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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

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Objectives<br />

Long bone failure characteristics under<br />

impact bending: an in-depth study<br />

Mike WJ Arun, A Chawla, S Mukherjee, Debasis Sahoo, Sourabh Barouah<br />

The objective of the current work is to exper-<br />

imentally study the tolerance of long bones<br />

bending under impact and to understand the<br />

mechanism which causes their failure.<br />

Materials & Methods<br />

Twelve isolated human humerus were tested<br />

in three point bending mode in the anterior<br />

to posterior direction. Bone specimens were<br />

“potted” with fixtures using a quick setting<br />

bone cement (Poly Methyl Methacrylate, PM-<br />

MA).<br />

Figure 1 Drop tower setup<br />

An instrumented drop tower was used to im-<br />

pact the bone. The drop tower consists of a car-<br />

riage of mass 31 kg that can fall freely through<br />

guided slots. The height of the drop can be ad-<br />

justed to vary impact velocity.<br />

Results<br />

Figure 2 shows the force vs time plot for the ex-<br />

periments. All plots are plotted till the fracture<br />

initiation as observed in high-speed videos.<br />

Indian Institute of Technology, Delhi, India<br />

1.5 m drop 1.0 m drop<br />

0.5 m drop Average<br />

Figure 2 Force-Time plots<br />

The average load taken by the bones for both<br />

1.5 m and 1.0 m drop was around 2.7 kN, while<br />

for 0.5 m drop it was 1.9 kN . Thus there was<br />

a 30% increase in maximum load at higher<br />

drop heights (i.e. higher strain rates), which is<br />

a well-documented behavior of bones. In 1.0<br />

m drop tests, the force vs time plots had two<br />

peaks before failure. This phenomenon was<br />

due to the inertial effect. For 1.0 m drop, the<br />

average time to fracture was 0.57 ms and for<br />

1.5 m drop, it was 0.3 ms. The slope of the force<br />

history during the first peak was observed to<br />

be the highest (20.1 kN/ms) in the 1.5 m drop<br />

case while the 0.5 m drop tests recorded the<br />

lowest (10.4 kN/ms). This shows an increase<br />

in bone stiffness with increase in impact ve-<br />

locity and signifies the strain rate dependen-<br />

cy of bones. It was observed that the average<br />

time for fracture propagation across the ten-<br />

sile side of bending was 0.1 ms, while across<br />

the compressive side was 0.8 ms. This is due<br />

to the asymmetric strength of bone in ten-<br />

sion and compression. Eleven fractures were<br />

oblique and one fracture was transverse in na-<br />

ture. Eight of the oblique fractures were of the<br />

pattern as shown in Figure 3.a, where there<br />

was a crack diversion in the compression side<br />

of impact. These fractures are observed only in<br />

1.5 m and 1.0 m drop experiments. The other<br />

three were of the pattern as shown in Figure<br />

3.b, where there was no crack diversion in the<br />

compression side of impact. This pattern is ob-<br />

served only in 0.5 m drop tests. The transverse<br />

fracture is shown in Figure 3.c.<br />

b. Oblique fracture with no<br />

crack diversion<br />

Figure 3 Observed fracture types<br />

a. Oblique fracture with<br />

crack diversion<br />

c. Transverse fracture<br />

The fracture event captured by high speed<br />

camera is shown in Figure 4.<br />

a. at time=0.26ms b. at time=0.37ms c. at time=1.1ms<br />

Figure 4 Fracture captured by high speed camera<br />

Conclusion<br />

A detailed experimental work had been carried<br />

out to study the tolerance and the mechanism<br />

of fracture in long bones. Interesting observa-<br />

tions have been made, which were not previ-<br />

ously reported. This information can be used<br />

effectively to derive material models that can<br />

be used in finite element simulations.

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