41 research outputs found

    Hyperelastic Material Properties of Mouse Skin under Compression

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    The skin is a dynamic organ whose complex material properties are capable of withstanding continuous mechanical stress while accommodating insults and organism growth. Moreover, synchronized hair cycles, comprising waves of hair growth, regression and rest, are accompanied by dramatic fluctuations in skin thickness in mice. Whether such structural changes alter skin mechanics is unknown. Mouse models are extensively used to study skin biology and pathophysiology, including aging, UV-induced skin damage and somatosensory signaling. As the skin serves a pivotal role in the transfer function from sensory stimuli to neuronal signaling, we sought to define the mechanical properties of mouse skin over a range of normal physiological states. Skin thickness, stiffness and modulus were quantitatively surveyed in adult, female mice (Mus musculus). These measures were analyzed under uniaxial compression, which is relevant for touch reception and compression injuries, rather than tension, which is typically used to analyze skin mechanics. Compression tests were performed with 105 full-thickness, freshly isolated specimens from the hairy skin of the hind limb. Physiological variables included body weight, hair-cycle stage, maturity level, skin site and individual animal differences. Skin thickness and stiffness were dominated by hair-cycle stage at young (6ā€“10 weeks) and intermediate (13ā€“19 weeks) adult ages but by body weight in mature mice (26ā€“34 weeks). Interestingly, stiffness varied inversely with thickness so that hyperelastic modulus was consistent across hair-cycle stages and body weights. By contrast, the mechanics of hairy skin differs markedly with anatomical location. In particular, skin containing fascial structures such as nerves and blood vessels showed significantly greater modulus than adjacent sites. Collectively, this systematic survey indicates that, although its structure changes dramatically throughout adult life, mouse skin at a given location maintains a constant elastic modulus to compression throughout normal physiological stages

    Timp-3 deficiency impairs cognitive function in mice

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    Extracellular matrix (ECM) degradation is performed primarily by matrix metalloproteinases (MMPs). MMPs have recently been shown to regulate synaptic activity in the hippocampus and to affect memory and learning. The tissue inhibitor of metalloproteinase (Timp) is an endogenous factor that controls MMP activity by binding to the catalytic site of MMPs. At present, four Timp isotypes have been reported (Timp-1 through Timp-4) with 35ā€“50% amino-acid sequence homology. Timp-3 is a unique member of Timp proteins in that it is bound to the ECM. In this study, we used the passive avoidance test, active avoidance test, and water maze test to examine the cognitive function in Timp-3 knockout (KO) mice. Habituation was evaluated using the open-field test. The water maze test showed that Timp-3 KO mice exhibit deterioration in cognitive function compared with wild-type (WT) mice. The open-field test showed decreased habituation of Timp-3 KO mice. Immunostaining of brain slices revealed the expression of Timp-3 in the hippocampus. In situ zymography of the hippocampus showed increased gelatinolytic activity in Timp-3 KO mice compared with WT mice. These results present the first evidence of Timp-3 involvement in cognitive function and hippocampal MMP activity in mice. Moreover, our findings suggest a novel therapeutic target to be explored for improvement of cognitive function in humans

    Compressive viscoelasticity of freshly excised mouse skin is dependent on specimen thickness, strain level and rate.

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    Although the skin's mechanical properties are well characterized in tension, little work has been done in compression. Here, the viscoelastic properties of a population of mouse skin specimens (139 samples from 36 mice, aged 5 to 34 weeks) were characterized upon varying specimen thickness, as well as strain level and rate. Over the population, we observed the skin's viscoelasticity to be quite variable, yet found systematic correlation of residual stress ratio with skin thickness and strain, and of relaxation time constants with strain rates. In particular, as specimen thickness ranged from 211 to 671 Ī¼m, we observed significant variation in both quasi-linear viscoelasticity (QLV) parameters, the relaxation time constant (Ļ„1 = 0.19 Ā± 0.10 s) and steady-state residual stress ratio (Gāˆž = 0.28 Ā± 0.13). Moreover, when Ļ„1 was decoupled and fixed, we observed that Gāˆž positively correlated with skin thickness. Second, as steady-state stretch was increased (Ī»āˆž from 0.22 to 0.81), we observed significant variation in both QLV parameters (Ļ„1 = 0.26 Ā± 0.14 s, Gāˆž = 0.47 Ā± 0.17), and when Ļ„1 was fixed, Gāˆž positively correlated with stretch level. Third, as strain rate was increased from 0.06 to 22.88 s-1, the median time constant Ļ„1 varied from 1.90 to 0.31 s, and thereby negatively correlated with strain rate. These findings indicate that the natural range of specimen thickness, as well as experimental controls of compression level and rate, significantly influence measurements of skin viscoelasticity

    Touch Receptors Undergo Rapid Remodeling in Healthy Skin

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    Sensory tissues exposed to the environment, such as skin, olfactory epithelia, and taste buds, continuously renew; therefore, peripheral neurons must have mechanisms to maintain appropriate innervation patterns. Although somatosensory neurons regenerate after injury, little is known about how these neurons cope with normal target organ changes. To elucidate neuronal plasticity in healthy skin, we analyzed the structure of Merkel-cell afferents, which are gentle touch receptors, during skin remodeling that accompanies mouse hair-follicle regeneration. The number of Merkel cells is reduced by 90% and axonal arbors are simplified during active hair growth. These structures rebound within just days. Computational modeling predicts that Merkel-cell changes are probabilistic, but myelinated branch stability depends on Merkel-cell inputs. Electrophysiology and behavior demonstrate that tactile responsiveness is less reliable during active growth than in resting skin. These results reveal that somatosensory neurons display structural plasticity at the cost of impairment in the reliability of encoding gentle touch

    Focused ultrasound excites action potentials in mammalian peripheral neurons in part through the mechanically gated ion channel PIEZO2.

