We are bounded in a nutshell of Infinite space: Blog Post #7, Worksheet # 3.1, Problem #4: But it
actually turns out to be flat…ish
4.
We actually observe a flat rotation curve in our own Milky Way. (You will show
this with a radio telescope in your second lab!) This means \(v(r)\) is nearly constant
for a large range of distances.
(a)
Lets call this constant rotational velocity \(V_c\)
. If the mass distribution of the Milky
Way is spherically symmetric, what must be the \(M( < r)\) as a
function of \(r\) in this case, in
terms of \(V_c\), \(r\), and \(G\) ?
(b)
How does this compare with the picture of the galaxy you drew last week with
most of the mass appearing to be in bulge?
(c)
If the Milky Way rotation curve is observed to be flat \((V_c \approx 240 km/s ) \) out
to 100 kpc, what is the total mass enclosed within 100 kpc? How does this
compare with the mass in stars? Recall the total mass of stars in the Milky
Way, a number you have been given in your first assignment and should commit to
memory.
(a)
Now that we redefined \(v(r)\) as \(V_c\), and \(M_{enc}\) will now be \(M( < r)\)
, these new description will appear in the formulas used previously. Following
this, we now start to understand the problem, we simply need to re-express the
values set forth by the previous problem with new definitions and understand
the interpretations. These equations now leave us with: \[V_c = \left(\frac{G M( < r)}{r}\right)^\frac{1}{2}
,\] \[\frac{V_c^2 r}{G} = M( < r)\] the form of the equation in its new
iteration with the new definitions for the variables and outputs.
(b)
However, as we start comparing the view of the Milky Way, as we saw in previous
blog posts and readily available as part of your night sky if you have low
light pollution and are in the southern hemisphere, and the mathematical models
we have been using the last couple of problems, there seems to be a problem. We
have been assuming the Milky Way can be considered a spherical galaxy when it
clearly is not, rather it is a Spiral Barred galaxy that has become flat
because of billions of years of rotations and conservation of angular momentum.
This also conflicts with the fact we have been assuming symmetrical mass
distribution when we are also aware of the fact of varying densities of the
galaxies depending on the distance from the center.
(c)
Now, taking into account the distance of 100 kpc where most of the mass of the
galaxy is found, and the apparent speed of the curvature of the galaxy \((V_c
\approx 240 km/s ) \), these values can simply be inserted into the equation to
find the mass of the galaxy. First, a few constants: \[G_{(gravitational
constant)}=6.674\times10^{-8}\frac{cm^3}{g s^2}\] \[2 \times 10^{23} \frac{g}{M_\odot
}\] \[ 1 pc = 3.1 \times 10^{18} \frac{cm}{pc}. \]
Using these values, we may start to plug into the
general equation, adding in some dimensional analysis conversion factors:
\[\frac{V_c^2 r}{G} = M( < r),\]
\[M ( < r)=\frac{(2.4 \times 10^2 \frac{km}{s} \cdot 10^5 \frac{cm}{km})^2 \cdot 10^2 kpc \cdot 3.1 \times 10^{18} \frac{cm}{pc} } {6.674\times10^{-8}\frac{cm^3}{g s^2}} , \]
\[M( < r)= 2.7 \times 10^{45} g , \]
\[M( < r)= \frac { 2.7 \times 10^{45} g } {2 \times 10^{23} \frac{g}{M_\odot} } , \]
\[M( < r)= 1.4 \times 10^{12} M_\odot .\]
Thus we have the calculation for the mass
of the galaxy where its majority accumulates, however, it is a known quantity that
the amount of stars in the galaxy equates to a mass of \( 10^{10} M_\odot \),
so there is a difference of 2 orders of magnitude in this scale. Therefore,
there is an enormous amount of matter in the galaxy that is not stars, it could
be dust, planets, gases and many other forms of matter, but even high estimates
of all the visible matter in the universe does not account for the total mass
of the galaxy. Therefore, there is mass in the galaxy that, so far, cannot be
observed, but its effects are evident and necessary to explain the speed the
galaxy spins at the distances it does. This is dark matter, some unknown
substance* in the universe that acts upon it without our being able to
ascertain what it is, it could be dark, un-ignited stars, it could be huge
amounts of rocks and dust that are in some way invisible, or it could be
accumulations and existence of massive quantic particles that seemingly never
interact with what we perceive as normal matter. And I thought we were just
talking about flat galaxies instead of spherical ones, yet the spherical now
starts to make sense when you think where all the extra matter might be.
So, the discrepancy between the observed distribution of stars in the Milky Way and the assumption of a spherical mass distribution may be a problem, but it’s actually not a terrible approximation even for the stellar population (with a small correction factor). Now, if we could ask you to assume that spherical symmetry is a pretty good approximation for the mass distribution of the Galaxy, is there something else that’s funny about the mass profile you derived? Whereas most of the stars visible in the Galaxy are confined within about 15 kpc, the rotational velocity is constant out to ~100 kpc (sorry if this hasn’t been made clear in the problem). What does this imply about the mass distribution between 15 and 100 kpc?
ReplyDelete(Answer: total enclosed mass keeps on increasing pretty dramatically with radius! M(<r) ~ r out to distances where we can’t see stars anymore!)
But, yes, nice reflection in the end! We do think the dark matter halo is actually pretty much spherical.
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