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Original Article  |  Open Access  |  21 Mar 2017

Pressures secondary to circumferential digital dressings in clay models

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Plast Aesthet Res 2017;4:41-8.
10.20517/2347-9264.2016.94 |  © 2017 OAE Publishing Inc.
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Abstract

Aim: With little manipulation, compression bandages placed circumferentially around the digit can be rolled up the digit, creating a tourniquet effect. The aim of this study was to elucidate the pressures induced by self-adherent bandages applied circumferentially around the fingers.

Methods: After fabricating various clay finger models using the live finger as a model, the pressure of each self-adherent bandage was measured at the level of the proximal phalanx. Two different self-adherent bandages were applied with variables of different levels of tightness, number of wraps, and whether each was rolled up or not. Pressure was measured using a digital measuring device at a standardized location.

Results: The measured pressure of 3 wraps along the adult finger model was higher than 1 wrap or 2 wraps, and untightened bandages had lower pressures than those of tightened bandages. The pressures of the unrolled bandages were lower than those of rolled up bandages, and pressures along the live finger of the rolled up group were higher than those in the adult finger model. Additionally, measured pressures from the child finger model were higher than those from the adult model.

Conclusion: Precautions should be taken to prevent rolling up dressing materials, especially in children.

Keywords

Pressure, fingers, compression bandages, occlusive dressings

Introduction

The hands and fingers are common sites of injury, accounting for an estimated 4.8 million injured persons treated in US hospital emergency departments in 2001 alone. Three million of these injuries involved one or more fingers, of which 1.3 million (44%) were diagnosed as finger lacerations.[1] To minimize the morbidity associated with these injuries, digital tourniquets are necessary to provide a bloodless environment to facilitate the identification of deep tissue injuries and foreign bodies.[2] After the repair of hand lacerations, the wound dressing is usually covered with compression bandages that are applied circumferentially around the digit. Often, dependable tapes are used. However, with very little manipulation, these bandages can be lifted and rolled up the digit distally, creating a tourniquet effect. Vascular insufficiency from an occlusive dressing is an iatrogenic and avoidable complication, and therefore circumferential digital dressings should be applied correctly.[3]

To prevent the dressing from rolling up and creating a tourniquet effect, Hart et al.[4] suggested that the dressing should be brought down from the finger, to include the hand and wrist. Despite the importance of preventing finger necrosis,[5,6] the pressures generated by circumferential dressings have not yet been studied. The aim of this study was to elucidate the pressures occurring secondary to self-adherent bandages applied circumferentially around the fingers.

Methods

Making a clay finger model

With clay, finger models of 7 cm (adult) and 4 cm (child) in circumference at the level of the proximal phalanx level were made. Biscuit firing was performed. The pressure of each self-adherent bandage was measured using live adult finger models (7 cm circumference). A 6 cm width Peha-haft (Hartmann USA, Inc, Rock hill, SC) and a Coban (3M Co, St. Paul, MN) were used as self-adherent bandages. Experiments were performed with the following variable for each model: dressing materials, wraps, tightness and roll-up states.

Applying methods

According to the length

The pressures were measured according to the total length of the elastic dressings:

1C: elastic dressing was wound 1 lap around a finger model with the same length as its circumference (7 cm).

2C: elastic dressing was wound 2 laps around a finger model with 2 times the length of its circumference (14 cm).

3C: eastic dressing was wound 3 laps around a finger model with 3 times the length of its circumference (21 cm).

According to the tightness

The pressures were measured according to the tightness of the elastic dressings:

T0: 0% tightened.

T1: 9.4% tightened.

T2: 19.7% tightened.

T3: 33.3% tightened.

T4: 50.5% tightened.

Adult finger model

In the adult finger model, the pressures were measured according to the total length of the bandages without tightening, different tightness using 2 wraps, roll-up states and different dressing materials. According to the total length of the bandages without tightening, the self-adherent bandage was wound 1 (1C-T0), 2 (2C-T0), or 3 times (3C-T0) around the finger model with 1 (7 cm), 2 (14 cm), or 3 (21 cm) times the length of its circumference. For the different tightness, the self-adherent bandage was wound employing 2 wraps around the finger model with twice (14 cm, 0% tightened, 2C-T0) the length of its circumference, 91.4% (12.8 cm, 9.4% tightened, 2C-T1), 83.6% (11.7 cm, 19.7% tightened, 2C-T2), 75% (10.5 cm, 33.3% tightened, 2C-T3), or at 66.4% (9.3 cm, 50.5% tightened, 2C-T4) the length of its circumference [Figure 1]. The pressures were measured in both unrolled (NR) and rolled up (R) states. The width of the rolled up portion of the bandage was 6 cm. Pressures were also measured according to the dressing materials, Peha-haft (Ph) or Coban (Co).

