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Monday, 07/24: Writing a pm-code - AIP

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dissipationless simulations 11<br />

Cosmological simulations: dissipationless case<br />

• For many problems it is warranted to ignore the baryonic effects and solve<br />

only evolution of dissipationless component (dark matter, stars).<br />

• In this case, only equations of particle motion and the Poisson equation are<br />

solved.<br />

• Very generally, each evolution time step of a dissipationless simulation<br />

consists of the following two main parts:<br />

— gravity solver: solve the Poisson equation and calculate particle<br />

accelerations.<br />

— time integrator: update particle positions and velocities.<br />

• different <strong>code</strong>s differ in how these two parts are implemented.<br />

• Today we will consider the Particle-Mesh (PM) technique for solving the<br />

Poisson equation and integrating particle trajectories.

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