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@ -64,10 +64,12 @@ are considered. The hottest Nswap atoms in layer 1 are selected.
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Similarly, the coldest Nswap atoms in the "middle" layer (see below)
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are selected. The two sets of Nswap atoms are paired up and their
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velocities are exchanged. This effectively swaps their kinetic
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energies, assuming their masses are the same. Over time, this induces
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a temperature gradient in the system which can be measured using
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commands such as the following, which writes the temperature profile
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(assuming z = edim) to the file tmp.profile:
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energies, assuming their masses are the same. If the masses are
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different, an exchange of velocities relative to center of mass motion
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of the 2 atoms is performed, to conserve kinetic energy. Over time,
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this induces a temperature gradient in the system which can be
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measured using commands such as the following, which writes the
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temperature profile (assuming z = edim) to the file tmp.profile:
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</P>
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<PRE>compute ke all ke/atom
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variable temp atom c_ke/1.5
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@ -54,10 +54,12 @@ are considered. The hottest Nswap atoms in layer 1 are selected.
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Similarly, the coldest Nswap atoms in the "middle" layer (see below)
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are selected. The two sets of Nswap atoms are paired up and their
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velocities are exchanged. This effectively swaps their kinetic
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energies, assuming their masses are the same. Over time, this induces
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a temperature gradient in the system which can be measured using
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commands such as the following, which writes the temperature profile
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(assuming z = edim) to the file tmp.profile:
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energies, assuming their masses are the same. If the masses are
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different, an exchange of velocities relative to center of mass motion
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of the 2 atoms is performed, to conserve kinetic energy. Over time,
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this induces a temperature gradient in the system which can be
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measured using commands such as the following, which writes the
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temperature profile (assuming z = edim) to the file tmp.profile:
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compute ke all ke/atom
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variable temp atom c_ke/1.5
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