Pressures secondary to circumferential digital dressings in clay models

Figure 1. Size of the self-adherent bandages for different tightness

Child finger model

In the child finger model, the same experiments as with adult finger model were done except the different tightness using two wraps. The width of the rolled up portion of the bandage was three cm.

Live adult finger

In the live adult finger, the same experiments as with child finger model were repeated. The width of the rolled up portion of the bandage was six cm.

Measurements using a pressure sensor

Pressures were measured using a FlexiForce B201-M pressure sensor, ELFTM system (Tekscan, Inc., South Boston, MA), which is a flexible, wafer thin (0.005”) 10 mm diameter disk-shaped sensor designed specifically to measure the force between 2 surfaces without disturbing the dynamics of the test.[2] The sensor was placed in a standardized location on the dorsum of each digit equidistant from the metacarpophalangeal and proximal phalangeal joints with the reasoning that the pressures of the dorsal and volar surfaces are the same in a circumferential dressing, and pressure measurements of the dorsum are easier to take in living subjects [Figures 2-4]. The pressure sensor was calibrated to measure pressures in the range of 0 to 4,500 mm of mercury obtained by the Economical Load and Force software program at a refresh rate of 200 Hz. The pressure measurements were made by the same person to prevent bias.

Pressures secondary to circumferential digital dressings in clay models

Figure 2. Making a finger tourniquet and pressure measurements. A: finger model, pressure sensor, and self-adherent bandage; B: the sensor was placed in a standardized location and the bandage was wound two wraps around the finger model; C: the bandage was rolled up along the finger model

Pressures secondary to circumferential digital dressings in clay models

Figure 3. Finger models. A: adult finger model; B: child finger model; C: finger of a living body

Pressures secondary to circumferential digital dressings in clay models

Figure 4. Schematic representation of the location of the pressure sensor (S) and wraps around the finger model (M); B: self-adherent bandage. A: 1 wrap with the same length of its circumference; B: 2 wraps with 2 times the length of its circumference; C: 3 wraps with 3 times the length of its circumference

Statstical analysis

The program SPSS 19.0 (IBM, Armonk, NY) was used for a statistical analysis. For comparison between 2 groups, the independent 2 samples t-test was used. For comparison among more than 3 groups, analysis of variance (ANOVA) was used. When the P value was less than 0.05, the data were interpreted as statistically significant.

Results

Measured pressures were higher in tighter bandages, in rolled-up bandages, with the use of Co, in the live models, and in adults.

According to the length along the adult finger model (1C-T0, 2C-T0, 3C-T0): the measured pressure of 3 wraps (3C-T0, 384.9 ± 660.5 mmHg) was significantly higher than that for 1 wrap (1C-T0, 35.3 ± 37.5 mmHg, P < 0.001), or 2 wraps (2C-T0, 44.1 ± 47.7 mmHg, P < 0.001). However, there was no significant difference between 1 wrap and 2 wraps (P = 0.994) [Figure 5].

Pressures secondary to circumferential digital dressings in clay models

Figure 5. Measured pressures according to the length of the bandage without tightness along the adult finger model. 1CT0: 1 wrap with the same length of its circumference; 2CT0: 2 wraps with 2 times the length of its circumference; 3CT0: 3 wraps with 3 times the length of its circumference. *P < 0.05

According to the tightness of 2 wraps along the adult finger model (2C-T0, 2C-T1, 2C-T2, 2C-T3, 2C-T4): the measured pressures of the untightened bandages (2C-T0, 44.1 ± 47.7 mmHg) were significantly lower than those of the tightened bandages (2C-T1~4, 680.2 ± 1,274.1 mmHg, P < 0.001). The measured pressures of the untightened bandages and each tightened bandage were 44.1 ± 47.7 mmHg (2C-T0, 0%), 61.2 ± 67.4 mmHg (2C-T1, 9.4%), 261.1 ± 409.5 mmHg (2C-T2, 19.7%), 471.2 ± 671.3 mmHg (2C-T3, 33.3%), and 1,945.0 ± 1,945.0 mmHg (2 CT4, 50.5%), respectively. The measured pressures of the 2C-T4 (50% tightened) were significantly higher (P < 0.001) than those in other groups. However, there was no significant difference between the 2C-T0, 2C-T1, 2C-T2, and 2C-T3 parameters (P > 0.05). For each material (Ph and Co), the measured pressures of the untightened bandage (T0-Ph, 34.8 ± 36.6 mmHg), (T0-Co, 53.5 ± 56.1 mmHg) was significantly lower than that of the tightened bandage (T1~T4-Ph, 511.9 ± 1,166.1 mmHg, P < 0.001), (T1~T4-Co, 848.4 ± 1,360.2 mmHg, P < 0.001) [Figure 6].

