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Biodiversity: A Conversation with Sir Partha Dasgupta
This conversation with Sir Partha Dasgupta moderated by Annual Review of Economics Editorial Commitee Member Tim Besley focuses on biodiversity and its implications for economic thought and policy.
Aerobreakup of Newtonian and Viscoelastic Liquids: Figure 19c
A video from the 2011 review by T.G. Theofanous "Aerobreakup of Newtonian and Viscoelastic Liquids."
Aerobreakup of Newtonian and Viscoelastic Liquids: Figure 9b
A video from the 2011 review by T.G. Theofanous "Aerobreakup of Newtonian and Viscoelastic Liquids."
Aerobreakup of Newtonian and Viscoelastic Liquids: Figure 15
A video from the 2011 review by T.G. Theofanous "Aerobreakup of Newtonian and Viscoelastic Liquids."
Aerobreakup of Newtonian and Viscoelastic Liquids: Figure 17a
A video from the 2011 review by T.G. Theofanous "Aerobreakup of Newtonian and Viscoelastic Liquids."
Aerobreakup of Newtonian and Viscoelastic Liquids: Figure 25
A video from the 2011 review by T.G. Theofanous "Aerobreakup of Newtonian and Viscoelastic Liquids."
Aerobreakup of Newtonian and Viscoelastic Liquids: Figure 9a
A video from the 2011 review by T.G. Theofanous "Aerobreakup of Newtonian and Viscoelastic Liquids."
Aerobreakup of Newtonian and Viscoelastic Liquids: Figure 14
A video from the 2011 review by T.G. Theofanous "Aerobreakup of Newtonian and Viscoelastic Liquids."
Aerobreakup of Newtonian and Viscoelastic Liquids: Figure 2
A video from the 2011 review by T.G. Theofanous "Aerobreakup of Newtonian and Viscoelastic Liquids."
Aerobreakup of Newtonian and Viscoelastic Liquids: Figure 1b
A video from the 2011 review by T.G. Theofanous "Aerobreakup of Newtonian and Viscoelastic Liquids."
Aerobreakup of Newtonian and Viscoelastic Liquids: Figure 19b
A video from the 2011 review by T.G. Theofanous "Aerobreakup of Newtonian and Viscoelastic Liquids."
Aerobreakup of Newtonian and Viscoelastic Liquids: Figure 3b
A video from the 2011 review by T.G. Theofanous "Aerobreakup of Newtonian and Viscoelastic Liquids."
Aerobreakup of Newtonian and Viscoelastic Liquids: Figure 19a
A video from the 2011 review by T.G. Theofanous "Aerobreakup of Newtonian and Viscoelastic Liquids."
Aerobreakup of Newtonian and Viscoelastic Liquids: Figure 3a
A video from the 2011 review by T.G. Theofanous "Aerobreakup of Newtonian and Viscoelastic Liquids."
Aerobreakup of Newtonian and Viscoelastic Liquids: Figure 11
A video from the 2011 review by T.G. Theofanous "Aerobreakup of Newtonian and Viscoelastic Liquids."
Aerobreakup of Newtonian and Viscoelastic Liquids: Figure 10
A video from the 2011 review by T.G. Theofanous "Aerobreakup of Newtonian and Viscoelastic Liquids."
Aerobreakup of Newtonian and Viscoelastic Liquids: Figure 1a
A video from the 2011 review by T.G. Theofanous "Aerobreakup of Newtonian and Viscoelastic Liquids."
Aerobreakup of Newtonian and Viscoelastic Liquids: Figure 20
A video from the 2011 review by T.G. Theofanous "Aerobreakup of Newtonian and Viscoelastic Liquids."
Aerobreakup of Newtonian and Viscoelastic Liquids: Figure 8
A video from the 2011 review by T.G. Theofanous "Aerobreakup of Newtonian and Viscoelastic Liquids."
The Role of Giant Impacts in Planet Formation, Supplemental Video 4: The disruption of two planets in a giant impact
Visualization of two planets undergoing a disruptive giant impact based on computer simulation output. Disruptive collisions are not expected to be common in Solar System formation and due to numerical effects the amount of disruption shown here is likely overestimated. The larger (target) body is one tenth the mass of the Earth and the smaller (impactor) body is 70% the mass of the target. The planets are colliding at 3.75 times their mutual escape velocity which equates to 12.60 km/s. The collision angle defined by the angle between the velocity vector at impact and the line of their centers of mass is 5°.
Variables: The top-left panel shows mantle and core materials as unique colors for the target and impactor. The top-right panel shows the density of material in kilograms per cubic meter. The bottom-left panel shows temperature in thousands of Kelvins. The bottom right panel shows pressure in Pascals.
Software: Simulation run by T.S.J. Gabriel ([email protected]) using SPLATCH a planetary Smooth Particle Hydrodynamics code developed at the University of Bern (Reufer 2011) maintained by A. Emsenhuber (Ludwig Maximillian University of Munich; [email protected]) and H. Ballantyne (University of Bern; [email protected]).
Citation: Gabriel & Cambioni (2023). The Role of Giant Impacts in Planet Formation Annual Reviews.