Your browser does not fully support modern features. Please upgrade for a smoother experience.
Submitted Successfully!
Thank you for your contribution! You can also upload a video entry or images related to this topic. For video creation, please contact our Academic Video Service.
Version Summary Created by Modification Content Size Created at Operation
1 handwiki Camila Xu -- 1702 2022-11-03 01:39:23

Video Upload Options

We provide professional Academic Video Service to translate complex research into visually appealing presentations. Would you like to try it?
Cite
If you have any further questions, please contact Encyclopedia Editorial Office.
HandWiki. CNO Cycle. Encyclopedia. Available online: https://encyclopedia.pub/entry/32656 (accessed on 25 September 2026).
HandWiki. CNO Cycle. Encyclopedia. Available at: https://encyclopedia.pub/entry/32656. Accessed September 25, 2026.
HandWiki. "CNO Cycle" Encyclopedia, https://encyclopedia.pub/entry/32656 (accessed September 25, 2026).
HandWiki. (2022, November 03). CNO Cycle. In Encyclopedia. https://encyclopedia.pub/entry/32656
HandWiki. "CNO Cycle." Encyclopedia. Web. 03 November, 2022.
CNO Cycle
Edit

The CNO cycle (for carbon–nitrogen–oxygen; sometimes called Bethe–Weizsäcker cycle after Hans Albrecht Bethe and Carl Friedrich von Weizsäcker) is one of the two known sets of fusion reactions by which stars convert hydrogen to helium, the other being the proton–proton chain reaction (p-p cycle), which is more efficient at the Sun's core temperature. The CNO cycle is hypothesized to be dominant in stars that are more than 1.3 times as massive as the Sun. Unlike the proton-proton reaction, which consumes all its constituents, the CNO cycle is a catalytic cycle. In the CNO cycle, four protons fuse, using carbon, nitrogen, and oxygen isotopes as catalysts, each of which is consumed at one step of the CNO cycle, but re-generated in a later step. The end product is one alpha particle (a stable helium nucleus), two positrons, and two electron neutrinos. There are various alternative paths and catalysts involved in the CNO cycles, all these cycles have the same net result: The positrons will almost instantly annihilate with electrons, releasing energy in the form of gamma rays. The neutrinos escape from the star carrying away some energy. One nucleus goes on to become carbon, nitrogen, and oxygen isotopes through a number of transformations in an endless loop. The proton–proton chain is more prominent in stars the mass of the Sun or less. This difference stems from temperature dependency differences between the two reactions; pp-chain reaction starts at temperatures around 4×106 K (4 megakelvin), making it the dominant energy source in smaller stars. A self-maintaining CNO chain starts at approximately 15×106 K, but its energy output rises much more rapidly with increasing temperatures so that it becomes the dominant source of energy at approximately 17×106 K. The Sun has a core temperature of around 15.7×106 K, and only 1.7% of 4He nuclei produced in the Sun are born in the CNO cycle. The CNO-I process was independently proposed by Carl von Weizsäcker and Hans Bethe in the late 1930s. The first reports of the experimental detection of the neutrinos produced by the CNO cycle in the Sun were published in 2020. This was also the first experimental confirmation that the Sun had a CNO cycle, that the proposed magnitude of the cycle was accurate, and that von Weizsäcker and Bethe were correct.

