Consider a pure hydrogen cloud with unform density surrounding a hot star. This star emits Q ultraviolet photons per second beyond the Lyman limit, i.e., photons capable of ionizing hydrogen from the ground state. Assume that each photon ionizes one and only one hydrogen atom.
Let R be the number of recombinations per cm3 per second. In a steady state, the number of recombinations will equal the number of ionizations inside the resulting spherical ionized region, called a Strömgren sphere, whose Strömgren radius, r is given by:
The recombination rate R involves a two-body process: the
two
bodies are the electron and the proton. The rate must be proportional
to
the product of their number densities (in cm-3), ne and np. Overall charge neutrality requires
that ne = np. So we have the total recombination
rate per cm3 per second:
a. Write down an expressions for the Strömgren radius in cm.
For temperatures characteristic of H II regions,
α is approximately
3 x 10-13 cm3sec-1. Assume ne = 10 cm-3.
b. Compute r in cm and in parsecs when Q = 3 x
1049 sec-1 (an O5 V star with T~40,000K and R~20
R☉).
e. What kinds of main-sequence stars create significant H II
regions around them?
f. O stars are often born in
clusters like the Trapezium in Orion. The Orion Nebula is 450 pc away,
and the portion known as M42 has an angular diameter of about 1
degree. Assume that M42 is a spherical pure hydrogen nebula with an
average density of 200
cm-3. How many equivalent 05 stars are
required to ionize M42? Compare this with the number of the brightest
Trapezium stars.
g. Now consider a planetary nebula central
star with a temperature of 150,000K and R~0.1 R☉.
h. Calculate the mass, in solar masses, contained in the
Strömgren sphere of the planetary nebulae above. How does this compare
this with the typical mass of a planetary nebula you learned about in
Astronomy 111, or in your studying?
i. Calculate the mass, in solar masses, contained in the
Strömgren sphere produced by the O5 star in part b. Compare this value with
the mass of the planetary nebula, and comment
c. Compute r in cm and in parsecs when Q = 4 x
1046 sec-1 (a BO V star with T~30,000K and R~5
R☉).
d. Compute r in cm and in parsecs when Q = 1 x
1039 sec-1 (a G2 V star with T~6000K and R~R☉).
It has Q = 1 x
1047 sec-1. Compute r in meters and in parsecs for this case, using
the same value for α, but with a
density characteristic of planetary nebulae, about 103 cm-3. Compare with the
O star above. Also comment on the ionization level in the
Strömgren sphere compared with that in the H II region for the O star above.
Back to Astronomy 402 syllabus.