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Aurora Kesseli Colby College
REU program-Summer 2011 |
Research projects of other REU students Useful links My conclusions |
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Out of all of the YSOs that were surveyed over half of them showed some form of vairability. Variability comes in a few different forms as observed by M.Morales-Calderon et al.:
I will not discuss the polarization plots or Spectral Energy Distributions but you can see the images of all of the polarization plots and SEDs here: Polarization plots and SEDs
From the light curve we can see that it exhibits a periodic variability.
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Plus Signs: I Band (0.8 microns) Asterix: J Band (1.23 microns) Filled Circle: IRAC band 1 (3.6 microns) Circle: IRAC band 2 (4.5 microns) |
In order to explain this light curve we can use what is known about the
effects of hotspots and warps and apply it to what can be seen in the movie
(fig.1). The difference between the hotspot and the rest of the star is
greatest in the V-Band since it has the shortest wavelength, therefore the V
band is affected mostly by the hotspot. As the wavelength increases the
influence of the hotspot becomes less prominent and the light is more stongly
affected by the disk. This is because the dust in the disk absorbs optical radiation and in
turn emits infrared radiation, and the temperature of the inner
wall of the disk emits most of its radiation in IRAC wavelengths. A blackbody
radiation curve can demonstrate this easily.

Looking at the radiation curves, we can see that the higher the temperature
the shorter the peak wavelength. Therefore as the temperature decreases as
we move further from the star the peak wavelength increases. At the disk
radius the peak wavelength is in the IRAC wavelength.The video below shows the
progression of wavelength from shortest to longest using the fiducial model.

As we cycle through the wavelengths the spot becomes less prominent and
the disk becomes more prominent. Using this we can explain the behavior of the
light curve nicely. When the spot is in view at 0 degrees and 360 degrees the
V band is at its highest point, and as the spot moves around the star the
V-Band magnitude decreases. There is a second small peak at 180 degrees
because the second hotspot briefly comes into view. This is only the case at a
large viewing angle, because at a viewing angle of less than around 50 degrees
the second spot does not come into view and we can see a more normal periodic
pattern.
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At 80 degrees when we are looking at the star we are looking almost directly through the disk which creates the chaotic pattern that is seen. There is not that much variation because not as much light is making it through the disk.
. We also increased the
accretion rate to increase the magnitude of the star. The more infalling material
onto the star the brighter it will be.

In the movie we see that the radius of the disk increases as the accretion rate increases also. This is because the infalling material is heating up the star. The dust gets destroyed around 1600 degrees and as the star heats up the radius where the temperature is 1600 degrees increases and moves further away from the star. Therefore, the disk radius increases as the dust destruction radius also increases.
Fig. 7. Variable accretion model where the amount of infalling material was increased slightly every 20 degrees. The model has a viewing angle of 60 degrees. |
Fig. 8. Light curve where the radius of the star was increased at every 20 degrees. This model was also seen at a viewing angle of 60 degrees. |
Fig. 9. Light curve where the temperature of the star was increased at every 20 degrees (60 degree viewing angle). |

A dip can be explained by the warp obsuring part of the star at that viewing angle.This dip occurs at 0 degrees, and from the movie we can see that the image at 0 degrees has the bottom and top of the star being covered by the warp in the disk. The V-Band, I-Band, and J-band exhibit very little variability besides the dip because there is no hotspot to cause the periodic variations. Also it is only the V, I, and J bands that experience the large dip because that is the light that is coming from the star and the IRAC is coming from the disk and just exhibits a normal periodic curve because of the warp like we saw in all of the other models.
In the fiducial model, seen at a viewing angle of 75 degrees we see a dip
in the IRAC bands this time instead of the optical bands.


This can be explained as the same phenomenon as the previous model except here since we are at such a high angle of inclination the hotspots are probably completely obscured by the disk so the optical light is pretty much constant. The IRAC bands now show the dip because of the warp also. We believe this is because the IRAC radiation is mostly coming from the disk and at 0 degrees the warp in the front of the disk obscures the back of the disk blocking the radiation from being seen and thus creating a dip in the light curve.
An image of the light curves of all of our different models can be found here.
SIMBAD (Stellar/Galactic database)
NASA Astrophysics Data Service