摘要
The transdermal delivery of therapeutics is limited to only a few molecules due to the outermost layer of
skin, the stratum corneum, which acts as a barrier against the ingress of substances into the body.
Microneedle arrays, which are commonly between 70μm and 900μm in length, have been developed as
a method of promoting drug and vaccine delivery by creating microperforations in the stratum corneum
to increase transport into the skin. The design of microneedle devices has significantly developed over
recent years to allow for the delivery of numerous compounds into in vivo and ex vivo skin. Microneedle
devices are now beginning to be taken away from the laboratory and towards clinical use but to achieve
this it is desirable that all microneedles within the device penetrate skin in vivo to a sufficient depth. As
microneedle devices have been extensively tested in cadaver tissue, a greater understanding of the
mechanical properties of skin in vivo and ex vivo is required and to hypothesise whether animal models
such as murine skin ex vivo serves as an appropriate model for human skin ex vivo.
Measurements were performed on human skin in vivo by applying small cylindrical and spherical
indenters to the volar aspect of the forearm on 7 volunteers. The average Young’s Modulus of the skin
was 39.64kPa and 65.86kPa when applying the spherical and cylindrical indenters respectively. In a
series of tensile measurements performed at three load axis orientations using ex vivo samples from
human and murine donors, it was found that the key variation was attributed to the deformation
experienced at initial low loads. This was shown to be significantly longer for human skin with an
average of 5.10mm, when compared with murine skin which had an average of 1.61mm (p<0.05).
Histological examination showed that human skin was far thicker, with an increased volume of dermal
tissue, compared with murine skin, and this anatomical variation may have been the main reason why
human and murine skin exhibited different mechanical properties.
Finite element models (FEMs) were established of skin indentation in vivo, which incorporated the
epidermis, dermis and hypodermis, and of human and murine skin in tension. Appropriate boundary
conditions and mesh densities were implemented and the geometries were taken from real life
measurements where possible. The Ogden material model of hyperelasticity was chosen to represent
the skin layers for the FEM of skin indentation and an anisotropic material was used to describe human
and murine skin in tension by adapting the Weiss et al model of transverse isotropy.
Inverse finite element analysis was then used to match the FEMs with the experimental measurements.
The multilayered FEM of skin was correlated against the in vivo indentation tests where model and
experimental fit gave average root mean squared errors (R2
ave) of between 0.00103 and 0.0488 for the 7
volunteers. The optimal material parameters showed correlations with experimental measurements,
where volunteers 1, 6 and 7 were shown to have the stiffest skin through Young’s Modulus calculations,
which was reflected in the increased nonlinearity of the parameters extracted for the hypodermal layer.
A stronger agreement between model and experiment for the anisotropic model of human and murine
skin in tension was shown where the R2
ave was between 0.0038 and 0.0163. Again, model and
experimental observations were shown to correlate where there was a significant difference (p<0.05)
between 6 of the 14 average material parameters (C2, C3,1, λ1, C3,2, C3,3, λ3) when comparing human to
murine skin.
The multilayered FEM of human skin in vivo was further validated by modelling the application of a
single microneedle to skin, prior to penetration. The model was then correlated against in vivo
measurements performed on one of the volunteers and it was found that the model provided a good
approximation for the experimental measurements. Using the multilayered FEM of human skin
indentation, it was possible to model the deflection of the skin during the application of a pressure load
comparable to microneedle array application. This allowed for the development of several curved
microneedle arrays which aimed to distribute the load over all microneedles to potentially create uniform
skin penetration by all those within the array. The microneedles were manufactured simply and quickly
using wire cutting technologies from stainless steel and tested in human skin in vivo and in ex vivo
samples of human and murine skin, where methylene blue was applied to identify any microchannels
created by the microneedles. Preliminary measurements taken from murine skin ex vivo were
discounted as microchannel staining was not possible. Analyses performed on human skin ex vivo
showed penetration at high loads (4-5N) for all four microneedle array designs and the microneedle
array with the smallest curvature (0.95mm) had the most consistent puncture for all microneedles,
however puncture in vivo was difficult to characterise using approach developed. Therefore further work
is required to assess more volunteers and donors.
This study has highlighted the great differences in the mechanical properties of human and murine skin,
suggesting that murine skin is not an appropriate model to assess microneedle puncture. It has also
shown that the underlying tissues and hypodermis play a pivotal role in microneedle insertion mechanics.