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ARUP; ISBN: 978-0-9562121-5-3 - CMBBE 2012 - Cardiff University

ARUP; ISBN: 978-0-9562121-5-3 - CMBBE 2012 - Cardiff University

ARUP; ISBN: 978-0-9562121-5-3 - CMBBE 2012 - Cardiff University

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Impact duration (Tp) can be obtained by numeric Integration from the forcedisplacement<br />

curve. The motion could be considered as a simple harmonic motion<br />

with an effective linear stiffness:<br />

(12)<br />

Fmax<br />

1<br />

K effec = =<br />

∆x ⎛ ⎞<br />

⎜ 1 1<br />

+<br />

⎟<br />

⎜ 2 1<br />

K<br />

⎟<br />

⎜ sh 3 3 K H . F ⎟<br />

⎝ max ⎠<br />

Now considering the related equations, the value of Tp could be obtained as:<br />

T<br />

P<br />

= π<br />

m<br />

K<br />

Where<br />

sh e m m m<br />

1 1 1<br />

= +<br />

*<br />

Head Injury Criteria (HIC) which is as explanation of impact severity can be obtained<br />

from the following equation:<br />

2.<br />

5<br />

⎡ ⎡ 1 t ⎤<br />

2 ⎤<br />

HIC = max(<br />

t1,<br />

t2<br />

) ⎢(<br />

t2<br />

− t1<br />

) ⎢ ( ) ⎥ ⎥ (14)<br />

⎢ ( )<br />

⎣ ⎣ − ∫ a t dt<br />

t t1<br />

2 t1<br />

⎦ ⎥⎦<br />

The term max(t1, t2) explains that the time distance between t1 and t2 must be so that<br />

the next term in brackets gains its maximum value. With the following assumption for<br />

the head acceleration<br />

(15)<br />

F ⎛ max t ⎞<br />

a( t) = Sin⎜π<br />

⎟<br />

msh ⎝ TP<br />

⎠<br />

and by replacing equation 15 in 14 and for 0 < t < TP<br />

, by simultaneous solution of<br />

the following equations, the time distance which maximize equations 14 would be:<br />

( )<br />

( HIC)<br />

*<br />

effec<br />

(13)<br />

∂ HIC<br />

∂t2<br />

= 0<br />

∂<br />

∂t1<br />

= 0 (16)<br />

After obtaining the values of t1 and t2, the peak value of HIC is specified.<br />

4. VALIDATION USING FEM.<br />

For FE analysis of current model, LS-Dyna module of ANSYS software has been<br />

used. For modeling a spherical shell as human head, two concentric spheres have been<br />

considered. Initially two smaller spheres as brain and one bigger sphere as skull were<br />

drawn. Then one of the smaller spheres was deducted from the larger one. The model<br />

was divided to two identical parts which were symmetrical with regard to the sagittal<br />

plane to reduce the computer run time. By defining points and constructing surfaces,<br />

the model was divided to four equal parts to create the mesh. MDT software is applied<br />

to model the torus shape object which has two different radii in impact region. After<br />

constructing the model in MDT, the file is saved as .sat format and introduced to<br />

ANSYS. The model is an object with two radii of 0.03m and 0.045m in the impact<br />

zone. The distance of the spherical shell from the torus body is 0.5mm.

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