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Analysis of an Eddy Current Brake with FEMM

Analysis of an Eddy Current Brake with FEMM

Analysis of an Eddy Current Brake with FEMM

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2 eddycurrentbrake.nb<br />

In[9]:= BHmax = 40; H∗ Energy product <strong>of</strong> the magnet in MGOe ∗L<br />

pp = 25 ∗mm; H∗ Pole pitch <strong>of</strong> the magnets ∗L<br />

wm = 20 ∗mm; H∗ Magnet width ∗L<br />

tm = 5 ∗mm; H∗ Magnet thickness ∗L<br />

tb = 5 ∗mm; H∗ Back iron thickness ∗L<br />

tp = 2.5 ∗mm; H∗ Conductive plate half−thickness ∗L<br />

g = 1 ∗mm; H∗ Air gap length between magnet <strong>an</strong>d plate ∗L<br />

σ = 30;H∗ Plate conductivity in MSêm ∗L<br />

h = 100 ∗mm; H∗ Depth <strong>of</strong> magnet array ∗L<br />

ε = 20 ∗mm; H∗ Plate overh<strong>an</strong>g on either side <strong>of</strong> the magnets ∗L<br />

ü Derived Qu<strong>an</strong>tities<br />

Mech<strong>an</strong>ical frequency <strong>of</strong> the magnet array<br />

In[19]:= β = π êpp;

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