This homework must be submitted on paper;
you may write out your work on paper,
or type it into some word processor and then print it.
Either way, staple together all pages and write your name
legibly at the top of each page.
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The star Sirius, in the constellation Canis Major, is the brightest
star in the sky (apart from the Sun). It is actually a
binary star system, in which an ordinary main sequence star,
Sirius A, orbits a white dwarf, Sirius B.
Some of their properties are listed below:
star temperature(K) radius(m)
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Sirius A 9,900 1.19 x 109
Sirius B 25,000 5.71 x 106
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- Suppose that we compared one square meter of each star,
side-by-side. The section of Sirius B would appear brighter,
because it is hotter. Assuming both stars radiate like
blackbodies, how many times brighter would the section of Sirius B
appear, compared to the section of Sirius A?
- However, the two stars have very different sizes.
What is the ratio of the surface areas?
- Putting together these two factors, estimate the ratio of
luminosity of Sirius B to that of Sirius A.
- Convert the ratio of luminosities to a difference in magnitudes.
How many magnitudes fainter should Sirius B appear?
- Look up the apparent V-band magnitude of Sirius A.
What is it? Using this value, the result of the previous
question, predict the apparent V-band magnitude of Sirius B.
- Bonus!
What is the actual apparent V-band magnitude of Sirius B?
- One way to describe the density of a crowd of people is to
measure the distance between people, not in feet or meters,
but in terms of the size of a person. If the typical distance
between people is 5 body-widths, each person can move freely.
If the typical distance is 1.2 body-widths, then everyone
is jammed pretty close together.
Let's try the same analysis to describe the density of matters
at the centers of star. Use the following very approximate
values as the sizes of an ordinary atom, and of an atomic nucleus.
radius of ordinary atom: 10-10 meters
radius of atomic nucleus: 10-15 meters
- Consider the center of the current Sun, where the density
is 77 x 103 kg/m3.
Assume that the material is pure hydrogen.
- How many H atoms in one cubic meter?
- What is the typical spacing between atoms,
expressed in units of atomic radii, and nuclear radii?
- Consider the center of a white dwarf, in which the density
is 2.3 x 109 kg/m3.
Assume that the material is pure helium.
- How many He atoms in one cubic meter?
- What is the typical spacing between atoms,
expressed in units of nuclear radii?
- Consider the center of a neutron stars, in which the density
is 4.12 x 1017 kg/m3.
Assume that the material is pure neutrons.
- How many neutrons in one cubic meter?
- What is the typical spacing between neutrons,
expressed in units of nuclear radii?
- In a type Ia supernova explosion, it is said that the runaway
thermonuclear reactions, which ultimately convert the carbon atoms
of a white dwarf into iron atoms, release so much energy
that the star breaks apart, explodes, and flies off into space.
Let's check to see if the physics supports this claim.
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Using the figure above, which shows the curve of binding
energy, to estimate the total energy released per nucleon
when fusion turns 12-Carbon into 56-Iron.
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Next, compute the total number of nucleons in a white dwarf
star by dividing the mass of dwarf at the Chandrasekhar limit
by the mass of one proton (protons and neutrons are the main
members of the nucleon family, and their masses are the same
as far as this problem is concerned).
- Multiply those numbers to compute the total energy released
due to the fusion of an entire white dwarf from carbon
to iron. Express that total energy in Joules.
- The energy required to move all parts of a spherical body
away from each other to infinity is given by the
absolute value of the gravitational
potential energy (GPE) of the body. Compute the GPE for a white
dwarf of mass M = 1.44 solar masses (convert to kg)
and R = 0.06 solar radii (convert to meters).
Express this GPE in Joules.
- Does the runaway fusion reaction produce enough energy
to blow the star apart?
- James Jeans figured out a way to determine if a cloud of gas
was gravitationally stable, or if it might collapse
under its own self-gravity. The Jeans' length
is the maximum size that a cloud with some given properties
may have and remain stable; if a cloud exceeds the Jeans length,
then it will likely collapse.
Anxious Fred listened to his astronomy professor describe this
analysis, and immediately worried that the atmosphere of
the Earth might someday collapse and leave people gasping for
breath. "It would be terrible if all the oxygen and nitrogen
gathered into a little ball in Saskatchewan," Fred thinks
to himself. "What would happen to us in Rochester?"
Can you show Fred that there is no need to worry?
Make the following assumptions about the Earth's atmosphere:
temperature T = 20 C = 293 K
density ρ = 1 kg/m^3
composition = pure nitrogen
- With these assumptions, what would be the mean molecular weight
μ of the atmosphere?
- With these assumptions, what is the Jeans' length
for the atmosphere?
- Based on this Jeans' length, should Fred worry
that our atmosphere might collapse?
- We have derived a formula which yields the equilibrium temperature
for an object, which emits and absorbs like a blackbody,
orbiting its host star at some particular distance.
Let's try applying this formula to the Earth.
- First, consider a perfect blackbody which orbits our Sun
at the same distance as the Earth: at 1 AU.
What would the equilibrium temperature of this
object be? Express the answer in Kelvin.
- What is the actual average surface temperature of the Earth,
expressed in Kelvin?
Please use a NASA source to look up this value;
provide a link to the source along with your value.
- How big is the difference? Can you explain it?