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Reflected Light From Extra Solar Planets Modeling light curves of planets with highly elliptical orbits Daniel Bayliss, Summer Student, RSAA, ANU Ulyana.

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Presentation on theme: "Reflected Light From Extra Solar Planets Modeling light curves of planets with highly elliptical orbits Daniel Bayliss, Summer Student, RSAA, ANU Ulyana."— Presentation transcript:

1 Reflected Light From Extra Solar Planets Modeling light curves of planets with highly elliptical orbits Daniel Bayliss, Summer Student, RSAA, ANU Ulyana Dyudina, RSAA, ANU Penny Sackett, RSAA, ANU

2 Introduction 119 extra solar planets detected. – 118 found by precise radial velocity measurements. – 1 by found by transit photometry. No reflected light from extra solar planets detected to date, however the albedo of τ Boo constrained by lack of signal (Charbonneau et al.,1999, ApJ, 522, L145).

3 Reflected light Amount of reflected light given by: p=albedod=planet-star separation  =phase function R p =planet radius

4 Space Photometry Current photometric precision limited by atmosphere to around L P /L * ~50 x 10 -6. Canadian micro satellite MOST target list includes 3 stars with planets (close-in, circular). NASA’s Kepler satellite (2007) with 100,000+ target stars. Predicted to achieve precision of L P /L * < 10 x 10 -6. MOST Kepler

5 Elliptical Orbits Semi-major axis ApocentrePericentre

6 Eccentricities of Extra Solar Planets Eccentricity Semi-major axis (AU)

7 Inclination: i=0° (face on) Orientation of the orbital plane - Inclination

8 Inclination: i=10°

9 Inclination: i=45°

10 Inclination: i~90° (edge on)

11 Argument of pericentre: ω=0° To observer Orientation of the orbital plane - Argument of Pericentre

12 To observer Argument of pericentre: ω=90°

13 To observer Argument of pericentre: ω=-90°

14 Model Reflective properties of planets based on Pioneer data of Jupiter. Planetary radius assumed to be 1 Jupiter radius. Example light curve properties: –Semi-major axis = 0.1 AU –Argument of pericentre = 60° –Eccentricity = 0.5

15 Time P days 8 x 10 -6 0 Example Light Curve i=90 o (Edge on) L P / L * PericentreApocentre

16 Time 8 x 10 -6 i=75 o 0 L P / L * P days

17 Time 8 x 10 -6 i=60 o 0 L P / L * P days

18 Time 8 x 10 -6 i=45 o 0 L P / L * P days

19 Time 8 x 10 -6 i=30 o 0 L P / L * P days

20 Time 8 x 10 -6 i=15 o 0 L P / L * P days

21 Time 8 x 10 -6 i=0 o (Face on) 0 L P / L * P days

22 Example - HD 108147b Extra solar planet discovered by Pepe, Mayor, et al (2002, A&A, 388, 632). Properties: –Semi-major axis = 0.104 AU –Period = 10.9 days –Eccentricity = 0.498 –Argument of pericentre = -41° –Inclination = ?

23 Time 10.9 days 40 x 10 -6 HD 108147b 0 L P / L *

24 Time 10.9 days 10 x 10 -6 Contrast contrast 0 L P / L *

25 Contrast for e=0 Inclination (i) 90 0 -90 Scale at 0.1 AU (x10 -6 ) 100 10 1 0.1 Argument of pericentre (ω) 090 Kepler

26 Contrast for e=0.6 Inclination (i) 90 0 -90 Scale at 0.1 AU (x10 -6 ) Argument of pericentre (ω) 090 100 10 1 0.1

27 Contrast for various e Argument of pericentre (ω) Scale at 0.1 AU (x10 -6 ) Inclination (i) e=0.6 e=0.7 e=0.8 e=0 e=0.1 e=0.2 e=0.3 e=0.4 e=0.5 100 10 1 0.1

28 Conclusions 1.A low inclination (face on) orientation can show strong contrast if it has a high eccentricity orbit. 2.Light curves from elliptical orbits may help constrain a systems inclination. 3.Favourable pericentric orientation can dramatically increase the contrast.


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