Three-Dimensional Radiofrequency Tissue Tightening: A Proposed Mechanism and Applications for Body Contouring

An ex-vivo study was conducted to measure subcutaneous collagenous tissue contraction with simultaneous monitoring of local tissue temperature to determine the threshold temperature of the collagen shrinkage. Three types of collagenous tissue were studied for thermal-induced contraction: (1) adipose tissue with septal and reticular connective tissue, (2) dermis, and (3) fascia.

Samples of ex vivo human tissue were taken from an abdominoplasty surgery and were tested within 10 min of excision. Immediate thermal testing was performed to minimize changes in tissue related to long storage and temperature variation or change of liquid content, including blood and lymphatic content. The tissue samples were placed between the two BodyTite™ (Invasix Ltd., Israel) RF electrodes, where the small-area, internal RF-active electrodes (cannula) were placed in contact with the studied tissue and the other large-area electrode was applied to the opposite side, or epidermal side, of the sample. Large samples of subcutaneous tissue were used, allowing observation of any contraction behavior in the tissue’s native environment in connection with its entire matrix structure. Two marks were placed 1 cm from the active internal electrode to visualize tissue displacement. The experiment design setup is shown in Fig. 1.

RF energy was delivered by the BodyTite device. The delivered power was 70 W at 1 MHz, and energy was delivered until evaporation of water from the adipocytes was observed. Video and thermal cameras (FLIR A-320) were used to monitor tissue displacement and temperature change during the treatment. The start of tissue displacement was correlated with tissue temperature to determine the contraction thermal threshold. Each experiment was repeated three times for each type of tissue to sample tissue averages and avoid measurements of random events.

Twenty-four consecutive patients, 22 female and 2 male, underwent RFAL to the abdomen and hips. The average age was 39.7 years (range = 19-52 years). The average preoperative weight was 71 kg. The selected patients were typical patients indicated for a liposuction procedure. All patients were healthy anesthetic risks and active with no significant medical diseases. Fifteen of 24 patients had a normal BMI (<25), while 9/24 patients were moderately overweight (BMI = 25–30) and 3 patients were obese (30 < BMI < 32).

RFAL was performed using the BodyTite device. The BodyTite device deploys a handpiece to deliver radiofrequency energy to the adipose tissue and skin. The internal cannula is coated with dielectric material and has a conductive tip that emits RF energy into the adipose tissue toward the skin surface. RF energy flows between the tip of the internal cannula and external electrode creating a localized, confined thermal effect between them. The internal cannula is inserted into the pretumesced fat to be contoured and is moved gently back and forth at various predetermined and controlled depths for uniform heating of the treated volume. There is also an external electrode that moves along the surface of the skin in tandem vertical alignment with the tip of the internal cannula (Fig. 2). The subcutaneous tissue and skin between the electrodes experience a significant thermal effect which is maximal near the tip of the internal cannula and decreases in intensity toward the skin electrode The operator controls the depth of the internal cannula within a predetermined range of 5–50 mm and moves the handpiece back and forth through the desired fat volume to be contoured. The RF energy coagulates the adipose, connective, and vascular tissues in the vicinity of the internal cannula tip and gently heats the dermis below the external electrode. The internal electrode also serves as an asynchronous internal suction cannula, aspirating the coagulated adipose, vascular, and fibrous tissues.

The RF power, in the range of 40–70 W, was used for uniform heating throughout a thick subcutaneous flap. The average total energy of about 72 kJ was delivered to the abdominal area. The temperature around the tip of the cannula reached 70-80°C. This internal temperature was observed using thermography on tissue cross section for preabdominoplasty patients treated with RFAL when the skin surface temperature reached 38–42°C (see Fig. 3, cross section of lower abdominal tissue showing the thermal image of the skin surface and tissue incision allowing visualization of the thermal profile of the internal subcutaneous temperature). The target skin temperature was monitored and controlled with a thermal sensor built into the external electrode. The sensor provides continuous real-time epidermal temperature monitoring and feedback loop control of RF power. The system was set to a target temperature of 38–42°C, which was maintained for 1–3 min. The strong and sustained tissue heating during the procedure results in thermal stimulation of the subdermal layer, the entire matrix of adipose tissue, and the vertical and oblique fibrous septa, eliciting a powerful three-dimensional retraction and contraction of the entire soft tissue envelope.

