BYU Astronomy Research Group Joins the Astrophysical Research Consortium (ARC)

As of January 2021 BYU will be a member of the ARC Consortium (Link to Consortium) with access to the ARC 3.5-m telescope and the 0.5-m ARCSAT telescope.  The primary use of the ARC 3.5-m telescope time is for graduate student projects.  This provides a wide array of instrumentation that is currently being used to study objects in the solar system all the way to studies of the large scale structure of the Universe.

Other BYU Astronomy Facilities

In addition to our telescope time from the ARC consortium, we operate a number of our own astronomical facilities

West Mountain Observatory (West Mountain)

This is our mountain observatory at about 6600 ft above sea level.  This consists of three telescopes: 0.9-m, 0.5-m, and a 0.32-m. It is a 40 minute drive that ends in a 5 miles drive up a dirt road. The mountain itself can be seen from campus. We don't provide any tours of this facility.

Orson Pratt Observatory

The Orson Pratt Observatory is named for an early apostle of the Church of Jesus Christ of Latter-Day Saints.  It is our campus telescope facility and contains a wide variety of telescopes for student research and public outreach. We operate a 24" PlaneWave telescope in the main campus dome, plus a 16", two 12", one 8", and a 6" telescope on our observation deck.  The telescopes are all fully robotic. Beyond this we have a large sections of telescopes used on public nights.

Royden G. Derrick Planetarium (Planetarium)

This is a 119 seat, 39" dome planetarium with acoustically treated walls to allow it's use as a lecture room. Recently we upgraded to an E&S Digistar7 operating system with 4K projectors.  The planetarium is used for teaching classes, public outreach, and astronomy education research projects.





Selected Publications

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Single-trail spectra of SX Phe have been obtained covering many cycles of this short-period dwarfcepheid variable at a dispersion of 18 Å mm⁻¹. The rapid changes in line intensities and the line doubling reported by Stock and Tapia (1971a) from 40 Å mm⁻¹ plates are not evident in our spectra.

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D. H. McNamara and R. Chapman
New radial-velocity measurements of the classical cepheid AW Per indicate the center-of-mass velocity of the star has increased by ~ 21 km sec⁻¹ since the radial-velocity measurements secured by Miller and Preston in 1960-63. The orbital period of the binary motion must exceed 20 years.
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Photometric (uvbyfi) observations of the RRc variable SS Psc suggest that it is more closely related to dwarf cepheids (RRs stars) than to the RRc variables. Intrinsic (b — y) and c₁ values are employed to derive the variations in surface gravity and temperature. The mean values are (log g eff) = 3.29 and (T eff ) = 7300° K. The mi index, ((mi) 0 ) = 0.178, and spectrum indicate it is a metal-strong star.

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D. H. McNamara and Kent. A. Feltz, Jr.

The geometric and photometric elements of the eclipsing star U Sge have been derived from uvby observations secured in 1973-74. The "best" elements are r₁ = 0.296, r₂ = 0.225, i = 90°; and L₁ = 0.130, L₂ = 0.870 in yellow light where the subscript 1 refers to the G2 IV-III component and the subscript 2 refers to the B8 V component. Radii and masses of the two stars can be derived by assuming that the larger star fills its Roche lobe. This assumption yields r₁ = 3.32 R⊙, r₂ = 2.52 ⊙, 𝕸₁ = 1.4⊙, and 𝕸₁ = 3.5⊙. The absolute magnitudes are found by two different methods and yield Mv = —0ṃ4 for the B star and Mv = +1ṃ8 for the G star. If corrections for radiative interactions are made, the absolute magnitude of the G star is Mv ≃+2ṃ2. Observational data secured in the u filter suggest that Balmer continuum emission can be detected from an emitting gas stream or disk. The gas must be concentrated near the following hemisphere of the B Star. The mi measurements of the secondary component suggest a metal deficiency of [Fe/H] = —0.6.

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D. H. McNamara and Kent. A. Feltz, Jr.

Photometric (uvbyβ) and spectrographic observations of the dwarf cepheid RS Gru are described. The photometry suggests that the star is slightly reddened, E(b-y)=+ 0ṃ026. Intrinsic (b-y) and c values are used to derive the variations in temperature and surface gravity. The mean values are >Teff< = 7620° and (log geff) = 3.83. With the aid of Wesselink's method, a radius of 3.1 Rṃ is found. The radius and effective temperature indicate Mv = + 1.2 which agrees well with the value Mv = + 1.3 derived directly from the photometry. A mass of 2.4 � � is found from the radius and effective gravity. The radial-velocity data indicate that γ = 82 km sec¹ and 2K = 49 km sec¹.

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S. K. Wilcken, D. H. McNamara, and H. K. Hansen

Photometric observations of RZ Set in the (U, B, and V passbands are described. Because of distortions in the light curves it is difficult to derive accurate light elements. The "best" light elements are r₁ = 0.26, r₂ = 0.26, k = 1, i = 84°, and L = 0.89, L₂ = 0.11 in yellow light. At fourth contact the system is approximately 0ṃ1 brighter than at first contact. The decrease in light near first contact is attributed to Thompson scattering by free electrons in circumstellar material. Estimates of the spectral types and absolute magnitudes of the two stars yield B2 (-4ṃ6) and A0(-2ṃ3). Both stars have radii ~ 14 R⨀ and are = 2ṃ5 brighter than main-sequence stars of similar spectral types. It appears that the secondary star fills its Roche limit. The color excess of the system is E(B–V) $ \simeq $ 0ṃ86.