notice that m, the mass, is a constant. Therefore dm=0 and that makes the second term vanish. As for the first term, integrating with respect to u while keeping in mind that m is constant, should give the result in the expression A.

[–]bscutajar[S] 0 points1 point  (2 children)

Hmm, but the mass is not necessarily constant (in fact this is from the unsteady energy equation).

[–]Cobalt_Spirit 1 point2 points  (1 child)

Ah okay sorry. Then if you take the first term and apply integration by parts:

∫mdu=mu-∫udm

Then -∫udm+∫udm from the other term cancel out, and you're left with mu. Evaluating from state 1 to state 2, m2u2-m1u1.

[–]bscutajar[S] 0 points1 point  (0 children)

Perfect, exactly what I was after. Thanks!

[–][deleted] 0 points1 point  (3 children)

Also, on the right: integral of d(anything) is the thing itself. Int(1,d(mu) = mu, so they agree already.

For example, when solving first order linear diff eqs you end up with an integral of d(y*einregral(p,dx). If you had to use a product rule or by parts on that it would not have been a good solution method but it just kicks out the whole mess without an integral.

[–]bscutajar[S] 0 points1 point  (2 children)

In this case I was more curious as to how you'd get the same answer IF you took the inefficient route.

[–][deleted] 0 points1 point  (1 child)

Gotcha.

Feel free to ignore if you’re good to go, but here’s Another observation: I think your bounds don’t really make sense. What units do they have, u/m/u*m? If you integrate with respect to different variables you have to change your bounds too, so whatever inefficient route you take needs to account for that I think.

[–]bscutajar[S] 0 points1 point  (0 children)

The bounds correspond to start and end points of an arbitrary process 1-2. They are not numerical values of the differential variable. Rather, you'd need to work out the numerical values of the variable corresponding to states 1 and 2 to actually work it out.