Caption:
"This log-log plot
shows the rate
of nuclear energy generation (ε i.e., probably
energy
per unit mass
per unit time
Cl-378)
for main-sequence stars as
a function of
temperature (T).
The green
curve is the
proton-proton (pp) chain reaction,
the blue
curve is the
CNO cycle,
and the red
curve
is the triple-alpha process.
The yellow
vertical line
represents the core temperature
of the Sun, and it shows
the pp chain reaction
is the primary source of energy generation
in the Sun.
The dashed line joining the
pp chain reaction
curve
to the CNO cycle is
the net energy generation
rate
of the combined
hydrogen nuclear burning
rates.
The overall slope of the curves
shows the greater temperature
sensitivity of the CNO cycle and
triple-alpha process relative
to the pp chain reaction."
(Somewhat edited.)
Features:
- The lack of numbers
on the axes
suggest the image
author may be being
somewhat qualitative.
- Density
and composition for the
log-log plot?
Probably, just
main-sequence star
central density
and
cosmic composition
for which the
solar composition
is a fiducial composition.
See also file
solar_composition.html
for a plot of the
of the solar composition.
- In the CNO cycle,
carbon (C, Z=6),
nitrogen (N, Z=7),
and
oxygen (O, Z=8)
isotopes
are used as
catalysts
in the nuclear burning process.
These isotopes are consumed
in various nuclear reactions,
but recreated in others.
There is NO net change in their abundances.
The CNO cycle
is believed to be the dominant
hydrogen burning
in main-sequence stars
of ⪆ 1.3 M_☉ for
which the
stellar core
temperature ⪆ 17*10**6 K
which is a bit higher than the
solar core
temperature of the 15.7*10**6 K
(Wikipedia: CNO cycle).
- The rapid increase in
hydrogen burning rate
with stellar core
temperature
for the CNO cycle
is an important factor in the rapid decrease in
stellar lifetime
with stellar mass.
- The CNO cycle actually does
rely on the weak nuclear interaction
via beta decays
(Wikipedia: CNO cycle:
Cold CNO cycles), but
the reliance is evidently much less important than that of the
proton-proton chain
via the
where a weak nuclear interaction
must convert a
proton (p) into a
neutron (n)
to make the deuteron (D,H-2)
which the
rate determining step
of the
proton-proton chain
(Wikipedia:
The proton-proton chain).
- The triple-alpha process
is NOT important for producing
energy
in main-sequence stars.
However, it is in
post-main-sequence stars
and its ash is
carbon (C, Z=6)
and, by a side effect process,
another product is
oxygen (O, Z=8).
Collectively
the triple-alpha process
and the side effect process
can be called
helium burning.
Some of the
cosmic composition
of carbon
and oxygen
is produced in
helium burning
in post-main-sequence stars
and some comes from
supernova explosions.
Credit/Permission: ©
User:RJHall
2008 /
Creative Commons
CC BY-SA 3.0.
Image link: Wikimedia Commons:
File:Nuclear energy generation.svg.
Local file: local link: nuclear_burning_processes.html.
File: Star file:
nuclear_burning_processes.html.