bethe–weizsäcker carbon–nitrogen–oxygen self-maintaining

References

  1. "Über Elementumwandlungen in Innern der Sterne I". Physikalische Zeitschrift 38: 176–191. 1937. 
  2. "Über Elementumwandlungen in Innern der Sterne II". Physikalische Zeitschrift 39: 633–646. 1938. 
  3. "Energy Production in Stars". Physical Review 55 (1): 541–7. 1939. doi:10.1103/PhysRev.55.103. PMID 17835673. Bibcode: 1939PhRv...55..103B.  https://dx.doi.org/10.1103%2FPhysRev.55.103
  4. "Energy production in stars". Physical Review 55 (5): 434–456. 1939. doi:10.1103/PhysRev.55.434. PMID 17835673. Bibcode: 1939PhRv...55..434B.  https://dx.doi.org/10.1103%2FPhysRev.55.434
  5. "Nuclear Physics, A: Stationary states of nuclei". Reviews of Modern Physics 8 (2): 82–229. 1936. doi:10.1103/RevModPhys.8.82. Bibcode: 1936RvMP....8...82B. https://authors.library.caltech.edu/51288/1/RevModPhys.8.82.pdf. 
  6. "Nuclear Physics, B: Nuclear dynamics, theoretical". Reviews of Modern Physics 9 (2): 69–244. 1937. doi:10.1103/RevModPhys.9.69. Bibcode: 1937RvMP....9...69B.  https://dx.doi.org/10.1103%2FRevModPhys.9.69
  7. "Nuclear Physics, C: Nuclear Dynamics, Experimental". Reviews of Modern Physics 9 (2): 245–390. 1937. doi:10.1103/RevModPhys.9.245. Bibcode: 1937RvMP....9..245L.  https://dx.doi.org/10.1103%2FRevModPhys.9.245
  8. Bardi, Jason Socrates (January 23, 2008). "Landmarks: What makes the stars shine?". Physical Review Focus 21 (3). doi:10.1103/physrevfocus.21.3. https://physics.aps.org/story/v21/st3. Retrieved November 26, 2018. 
  9. Krane, Kenneth S. (1988). Introductory Nuclear Physics. John Wiley & Sons. p. 537. ISBN 0-471-80553-X. https://archive.org/details/introductorynucl00kran. 
  10. Ray, Alak (2010). "Massive stars as thermonuclear reactors and their explosions following core collapse". in Goswami, Aruna; Reddy, B. Eswar. Principles and Perspectives in Cosmochemistry. Springer Science & Business Media. p. 233. ISBN 9783642103681. https://books.google.com/books?id=gCr9WVH0utwC&pg=PA233. 
  11. Wapstra, Aaldert; Audi, Georges (18 November 2003). "The 2003 Atomic Mass Evaluation". Atomic Mass Data Center. http://amdc.in2p3.fr/web/masseval.html. 
  12. Lemut, A.; Bemmerer, D.; Confortola, F.; Bonetti, R.; Broggini, C.; Corvisiero, P. et al. (2006). "First measurement of the 14N(p,γ)15O cross section down to 70 keV". Physics Letters B 634 (5–6): 483–487. doi:10.1016/j.physletb.2006.02.021. Bibcode: 2006PhLB..634..483L.  https://dx.doi.org/10.1016%2Fj.physletb.2006.02.021
  13. Note: It is not important how invariant masses of e and ν are small, because they are already small enough to become relativistic. What is important is that the daughter nucleus is heavy compared to p/c .
  14. Scheffler, Helmut; Elsässer, Hans (1990). Die Physik der Sterne und der Sonne. Bibliographisches Institut (Mannheim, Wien, Zürich). ISBN 3-411-14172-7. 
  15. https://core.ac.uk/download/pdf/31144835.pdf
More
Upload a video for this entry
Information
Contributor MDPI registered users' name will be linked to their SciProfiles pages. To register with us, please refer to https://encyclopedia.pub/register :
View Times: 3.5K
Entry Collection: HandWiki
Revision: 1 time (View History)
Update Date: 03 Nov 2022
Notice
You are not a member of the advisory board for this topic. If you want to update advisory board member profile, please contact office@encyclopedia.pub.
OK
Confirm
Only members of the Encyclopedia advisory board for this topic are allowed to note entries. Would you like to become an advisory board member of the Encyclopedia?
Yes
No
${ textCharacter }/${ maxCharacter }
Submit
Cancel
There is no comment~
${ textCharacter }/${ maxCharacter }
Submit
Cancel
${ selectedItem.replyTextCharacter }/${ selectedItem.replyMaxCharacter }
Submit
Cancel
Confirm
Are you sure to Delete?
Yes No
Academic Video Service