Human postburn oedema measured with the impression method

Tactile resonance sensors in medicine

Tactile sensors in general are used for measuring the physical parameters associated with contact between sensor and object. Tactile resonance sensors in particular are based on the principle of measuring the frequency shift, Deltaf, defined as the difference between a freely vibrating sensor resonance frequency and the resonance frequency measured when the sensor makes contact to an object. Deltaf is therefore related to the acoustic impedance of the object and can be used to characterize its material properties. In medicine, tactile resonance sensor systems have been developed for the detection of cancer, human ovum fertility, eye pressure and oedema. In 1992 a Japanese research group published a paper presenting a unique phase shift circuit to facilitate resonance measurements. In this review we summarize the current state-of-the-art of tactile resonance sensors in medicine based on the phase shift circuit and discuss the relevance of the measured parameters for clinical diagnosis. Future trends and applications enabled by this technology are also predicted.

The spatio-temporal strain response of oedematous and nonoedematous tissue to sustained compression in vivo

Poroelastic theory predicts that compression-induced fluid flow through a medium reveals itself via the spatio-temporal behaviour of the strain field. Such strain behaviour has already been observed in simple poroelastic phantoms using generalised elastographic techniques (Berry et al. 2006a, 2006b). The aim of this current study was to investigate the extent to which these techniques could be applied in vivo to image and interpret the compression-induced time-dependent local strain response in soft tissue. Tissue on both arms of six patients presenting with unilateral lymphoedema was subjected to a sustained compression for up to 500 s, and the induced strain was imaged as a function of time. The strain was found to exhibit time-dependent spatially varying behaviour, which we interpret to be consistent with that of a heterogeneous poroelastic material. This occurred in both arms of all patients, although it was more easily seen in the ipsilateral (affected) arm than in the contralateral (apparently unaffected) arm in five out of the six patients. Further work would appear to be worthwhile to determine if poroelasticity imaging could be used in future both to diagnose lymphoedema and to explore the patho-physiology of the condition.

Dielectric measurement in experimental burns: a new tool for burn depth determination?

BACKGROUND

There has been a lack of methods to provide quantitative information of local tissue edema after burn injury. Noninvasive dielectric measurements provide this information. The measured value, the dielectric constant, is directly related to the amount of water in tissue. Using probes of different sizes, the measurements give information from different tissue depths. The aim of this study was to characterize edema formation at different tissue depths and to examine whether the dielectric measurements could be used to distinguish partial- and full-thickness burns in pigs.

METHODS

An experimental animal study with pigs (n = 6) was performed in which dielectric measurements were taken of superficial, partial-thickness, and full-thickness burns for 72 hours.

RESULTS

There was an increase in tissue water content in the superficial dermis in the partial-thickness burns at 48 hours. In whole dermis, the superficial burns resulted in increased tissue water content at 8 hours, and the partial-thickness burns resulted in increased tissue water content at 8, 24, and 72 hours. In deep burns, the water content was significantly decreased in the superficial dermis at 24 hours. All burns resulted in a considerable increase in fat water content. The dielectric probes could be used to differentiate partial- and full-thickness burns as early as 8 hours after burn. Receiver operating curve analysis of the measurements indicated 70 to 90 percent sensitivity and 80 to 100 percent specificity after 8 hours.

CONCLUSIONS

The dielectric measurements provide a sensitive and noninvasive method for examining tissue edema and differentiate partial- and full-thickness burns in experimental burns. Thus, they are of clinical interest for early burn depth determination.

Non-invasive assessment of fluid volume status in the interstitium after haemodialysis

During dialysis excess fluid is removed from uraemic patients. The excess fluid is mainly located in the skin and subcutaneous tissues. In this study we wished, with two noninvasive techniques, the IM (impression method) and BIA (bioimpedance analysis), to study what mechanical (IM) and electrical cellular membrane (BIA) effects the fluid withdrawal has on these tissues. The IM measures the resistive force of the tissues when mechanically compressed. From the force curve two parameters are calculated, the F(0), indicative of interstitial tissue pressure and the FT corresponding to the translocation of tissue fluid (interstitial movable water). The BIA phase angle shift (phi), i.e. geometrical angular transformation of the ratio between reactance and resistance, which has been associated with cellular membrane function, was used as a measurement of electrical cellular membrane effects. Twenty patients were studied before and after haemodialysis measuring the F(0), FT and phi. Theresults showed that the patients lost a median of 3.7 kg during the haemodialysis. F(0) increased until after dialysis, but did not reach significant values, whereas FT increased significantly after dialysis, p < 0.001, as compared with before. After a peak at one hour postdialysis the FT value returned to predialysis values at four hours after termination of dialysis. Also phi increased from before to after dialysis, p < 0.001, but already after one hour it returned to predialysis values. It is common knowledge that dialysis alters the dynamics of fluid in the interstitium of the skin and subcutis. We conclude that the impression method is sensitive enough to detect and chronicle these changes. Furthermore, with the BIA, (phase angle) signs of changes in the electrical properties of the tissues, possibly reflecting cellular membrane function, could be detected.

