AISIM 3 Rheology of the liver |
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Le texte suivant (en anglais) est la synthèse d'un échange d'e-mail entre Marc
Thiriet et Fiona Carter a propos de la rhéologie du foie.
Fiona Carter
To summarise, I cannot fully explain why we are getting such vastly
different results without knowing a little more about Dan's
experimental methods. There could be a number of reasons for the
disparity and I would be more than happy to discuss them further if
you want to give me a few more clues.
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there is two strategies, both useful for our work
(biomechanical modelling and augmented reality imaging)
Here is an e-mail exchange between Fiona Carter and
Marc Thiriet
I would like to have further informations
on your results
my questions are
All of the stress-strain curves for human liver indentation tests are
in-vivo. We have done no post-mortem studies in humans due to the
fact that extensive investigations were performed on excised animal
tissue and we really wanted to move on to look at living human
tissue.
The values in the table are ex-vivo for pig liver and in-vivo for
human liver (curves for one subject shown). As I mentioned in my
talk, you can only consider a linear relationship between stress and
strain at very low levels of strain. For this reason I was pretty
careful not to call this relationship Young's modulus - there is no
single value for Young's modulus of biological tissue. The figures
in the table indicate the gradient of the curve up to 10% strain. It
is very important to note that once strain levels increase beyond
this level, the initial linear gradient given will not characterise
the tissue accurately. Thus far 8 patients with normal liver tissue
have been examined and the initial linear gradient values have fallen
in the range given. I also briefly mentioned that it may be possible
to characterise more of the stress-strain curve by considering an
exponential relationship. This analysis is ongoing in my department
at present.
Research Assistant
Dept. of Surgery
Level 6
Ninewells Hospital and Medical School
DUNDEE DD1 9SY
Scotland
01382 660111 ext:32561
f.j.carter@dundee.ac.uk
a rapid check give indeed a crude value
of 2.e5 between .05 and 1
the order of magnitude is 1.e3
higher than in vitro test given to us by Dan D.
the specimen being tested in fluid.
What is your opinion with this discrepency
in vitro - not dry - vs. in vivo.
I think that I discussed these experiments with the person in
question briefly during my visit to Sophia. It was my understanding
that the methods for Dan's experiment involve cutting
segments/sections out of intact liver tissue. It was not clear to me
if this was human liver or animal liver and another important factor
is how these sections were stored and how soon they were tested
post-mortem. In pig liver, and to a lesser extent in human liver,
there is a dense fibrous tissue network surrounding the liver lobules
which acts as a support structure for the whole organ. Depending on
the size of Dan's samples taken from the liver, a certain amount of
this support structure will be lost and this may effect the measured
compliance.
In our in-vivo tests the organ was intact with it's normal blood
supply still in place. I have found a marked increase in compliance
when excised tissues have been reperfused before testing - this may
be another part explanation in the differences between our results.
Another structure which has vital importance for the liver's
mechanical properties is the surface region (Glisson's capsule),
which is made up of densely packed fibrous tissue (mainly collagen).
The presence or absence of this layer has a marked affect on the
tissue properties - if the surface capsule is removed or damaged you
definitely will notice a marked reduction in tissue stiffness.
Finally, I seem to recall that the liver samples in Dan's tests were
impacted at high speeds. In our tests we merely indent the surface
of an organ at speeds between 1-2mm/sec using a small blunt indentor.
I would have thought that using a higher strain rate would in fact
produce a higher value for the elastic modulus with the tissue
behaving as a stiffer material - so I can't see why Dan's results
would give a lower value than ours if this were the only difference !
Dan's harmonic compression tests were performed on
parenchyma cylindrical samples
(height of 10mm, diameter of 20mm)
without large vessels.
The tests were carried out on specimens
immerged in petroleum bath to avoid
deshydratation and to put fluid inside
the sample.
The bath temperature was maintained
at 25 degrees Celsius.o
It sounds like the tests you describe are to measure the bulk
modulus of the liver tissue (this value should be approaching that of
water - i.e. that the tissue is virtually incompressible). Our two
centres approach' to the question of biomechanical measurement are
fundamentally different. To cut out very small samples (with respect
to the total size of the organ) and immerse them in petroleum is
basically treating biological tissue as an engineering material. You
would perform this sort of test on something like rubber where taking
a small sample from the whole should not affect it's intrinsic
properties. In our centre we try to devise tests that involve
testing the tissue in it's natural physiologial state - i.e. with the
blood supply and the fibrous support system intact, filled with and
surrounded by natural body fluids and at body temperature (37.4 deg).
