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TR Circular E-C058_9th LRT Conference_2003.pdf - Florida ...

TR Circular E-C058_9th LRT Conference_2003.pdf - Florida ...

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124 Transportation Research <strong>Circular</strong> E-<strong>C058</strong>: <strong>9th</strong> National Light Rail Transit <strong>Conference</strong><br />

Derailment Investigation Approach<br />

The wheel to rail interface was exhaustively investigated, and complex mathematical models<br />

were developed to simulate the behavior of the vehicle on measured Green Line track geometry<br />

and irregularities. The aim of this investigation was to isolate the detailed mechanics of the<br />

derailment, and to identify appropriate corrective action strategies.<br />

Initial work focused on addressing the derailments using the simple Nadal theory as a<br />

safety limit (Figure 2). This limit remains a conservative one; although, for an independent<br />

wheel, more accurate approaches can be employed when full details of the wheel-to-rail interface<br />

are available. Initial efforts were focused on increasing the Nadal limiting value by addressing<br />

the most controllable variable—the effective flange angle. The original wheel profile design<br />

employed a 63-degree flange angle, driven by the fact that all other vehicles on the Green Line<br />

use such a profile. Analysis quickly showed that a change to a more modern 75° flange angle<br />

was feasible and should deliver significant increases in the derailment safety margin by<br />

increasing the Nadal limit. Considered simply, for a constant vertical load, the tolerable lateral<br />

force between wheel and rail could be increased by 53% by changing the flange angle. In order<br />

to confirm the validity of this premise, an extensive investigation was launched.<br />

The conceptual approach followed during the investigation is shown in Figure 3. This<br />

approach was followed to develop, refine, and validate an accurate dynamic model of the vehicle<br />

Vertical Load – V<br />

Nadal’s limit:<br />

Lateral<br />

Force – L<br />

L<br />

V<br />

Tan δ − µ<br />

=<br />

1+<br />

Tan δ<br />

Where µ is the coefficient of friction<br />

between wheel and rail<br />

Effective Flange Angle δ<br />

FIGURE 2 Nadal’s derailment theory.

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