Hyperloop Cfd Analysis

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    HYPERLOOP CFD Analysis

    Objective

    To calculate aerodynamic load on the pods at its top speed, fnd out where ow

    separation occurs, observe the shocks ormed and to optimize the exterior shape o

    the pod.

    Problem physics

    Since pure vacuum is not easible to produce the tubes are maintained at 1 !a

    pressure and a temperature o "# by usin$ pumps.

    %n reality the pod accelerates to its top speed o &' mph in one minute. (owever

    or the simulation % have assumed the pod accelerates to its top speed o &'mph

    instantaneously at start time o analysis. The pod aerodynamics is studied without

    considerin$ the e)ect o compressor intake or now. The air in ront o the pod which

    tries to ow throu$h the bypass area * between pod and tube + $ets choked. This airis accumulated in ront o the pod thereby increasin$ pressure in the ront o the

    pod*the pod acts like a piston compressin$ the air in ront o it+.The air which

    mana$es to pass throu$h the bypass expands when it reaches the back o the pod

    reachin$ supersonic speeds. ddin$ a compressor intake at the ront can reduce the

    e)ect but cannot eliminate the problem o air accumulation at the ront due to the

    desi$n constraints o an intake system.

    Tube dimensions *in inches+ are as $iven below

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    Computational domain

    -omputational domain as modeled in -T%. This is a case o pod without an intake.

    nly hal o the tube and pod is modeled by takin$ symmetry into account.

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    eshin!

    /nstructured tetra0prism mesh usin$ elauney method. 2efnements are made only

    in the boundary layers and in the wake re$ion. !rism layers are used at the

    boundaries.

    3irst the mesh was $enerated usin$ ctree method and then elauney method wasused later $enerate the fnal mesh usin$ the ormer mesh.

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    "O#$DARY CO$D%&%O$'The wall boundaries apart rom the pod itsel are movin$ with the velocity o the

    pod in a rame o reerence attached to the pod. The pod is ali$ned alon$ the 45axis

    lon$itudinally and velocity o pod is in the positive 45direction.

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    Dynamic (radient Adaptive esh

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    CO$CL#'%O$

    ll the iterations in each time step was conver$ed.

    nly 1.e5" seconds o ow was simulated.