Pressures secondary to circumferential digital dressings in clay models

Figure 6. Measured pressures according to the tightness in different materials along the adult finger model. T0: untightened bandage; T1~T4: tightened bandages; Ph: Peha-haft; Co: Coban. *P < 0.05

Regarding rolled bandages in the adult finger model (NR, R): the measured pressures of the unrolled bandages (NR, 14.2 ± 25.4 mmHg) were significantly lower than those of the rolled bandages (R, 793.1 ± 1,265.7 mmHg, P < 0.001). In each untightened and tightened bandage (T0-1C~3C), (T1~T4-2C), the measured pressures of the unrolled bandages (T0-1C~3C-NR, 0 ± 0 mmHg), (T1~T4-2C-NR, 28.3 ± 29.9 mmHg), were significantly lower than those for the rolled bandages (T0-1C~3C-R, 309.6 ± 544.0 mmHg, P < 0.001), (T1~T4-2C-R, 1,332.0 ± 1,551.1 mmHg, P < 0.001) [Figure 7].

Pressures secondary to circumferential digital dressings in clay models

Figure 7. Measured pressures according to the rolling up of untightened dressings and tightened dressings along the adult finger model. NR: unrolled; R: rolled up; T0-1C~3C: untightened bandages; T1~T4-2C: tightened bandages. *P < 0.05

Regarding rolls of bandages at various lengths along the adult finger model (NR, R in 1C-T0, 2C-T0, 3C-T0): in each wrap (1C-T0, 2C-T0, 3C-T0), the measured pressures of the unrolled bandages (1C-T0-NR, 0 ± 0 mmHg), (2C-T0-NR, 0 ± 0 mmHg), (3C-T0-NR, 0 ± 0 mmHg) were significantly lower than those of the rolled bandages (1C-T0-R, 70.7 ± 15.9 mmHg, P < 0.001), (2C-T0-R, 88.2 ± 24.0 mmHg, P < 0.001), (3C-T0-R, 769.8 ± 764.0 mmHg, P < 0.001). In the above situations, the same results were yielded for each material (Ph, Co) [Table 1].

Table 1

Measured pressures according to the length of different dressing materials and in a rolled up state in the adult finger model (mean ± SD)

GroupNRRP value
1C-T0-Ph0.0 ± 0.057.9 ± 7.2< 0.001
2C-T0-Ph0.0 ± 0.069.5 ± 12.1< 0.001
3C-T0-Ph0.0 ± 0.0114.1 ± 34.0< 0.001
1C-T0-Co0.0 ± 0.083.5 ± 10.6< 0.001
2C-T0-Co0.0 ± 0.0107.0 ± 17.0< 0.001
3C-T0-Co0.0 ± 0.01,425.6 ± 524.9< 0.001

Regarding various levels of tightness along the adult finger model (NR, R in 2C-T0, 2C-T1, 2C-T2, 2C-T3, 2C-T4): at each tightness level, bandages of the 2 C group (2C-T0, 2C-T1, 2C-T2, 2C-T3, 2C-T4), measured pressures of the not-rolled up bandage (2C-T0-NR, 0 ± 0 mmHg), (2C-T1-NR, 0 ± 0 mmHg), (2C-T2-NR, 24.8 ± 25.4 mmHg), (2C-T3-NR, 24.76 ± 25.4 mmHg), (2C-T4-NR, 63.9 ± 14.7 mmHg) were significantly lower than those for the rolled up bandage (2C-T0-R, 88.2 ± 24.0 mmHg, P < 0.001), (2C-T1-R, 122.4 ± 37.9 mmHg, P < 0.001), (2C-T2-R, 497.5 ± 475.3 mmHg, P < 0.001), (2C-T3-R, 917.7 ± 710.4 mmHg, P < 0.001), (2C-T4-R, 3,790.4 ± 675.2 mmHg, P < 0.001). In the above situations, the same results were shown for each material (Ph, Co) [Table 2].

