CHM 132 Chapter Notes - Chapter 9: Thermodynamics, Enthalpy, Ideal Gas

19 views2 pages

Document Summary

Is a state function: h = e + pv (cid:894) h = e + (cid:894)pv(cid:895)(cid:895, u(cid:374)de(cid:396) (cid:272)o(cid:374)sta(cid:374)t p(cid:396)essu(cid:396)e, the (cid:396)ea(cid:272)tio(cid:374) of h (cid:449)ould (cid:271)e h = e + p v. At the sa(cid:373)e ti(cid:373)e, e = (cid:395)p p v. Combining the two equations you get that h = (cid:395)p: at (cid:272)o(cid:374)sta(cid:374)t p(cid:396)essu(cid:396)e, h = qp change i(cid:374) e(cid:374)thalp(cid:455) is the flo(cid:449) of heat. Molar heat capacity the energy required to raise the temperature of 1 mole of that substance by 1k: of an ideal gas, the molar heat capacity is 3r/2. Heating an ideal gas at constant volume: whe(cid:374) the(cid:396)e is (cid:272)o(cid:374)sta(cid:374)t (cid:448)olu(cid:373)e the(cid:396)e is (cid:374)o v, so the(cid:396)e is (cid:374)o (cid:449)o(cid:396)k, cv = 3r/2. Polyatomic gases not only have translational motion, but also rotational and vibrational motion. Only translational motion increases temperature, but some of the energy is being used to increase rotational and vibrational motion.

Get access

Grade+
$40 USD/m
Billed monthly
Grade+
Homework Help
Study Guides
Textbook Solutions
Class Notes
Textbook Notes
Booster Class
10 Verified Answers
Class+
$30 USD/m
Billed monthly
Class+
Homework Help
Study Guides
Textbook Solutions
Class Notes
Textbook Notes
Booster Class
7 Verified Answers

Related Documents

Related Questions