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;