Table 2

Measured pressures according to the tightness of different dressing materials and rolled up state in the adult finger model (mean ± SD)

GroupNRRP value
2C-T0-Ph0.0 ± 0.069.5 ± 12.1< 0.001
2C-T1-Ph0.0 ± 0.087.9 ± 17.3< 0.001
2C-T2-Ph0.0 ± 0.0112.5 ± 13.7< 0.001
2C-T3-Ph0.0 ± 0.0370.6 ± 156.7< 0.001
2C-T4-Ph49.5 ± 0.03,475 ± 803.3< 0.001
2C-T0-Co0.0 ± 0.0107 ± 17.0< 0.001
2C-T1-Co0.0 ± 0.0156.9 ± 9.4< 0.001
2C-T2-Co49.5 ± 0.0882.5 ± 383.7< 0.001
2C-T3-Co49.5 ± 0.01,464.8 ± 613.0< 0.001
2C-T4-Co78.2 ± 0.04,105.8 ± 309.6< 0.001

Rolling up of different dressing materials along the adult finger model (NR, R in Ph, Co): for the Ph, the measured pressures of the unrolled elastic dressing (Ph-NR, 7.1 ± 17.5 mmHg) were significantly lower than those for the rolled up elastic dressing (Ph-R, 612.5 ± 1,217.8 mmHg, P < 0.001). For the Co, the measured pressures of the unrolled elastic dressing (Co-NR, 25.3 ± 30.8 mmHg) were significantly lower than those for the rolled up elastic dressing (Co-R, 1,175.2 ± 1,372.4 mmHg, P < 0.001) [Figure 8].

Pressures secondary to circumferential digital dressings in clay models

Figure 8. Measured pressures according to the rolling up of the Peha-haft (Ph) and Coban (Co) along the adult finger model. NR: unrolled; R: rolled up. *P < 0.05

According to the dressing materials along the adult finger model (Ph, Co): the measured pressures of Ph (Ph, 309.8 ± 910.3 mmHg) were significantly lower than those for Co (Co, 600.2 ± 1,126.2 mmHg, P = 0.018). In the unrolled group (NR), the measured pressures of the Ph (UR-Ph, 7.1 ± 17.5 mmHg) were significantly lower than those for Co (UR-Co, 25.3 ± 30.8 mmHg, P < 0.001). In the rolled up group (R), the measured pressures of the Ph (R-Ph, 612.5 ± 1,217.8 mmHg) were significantly lower than those for Co (R-Co, 1,175.2 ± 1,372.4 mmHg, P = 0.011) [Figure 9]. In the untightened bandages (T0-1C~3C), the measured pressures of the Ph (T0-1C~3C-Ph, 40.2 ± 46.4 mmHg) were significantly lower than those for Co (T0-1C~3C-Co, 269.3 ± 562.0 mmHg, P = 0.002). In the tightened dressings (T1~T4-2C), the measured pressures of the Ph (T1~T4-2C-Ph, 511.9 ± 1,166.1 mmHg) and Co (T1~T4-2C-Co, 848.4 ± 1,360.2 mmHg) were not significantly different (P = 0.095). In 1 and 2 wraps (1C-T0, 2C-T0), the measured pressures of the Ph (1C-T0-Ph, 28.9 ± 30.1 mmHg), (2C-T0-Ph, 34.8 ± 36.6 mmHg) and Co (1C-T0-Co, 41.8 ± 43.5 mmHg), (2C-T0-Co, 53.5 ± 56.1 mmHg) were not significantly different (P = 0.285, P = 0.220). However, for 3 wraps (3C-T0), the measured pressures of the Ph (3C-T0-Ph, 57.0 ± 63.0 mmHg) were significantly lower than those for Co (3C-T0-Co, 712.8 ± 815.7 mmHg, P = 0.002). At each different tightness of the bandages of the 2C group, the measured pressures of the Ph and Co were not significantly different except at 19.7% and 33.5% of the tightened bandages of the 2C group. In the 19.7% and 33.5% tightened bandages of the 2C group (2C-T2, 2C-T3), the measured pressures of the Ph (2C-T2-Ph, 56.2 ± 58.5 mmHg), (2C-T3-Ph, 185.3 ± 218.6 mmHg) were significantly lower than those for Co (2C-T2-Co, 466.0 ± 502.3 mmHg, P = 0.002), (2C-T3-Co, 757.2 ± 839.7 mmHg, P = 0.008).

Pressures secondary to circumferential digital dressings in clay models

Figure 9. Measured pressures according to the bandage materials in the unrolled group (NR) and the rolled up group (R) along the adult finger model; Ph: Peha-Haft; Co: Coban. *P < 0.05

Rolling up at different lengths along the child finger model (NR, R in 1C-T0, 2C-T0, 3C-T0): in each wrap using the Ph (1C-T0-Ph, 2C-T0-Ph, 3C-T0-Ph), the measured pressures of the unrolled bandage (1C-T0-Ph-NR, 0 ± 0 mmHg), (2C-T0-Ph-NR, 0 ± 0 mmHg), (3C-T0-Ph-NR, 0 ± 0 mmHg) were significantly lower than those for the rolled up bandage (1C-T0-Ph-R, 210.6 ± 117.0 mmHg, P < 0.001), (2C-T0-Ph-R, 323.7 ± 186.9 mmHg, P < 0.001), (3C-T0-Ph-R, 904.9 ± 462.1 mmHg, P < 0.001) [Table 3].

