SAMPE Journal - January/February 2017 - 44

Feature Article
Figure 5. Geometry and boundary
conditions of the thermal threedimensional model.

surface is calculated. Therefore an
external current density is defined
on the coil connection point. The
external current density is defined as
followed:

[1]
Je is the external current density, p
is the generator power in percentage
of the maximum generator power,

I10 is the experimental determined
average electric current at 10%
generator power (637 Ampere), do
and di are the pipe outer and inner
diameter respectively (do= 3 mm and
di= 2 mm).
In a second step the electromagnetic
field and joule losses in the two
laminates are calculated. The
calculated surface current density
on the coil surface and the generator
frequency (400 kHz) are the input
parameters.

In the third step the temperature
of the laminates are calculated. The
before calculated joule losses are
implemented as an internal heat
source inside the laminate. The
solution is generated by moving
the material stepwise against
the process direction while the
overall net of the model is fixed.
For each material movement the
temperature is calculated. Due to
the constant boundary conditions
the calculation is finished and the
simulation converged, when a state
of equilibrium is reached and the
calculated temperature distribution
in the laminates doesn't change with
the next material movement.

Figure 6. Process diagram specification based on the surface and joining temperature in the middle of the joining area.
44

SAMPE Journal, Volume 53, No. 1, January/February 2017



Table of Contents for the Digital Edition of SAMPE Journal - January/February 2017

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