1 / 17

The Properties of Gases

The Properties of Gases. 박영동 교수 자연과학대학 화학과. 기체는 왜 다루는가 ?. 역사적인 배경과 의미 Boyle’s Law – First Scientific Experiment, 1661 Charles’s Law – Definition of Temperature, 1780s Avogadro’s Hypothesis –

italia
Download Presentation

The Properties of Gases

An Image/Link below is provided (as is) to download presentation Download Policy: Content on the Website is provided to you AS IS for your information and personal use and may not be sold / licensed / shared on other websites without getting consent from its author. Content is provided to you AS IS for your information and personal use only. Download presentation by click this link. While downloading, if for some reason you are not able to download a presentation, the publisher may have deleted the file from their server. During download, if you can't get a presentation, the file might be deleted by the publisher.

E N D

Presentation Transcript

  1. The Properties of Gases 박영동교수 자연과학대학 화학과

  2. 기체는 왜 다루는가? 역사적인 배경과 의미 Boyle’s Law – First Scientific Experiment, 1661 Charles’s Law – Definition of Temperature, 1780s Avogadro’s Hypothesis – Combined Ideal Gas Law and Kinetic Theories– First Successful Scientific Law derived from purely mathematical approach. 실용적인 배경과 의미 기체는 열역학의 기초, 열역학 제1, 2 법칙을 설명 화학 평형, 화학적 퍼텐셜의 기초 화학반응의 근본적 이해를 도움- 반응동력학 기체를 다루는 공정 이해에 중요한 기초를 줌

  3. The perfect gas equation of state pressure is the force F acting on an area A N/m2 = Pa(pascal) 1 atm = 1.013×105 Pa = 760 torr 1 bar = 1×105 Pa Boyle’s law in 1660. Isotherms of an ideal gas and a real gas. an ideal gas and a real gas

  4. The perfect gas equation of state Charles’s law in 1780s. Avogadro’s principle in 1811. Charles’s law and a perfect gas

  5. Pressure and partial pressure Dalton’s concept of partial pressure in 1801. Partial pressure of idea gases

  6. Kinetic model of an ideal gasMaxwell distribution of speeds Basic assumptions: very small particles, all with non-zero mass. in constant, random motion. perfectly elastic collisions with the walls. negligible interactions among molecules except collisions. The total volume of the gas molecules is negligible. The molecules are perfectly spherical in shape, and elastic. no relativistic effects. no quantum-mechanical effects. instant collision with the wall. The equations of motion of the molecules are time-reversible. an ideal gas in a container of side l Kinetic model of an ideal gas for basics Click here to see KineticTheory_of_Gas.pdf

  7. Maxwell distribution of speeds

  8. Maxwell distribution of speeds

  9. Diffusion, Effusion • Effusion when diameter is smaller than the mean free path λ. • Effusion rate is proportional to speed of molecules, and area of a small hole. Effusion rate ∝c∝(T/M)1/2 (a) Diffusion, (b) Effusion

  10. Molecular Collisions number density of molecules = N/V = nNA/V = pNA/RT ‘c’ sweep volume= ‘c’ σ collision rate z =‘c’ σ × number density of molecule =21/2NAσcp/RT mean free path λ= RT/(21/2NAσp) cross sectional area σ= πd2

  11. Real Gases Interactions phase transition finite sizes of molecules Phase transition and the critical temperature Interaction between molecules potential energy variation Isotherms of CO2

  12. Critical Temperature 31 ℃ http://www.youtube.com/watch?v=8ZbZVikZP9w&feature=related CO2 at the pressure of 75 atm

  13. Compression Factor, Z Compression factor at 0 ℃

  14. The van der Waals equation of state • van der Waals correction to size effect accessible volume is smaller than the physical volume due to the molecular volume. interaction effect pressure measured is smaller than the ‘ideal’ pressure due to the attractions between molecules. volume effect

  15. The van der Waals equation • at critical point, van der Waals isotherms interpretation of the van der Waals equation

  16. The liquefaction of gases The principle of the Linde refrigerator.

  17. The van der Waals gas and Boyle Temperature • Z=0 at Boyletemperature TB, • B = b - a/RT = 0

More Related