The effect of burn subeschar tissue fluid on skeletal muscle and hepatic amino acid uptake in an experimental system in vitro

Burn injury is associated with major metabolic disturbances. Many factors or mediators are responsible for post-burn metabolic changes. The present study was designed to test the role of interstitial edema fluid from burn eschar in regulating amino acid transport into hepatic and muscle tissue. Subeschar tissue fluid (SEF) was collected from just under the full thickness burn area. Amino acid transport, determined as the uptake of [3H]-alpha-aminoisobutyric acid by incubated soleus muscles or liver slices in vitro, was reduced after the addition of subeschar tissue fluid. The suppression was more marked with fluids taken from patients with a large burn area. Significant findings were noted when the total surface burn area was more than 70%. There were significant differences in the SEF suppression effect between survivors and non-survivors, but not between inhalation and non-inhalation victims. The results suggest the presence of one or more factors in subeschar tissue fluid that inhibit both muscle and liver amino acid transport. The data also suggest that the inhibitory factors are most likely produced by the burned tissue. This suppression effect may be beneficial to burn victims in maintaining near-normal vascular osmolarity by way of an increased plasma amino acid level.

Non-invasive assessment of intercompartmental fluid shifts in burn victims

Two non-invasive methods (the bioimpedance technique, BIA, and the impression method, IM) were studied, to find out whether they are sensitive enough to detect and chronicle the development of the oedema and fluid resuscitation effects (Parkland formula) that occur secondary to a major burn. Ten patients with a total burned body surface area (TBSA) of more than 10% were included in this prospective study. Total body water (TBW), as measured by the resistance (BIA) or F(0) variable (IM), reached a maximum on day 2. The tissue fluid translocation (INT) variable (IM) followed a different course, increasing slowly to reach a maximum on day 6, when it was 40% higher than the 12 h value. TBW and the interstitial translocatable fluid were still increased 1 week post-burn. The non-invasive measurements of TBW (resistance by BIA and F(0) by IM) reflected the anticipated changes in TBW. The phase angle (BIA) indicative of cellular membrane effects of burn and sepsis had its lowest values at day 1.5, and stayed significantly low until day 4. Interestingly, the phase angle was lowest in the two cases that died subsequently. The different time course of the INT value (IM), which reflected the translocatable interstitial fluid volume in skin, may be the result of resuscitation fluid remaining in this compartment, due to the excess sodium content together with a possible change in tissue compliance secondary to the early total water peak on day 2.

An in vivo method for measuring the mechanical properties of the skin using ultrasound

In this study, we report a new and original device called the "echorheometer," comprising a suction system with an ultrasound scanner (A-mode, TM-mode and B-mode) that enables the simultaneous visualization and measurement of the deformation of skin structures in vivo. With the scanner described here, high resolution is obtained using a strongly focused, wide-band 20-MHz center frequency transducer, with an axial resolution of 0.07 mm. This device can determine, noninvasively, not only those skin structures that are involved in the deformation, but also their morphological variation and their extent of involvement with the degree of stress applied. Using this device, the behavior of the dermis and subcutaneous fat, while under suction, was investigated on the volar forearm of 10 volunteers. The results showed that the resistance to the applied vertical stress is essentially due to the dermis rather than the subcutaneous fat, and that there is a certain amount of infiltration of fluid into the tissues under suction. In addition, it was shown that the dermal response to an applied suction is initially due to its own natural tension and that, with increasing deformation, the intrinsic dermal elasticity has a greater contribution to the resistance of stress. With this information, we hope to develop a mechanical model to define appropriate mechanical parameters for skin. This will allow the evaluation of changes in the dermis and also enable therapeutic intervention to be assessed. Furthermore, it could also be applied to studies of skin ageing and the assessment of cosmetic product efficacy (emolliency, hydratation, etc.).

The evaluation of a biexponential model for description of intercompartmental fluid shifts in compressed oedematous tissue

A parametric model was fitted to force curve data gained by a non-invasive impression method that measures force and fluid translocation during mechanical compression of the skin. The ability of the model parameters to estimate high- and low-viscosity fluid flow in compressed areas were evaluated in a silicone rubber model and in six patients with chronic pitting oedema. Different softnesses of silicone rubber gave significantly different parameter values. The flow properties of the silicone model could be analysed in detail with the suggested model. Parameter analysis showed a higher fraction of low-viscosity fluid for oedema than for reference sites. The model parameters could be interpreted in softness value according to an international standard for consistency (ISO 2137). The suggested parametric model gave reliable and detailed information about high- and low-viscosity fluid flow and can be used to estimate intercompartmental fluid shifts in oedematous tissue.