It seems very clear to me that if you treat a complex biological
tissue as a homogenous engineering material there will be
difficulties in extrapolating the results to the systemic, in-vivo
situation.
There are a few issues here:
In summary, I think that the most important reason why Dan's
experiments yield lower elasticity values than our experiments is due
to the effect of cutting out small samples from the tissue. I
suppose that I could try preparing similar samples here and testing
them using our methods, to see if I get similar figures to Dan. If I
get some time then I will have a look at this.
It has been recognised since the mid 1960's biological tissue has
very complex mechanical properties and that devising methods to tests
these properties is problematic. Early methods of testing soft
tissues (such as mesentery or muscle) involved cutting strips from an
excised organ and performing simple extension tests (uniaxial) - see
Fung, Am. J. Physiol. 1967 for good descriptions. When some
investigators looked at tethering all the free edges of the specimen
(biaxial tension tests) they found that the same material yielded
quite different results - in general samples that were tethered
around all free edges behaved as a stiffer material than those in
uniaxial tension.
The suggested reason is that, although you may need to treat
biological tissue as homogenous for modelling purposes, the
microscopic structure of the tissue is very complex. Tissue fibres
which give mechanical support to the tissue, run through it in many
directions. If a tissue is cut then these tissue fibres are damaged
and some of the support is lost. One way to overcome this problem in
extension tests is to fix all the free edges of the specimen - trying
to mimic the in-vivo situation. This is still far from ideal though
since any manipulation of the tissue (attaching hooks or stitches for
example) will further damage the tissue and affect it's mechanical
response to stress.
Several centres studying soft tissue biomechanics have moved away
from small sample testing and endeavour to devise methods to measure
elasticity of whole organs or systems. These methods are generally
very complex and involve large and expensive imaging methods - e.g
the breast elastography techniques used at the Mayo Clinic (R Ehman)
using MRI. At our centre we used simple methods initially to get
some basic data about the tissues and then developed novel
instrumentation to get information from the tissue in it's natural
state.
I suggest that one reason that the elasticity constant, from Dan's
liver experiments, is lower than ours is because of the tissue
samples tested. You mention that the samples were free of large
blood vessels - these are an important support structure in the
intact organ, both physiologically and mechanically. In our early
tests on liver we looked at indenting the surface of an organ
with the surface capsule removed - i.e. the surface raw or damaged -
similar to Dan's liver samples. Indentation tests showed that the
tissue compliance increased significantly - initial elastic modulus
value around 0.03-0.06 MPa for sheep liver ex-vivo.
Since 70-80% of biological tissue is made up of water then the fluid
supply to the tissue is of vital importance. In pathological
situations, an increased vascularity (blood flow) to an area will
result in the local area becoming swollen and stiffer initially.
Likewise, if blood supply is removed e.g. in an excised organ, then
the tissue will be more flaccid and compliant. We have found that
reperfusing excised tissue with a physiological fluid significantly
affects it's elasticity (experiments with pig and sheep spleen).
There are also subtle differences between reperfusing tissue with an
isotonic solution and with water - water produces increased tissue
swelling and stiffness even in dead tissue. This is partly due to
osmosis, the means by which cells take up or release water.
I am not sure what osmotic effect petroleum will have on liver
tissue but I doubt that it will be improving the tissue's fluid
balance.
Some authors have found that altering the rate of strain applied to
the tissue sample affects the measured tissue stiffness. There is
little agreement in this area however, we have found that reducing
the indentation speed to 0.15mm/sec affects the measured tissue
response as there is some stress relaxation occurring during the test.
Since our interest is in surgical interventions with tissue, we have
limited the speed of indentations between 1-2mm/sec and have found no
variation in elastic response in this range.
You have not mentioned the testing speed so I cannot comment much
further here - except to say that it would probably not make much
difference.
Again, there should be little difference in results due to
temperature as our ex-vivo tests were performed at room temperature
and the in-vivo tests at body temperature. It is expected that the
high water content of biological tissue will be the main factor
influencing how elasticity changes with lower temperature and the
protein content of tissue influencing the elasticity at high
temperature (denaturation or 'cooking' occuring).
further to our correspondance, I did some test on samples of fresh
pig liver Friday may 21st. Using cylindrical sections (20mm diam, 10mm
depth) held in rigid containers I indented them using our testing
methods. The results for tissue samples which still had the surface
capsule, the initial gradient up to 10% strain was roughly 2kPa,
removing the surface capsule roughly halves the initial gradient
value (1kPa).
I think that this simple test reinforces the idea that
removing small sections of liver and testing them individually will
give much lower values of elasticity.