How Is Heat Energy Distributed in H2 Combustion?

  • Thread starter Thread starter quasar_4
  • Start date Start date
quasar_4
Messages
273
Reaction score
0

Homework Statement



Consider the combustion of one mole of H2 with 1/2 mole of O2 under standard conditions. How much of the heat energy produced comes from a decrease in the internal energy of the system and how much comes from work done by the collapsing atmosphere? Treat the volume of the liquid water as negligible.

Homework Equations



We've got enthalpy, which is given by H = U + PV. Also, we know from a statement in the book that the enthalpy of formation for the chemical reaction is -286 kJ.

The Attempt at a Solution



If I understand the concept of enthalpy correctly, the idea is that enthalpy is the total energy "cost" for either creating or annihilating something. This consists of the "cost" of energy both from the object itself, and also from the need to make "room" or "collapse" the air around it. So this problem wants me to take the total cost (the enthalpy) and break it down into these constituent parts.

But I don't see at all how to do this. I know intuitively that most of the "cost" comes from the change in internal energy, not the collapse of the atmosphere. But, I don't know how to quantify this.

I am thinking maybe I can do the following, but am hoping for some feedback on it:

I can take the ideal gas law, PV=nRT, and use it to define the volume for 1 mole of water. Assuming the pressure is constant, then I could calculate the work done to "make room" for the liquid water. And then since I know the final enthalpy, I could subtract to get the other part (the change in internal energy).

But is that right? Or do I need to find the volume for 1 mole of H2 and the 1/2 mole of O2, and add them together instead (and would that even be the right way to find the whole volume)? I guess it's not clear to me which I should use.
 
Last edited:
Physics news on Phys.org
never mind, it wasn't bad. I figured it out.
 
Thread 'Need help understanding this figure on energy levels'
This figure is from "Introduction to Quantum Mechanics" by Griffiths (3rd edition). It is available to download. It is from page 142. I am hoping the usual people on this site will give me a hand understanding what is going on in the figure. After the equation (4.50) it says "It is customary to introduce the principal quantum number, ##n##, which simply orders the allowed energies, starting with 1 for the ground state. (see the figure)" I still don't understand the figure :( Here is...
Thread 'Understanding how to "tack on" the time wiggle factor'
The last problem I posted on QM made it into advanced homework help, that is why I am putting it here. I am sorry for any hassle imposed on the moderators by myself. Part (a) is quite easy. We get $$\sigma_1 = 2\lambda, \mathbf{v}_1 = \begin{pmatrix} 0 \\ 0 \\ 1 \end{pmatrix} \sigma_2 = \lambda, \mathbf{v}_2 = \begin{pmatrix} 1/\sqrt{2} \\ 1/\sqrt{2} \\ 0 \end{pmatrix} \sigma_3 = -\lambda, \mathbf{v}_3 = \begin{pmatrix} 1/\sqrt{2} \\ -1/\sqrt{2} \\ 0 \end{pmatrix} $$ There are two ways...
Back
Top