The distance between the internal and external electrodes was controlled with an eccentric spring-loaded mechanism that keeps the external electrode on the surface of the skin at all times. The device also controls vaporization and prevents carbonization around the tip of the cannula. When evaporation around the internal cannula occurs, the tissue impedance rises and exceeds the online monitored high impedance and the device shuts off the RF energy.

All patients had their treatment area infiltrated with tumescent anesthesia prior to the RFAL procedure. Tumescent anesthesia is critical in the technique as the RF current travels through tissue most efficiently in a salinated environment.

The objective of this in vivo portion of the study was to optimize treatment parameters and correlate treatment soft tissue contraction results with procedure and patient variables, including amount of deposed RF energy, body mass index (BMI) of the patients, and amount of aspirated fat.

A zone measuring as large as 15 × 10 cm (150 cm²) may be heated to critical target temperature within 3–8 min depending on the thickness of the treated fat layer and then uniform volumetric heating can be safely performed to reach uniform temperature distribution over the entire treated volume.

All patients from the study were followed up at 6, 12, and 24 weeks. To measure linear contraction, the distance between two fixed points was measured preoperatively and then at the 24-week postoperative visit. Distances between incision ports and natural “fixed” anatomical registration points, such as moles or the umbilicus, were measured before the treatment, after the treatment, and at 3- and 6-month follow-up visits. The linear contraction was measured as relative change of distance between two points over the curved surface of the body. Distances were measured using a flexible ruler applied over the skin surface. For the abdominal area, at least three measurements were taken between three different points and average linear contraction was calculated (Fig. 4).

Pre- and postoperative photography, weights, and circumferential reduction data were obtained on all patients. One RFAL study patient had a biopsy of the thermally treated skin 12 months after the procedure during which epidermal skin temperatures of 40°C had been attained and there was an area contraction of 43% at 6 months.

The adipose tissue with septal and reticular collagen behavior is shown in Fig. 5. The experiments showed that the marker movement (contraction) started within 2 s after the start of RF energy delivery. Tissue contraction was not symmetrical as the displacement from one side was 8 mm and from the other side the average displacement was 3 mm. Adipose fibrous septal tissue coagulation and vaporization started to be observed at 13 s after the initiation of RF energy. Nonsymmetrical behavior can be explained by the nonuniform structure of connective tissue and the nonsymmetrical geometry of the studied tissue sample. The average marker migration and tissue contraction for the three experiments with adipose tissue was 6.5 mm.

Figure 6 shows thermal images of the same sample taken before the treatment, at the beginning of tissue displacement, and at the end of the treatment showing the rise in thermal profile with time and onset of contraction. For fascial tissue, contraction started when the maximal adipose tissue temperature near the active internal electrode reached 69.4°C. Adipose fibrous septal tissue coagulation and vaporization started when tissue temperature reached 90-100°C and is most probably associated with boiling of adipocyte water content.

Fascia contraction is demonstrated in Fig. 7. The displacement of the markers and tissue contraction in fascia were significantly less than in adipose tissue. The average movement was 2.75 mm or approximately 2.5 times less than the mark migration and tissue contraction observed in adipose tissue. The marker migration and medial contraction started after 3.5 s and maximal temperature near the active electrode at this moment was 61.5°C.

Skin behavior is presented in Fig. 8. The migration of markers and medial displacement and tissue contraction on the skin were similar to the fascia. The average movement was 2.0 mm or approximately 3 times less than the marker migration and contraction observed in adipose tissue. The medial marker movement started after 2.5 s and the maximal temperature near the active electrode during this contraction was 81.9°C.

Table 1 summarizes the results on subcutaneous tissue contraction. From the results one can see that the strongest contraction response was observed in adipose tissue containing septal connective tissue and reticular collagen fibers encasing fat cells. The contraction temperature threshold was the highest for dermis. It is clear that the immediate contraction of dermal collagen is not possible to achieve without a skin burn, which happened when the epidermal temperature exceeded 45°C [13]. Fascia and septa can be heated to these high, optimal contraction temperatures, but it can be done only in a minimally invasive transcutaneous manner that deposits the thermal RF energy directly into the adipose tissue and subdermal space, thus avoiding heating the epidermal surfaces.