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    Neurons of the peripheral nervous system (PNS) are tasked with diverse roles, from encoding touch, pain, and itch to interoceptive control of inflammation and organ physiology. Thus, technologies that allow precise control of peripheral nerve activity have the potential to regulate a wide range of biological processes. Noninvasive modulation of neuronal activity is an important translational application of focused ultrasound (FUS). Recent studies have identified effective strategies to modulate brain circuits; however, reliable parameters to control the activity of the PNS are lacking. To develop robust noninvasive technologies for peripheral nerve modulation, we employed targeted FUS stimulation and electrophysiology in mouse ex vivo skin-saphenous nerve preparations to record the activity of individual mechanosensory neurons. Parameter space exploration showed that stimulating neuronal receptive fields with high-intensity, millisecond FUS pulses reliably and repeatedly evoked one-to-one action potentials in all peripheral neurons recorded. Interestingly, when neurons were classified based on neurophysiological properties, we identified a discrete range of FUS parameters capable of exciting all neuronal classes, including myelinated A fibers and unmyelinated C fibers. Peripheral neurons were excited by FUS stimulation targeted to either cutaneous receptive fields or peripheral nerves, a key finding that increases the therapeutic range of FUS-based peripheral neuromodulation. FUS elicited action potentials with millisecond latencies compared with electrical stimulation, suggesting ion channelā€“mediated mechanisms. Indeed, FUS thresholds were elevated in neurons lacking the mechanically gated channel PIEZO2. Together, these results demonstrate that transcutaneous FUS drives peripheral nerve activity by engaging intrinsic mechanotransduction mechanisms in neurons [B. U. Hoffman, PhD thesis, (2019)]

    FE simulations for a skin thickness of 400 Ī¼m, at stretch levels of 0.5, 0.6 and 0.7, under frictionless (solid lines) and rough (dashed lines) friction conditions.

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    <p>A: displacement stimuli to achieve desired stretch level; B: responsive force traces for three stretch levels under different frictional conditions; C: calculated relaxation function for force traces shown in B. Note that while frictional conditions have an impact on responsive force traces, they do not impact the calculated viscoelastic reduced relaxation function.</p

    Correlations between skin thickness/stretch level and residual stress ratio (<i>G</i><sub><i>āˆž</i></sub>).

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    <p>A: In the first experiment where only thickness varied, the steady-state residual stress ratio (<i>G</i><sub><i>āˆž</i></sub>) correlates with increasing skin thickness, <i>n</i> = 44. Linear regression (solid line) with residual stress ratio <i>G</i><sub><i>āˆž</i></sub> as the dependent variable was performed, which returns <i>p</i> < 0.001 for independent variable thickness <i>l</i><sub>0</sub>, and <i>G</i><sub><i>āˆž</i></sub> = 9.997 Ɨ 10<sup>āˆ’4</sup> Ī¼m<sup>āˆ’1</sup> ā‹… <i>l</i><sub>0</sub> + 0.077. In the second experiment where both thickness and strain level varied, the residual stress ratio (<i>G</i><sub><i>āˆž</i></sub>) correlates with both B: stretch and C: skin thickness. Note that the two correlations are independent from each other because there is no correlation between stretch and skin thickness. Multilinear regression with residual stress ratio <i>G</i><sub><i>āˆž</i></sub> was also performed, which returns <i>p</i> < 0.001 for independent variable stretch <i>Ī»</i><sub><i>āˆž</i></sub>, <i>p</i> < 0.001 for independent variable thickness <i>l</i><sub>0</sub>, and <i>G</i><sub><i>āˆž</i></sub> = 0.810 ā‹… <i>Ī»</i><sub><i>āˆž</i></sub> + 4.25 Ɨ 10<sup>āˆ’4</sup> Ī¼m<sup>āˆ’1</sup> ā‹… <i>l</i><sub>0</sub>ā€“0.074. Note that in B and C, solid lines are single-linear regressions for residual stress ratio with respect to stretch and thickness respectively.</p

    Example run of the compressive test procedure for one skin specimen when varying strain rates.

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    <p>A: Position of the compression platen over time, as measured by its distance from the fixed platform. B: Reaction force at the compression platen. C: Magnified view of reaction force and platen position for Compression 6, demonstrating that ā€œskin thicknessā€ was defined by ā€œcontact pointā€ as determined from the force trace. The platen was moved into the skin with an acceleration of 0.06 s<sup>āˆ’1</sup> for each of the first 10 repetitions. Then, 10 additional compressions were performed at 22.88 s<sup>āˆ’1</sup>. The 6th compression was analyzed in each sequence of 10 compressions.</p
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