The contraction temperatures of collagen in our ex vivo study were in the same range reported for other collagenous tissues. We observed tissue contraction in the area with a diameter of 2 cm, which corresponds to a spherical contraction volume of 4.2 cm³. Knowing the tissue volume and deposited energy before the start of contraction, we can estimate the energy density required for each cubic centimeter of treated tissue to reach tissue contraction effects. We can calculate that for 1 L of adipose tissue up to 48.3 kJ is required to start to see immediate and significant collagen contraction. These calculations of tissue energy needed to initiate adipose contraction are consistent with empirical data obtained with LAL treatment where energy from 50 up to 100 kJ is recommended for treatment of the abdominal area.

In vivo clinical monitoring of temperature in the adipose tissue and on the epidermal surface should allow the physician to predict more accurately the thermal treatment times and reduce the risk of thermal injuries.

The skin biopsies taken from an RFAL study patient at 12 months show normal dermal architecture with healthy collagen (Fig. 9) and elastin fibers (Fig. 10) in the deep reticular dermis and no evidence of scar tissue or abnormal collagen fibers. All RFAL patients demonstrated some level of contraction. From 8 to 15% linear tightening was observed at the end of the surgery on the operating table. It then increased dramatically during the first week when most of the swelling was reduced. The linear and area contraction process continued for weeks and maximum contraction was noted at the last follow-up visit 24 weeks after the treatment.

Linear contraction observed at 6 months follow-up was much more significant than reported with any other technology and varied from 12.7 up to 47% depending on patient and treatment variables. It is important to note that soft tissue area contraction can be calculated as the square of the linear contraction and represents much higher numbers. The measured linear contraction was then correlated with three parameters: (1) aspirated volume that ranged from 0.5 to 3.4 L, with an average volume of 2.0 L, (2) BMI that varied from 20.8 to 31.7, with an average index of 25.7, and (3) deposed RF energy that varied from 60 to 96 kJ per abdominal area, with an average RF energy of 72 kJ.

For statistical analysis of the correlation between the measured variables and linear contraction, the Pearson product moment correlation coefficients were calculated. The closer the coefficient is to 1, the higher the linear correlation between the measured variable and tissue contraction. Analysis shows no or very weak correlation between aspirated volume and linear skin contraction. The Pearson coefficient is about 0.22. Figure 11 shows the correlation between these values and has a random distribution. The Pearson coefficient for correlation between contraction and patient BMI is much higher and equal to 0.64. Figure 12 demonstrates a much stronger connection between these parameters and it is easy to understand that a patient with a larger volume of adipose tissue would have more tissue available to undergo contraction.

The highest correlation (0.86) was obtained between deposed RF energy and skin contraction. Figure 13 shows measurement results that have an almost linear function between these two parameters. The more energy deposited, the more linear contraction that was observed. In spite of improved contraction obtained at higher energies, the amount of energy used during treatment can and should be measured and controlled to avoid side effects such as seroma and skin burn and still achieve optimal linear and area contraction.

Features of an ideal liposuction procedure would include reduced ecchymosis, pain, and edema from preaspiration coagulation of adipose and vascular tissue, followed by less forceful and traumatic extraction forces, as well as significant soft tissue contraction when host tissue elasticity is compromised. Thermal-based lipoplasty appears to hold this potential.

In the present study based on volumetric heating, we reached an average local linear contraction of 31% that is statistically significantly higher than that reported with other energy-emitting liposuction technologies. Overall area contraction was much higher than linear contraction. We believe that these in vivo results confirm our proposed mechanism of RF-based tissue tightening and recruitment of the vertical and oblique fibrous adipose matrix. Our biopsy at 7 months suggests that the papillary and reticular dermis is populated with normal collagen and elastin that have been stimulated and remodeled by subnecrotic subdermal RFAL temperatures.

About 30% of patients noted minor weight loss but it is premature to correlate it with the treatment procedure.

The in vitro experiments produced different degrees of contraction for septal and dermal tissues which emphasizes the balance between these processes for optimal aesthetic results. Lower two-dimensional contraction of the skin and significant three-dimensional contraction of subdermal adipose connective tissue may cause wrinkling of the skin surface in high-volume liposuction patients.

During this study we had one case of a seroma that was treated with closed serial aspiration. Seroma is not a rare side effect for energy-assisted liposuction, especially for high-volume treatment and may necessitate a lower threshold for closed drainage systems in selected patients.