Table 3

Statistical differences according to rolling up at different lengths in the child finger model (mean ± SD)

GroupNRRP value
1C-T0-Ph0.0 ± 0.0210.6 ± 117.0< 0.001
2C-T0-Ph0.0 ± 0.0323.7 ± 186.9< 0.001
3C-T0-Ph0.0 ± 0.0904.9 ± 462.1< 0.001

Rolling up at different lengths along the live adult finger (NR, R in 1C-T0, 2C-T0, 3C-T0): in each wrap with the Ph (1C-T0-Ph, 2C-T0-Ph, 3C-T0-Ph), the measured pressures of the unrolled bandage (1C-T0-Ph-NR, 0 ± 0 mmHg), (2C-T0-Ph-NR, 0 ± 0 mmHg), (3C-T0-Ph-NR, 0 ± 0 mmHg) were significantly lower than those for rolled up bandage (1C-T0-Ph-R, 277.5 ± 227.5 mmHg, P = 0.004), (2C-T0-Ph-R, 636.2 ± 558.0 mmHg, P = 0.006), (3C-T0-Ph-R, 1,005.6 ± 644.5 mmHg, P = 0.001) [Table 4].

Table 4

Statistical differences according to rolling up at different lengths in the adult finger of a living body (mean ± SD)

GroupNRRP value
1C-T0-Ph0.0 ± 0.0277.5 ± 227.50.004
2C-T0-Ph0.0 ± 0.0636.2 ± 558.00.006
3C-T0-Ph0.0 ± 0.01,005.6 ± 644.50.001

In the rolled up bandage of the untightened group (1C~3C-T0-R), the measured pressures along the adult finger model (1C~3C-T0-R, 80.5 ± 32.1 mmHg) were significantly lower than those in the child finger model (1C~3C-T0-R, 479.7 ± 420.8 mmHg, P < 0.001) and live adult finger (1C~3C-T0-R, 639.7 ± 577.1 mmHg, P < 0.001). In the above situations, the same results were shown for each wrap [Tables 5 and 6].

Table 5

Statistical differences according to rolling up of adult and child finger models (mean ± SD)

GroupABP value
1C-T0-Ph-R57.9 ± 7.2210.6 ± 117.00.003
2C-T0-Ph-R69.5 ± 12.1323.7 ± 186.90.002
3C-T0-Ph-R114.1 ± 34.0904.9 ± 462.10.000
(1C~3C)-T0-Ph-R80.5 ± 32.1479.7 ± 420.8< 0.001
Table 6

Statistical differences according to rolling up of the adult finger model and the live finger (mean ± SD)

GroupACP value
1C-T0-Ph-R57.9 ± 7.2277.5 ± 227.50.014
2C-T0-Ph-R69.5 ± 12.1636.2 ± 558.00.011
3C-T0-Ph-R114.1 ± 34.01,005.6 ± 644.50.002
(1C~3C)-T0-Ph-R80.5 ± 32.1639.7 ± 577.1< 0.001

Discussion

As material is rolled around a digit, it becomes tighter, exsanguinating the fingertip and constricting the digit. This quickly becomes uncomfortable. If this happens to an adult, the patient will likely cut and remove the constricting device. However, children, especially those two years old and under, do not understand this and cannot remove the dressing quickly. A similar lack of understanding or action also may occur in elderly and mentally compromised patients. If the constriction tightens to the point that all vascular flow is impeded into the tip of the digit, hypoxia and eventually tissue necrosis will occur. Thus, a simple, soft tissue injury can become a more serious injury. Although no studies in the literature have reported the incidence of this condition, any physician who has applied a finger dressing knows how easily a circumferentially applied dressing, such as Co, can roll up when manipulated, as when a child plays with a dressing.[4]

Lahham et al.[2] noted that digital tourniquet methods have complications associated with their use. Necrosis of a digit due to a forgotten tourniquet is an uncommon but catastrophic complication.[7-11] Most complications occur with use of the least conspicuous dressings.[12-16] While digital necrosis secondary to a forgotten tourniquet is the most severe complication related to digital tourniquet use, most complications are related to excessive tourniquet pressure.

Co (3 M Co, St. Paul, MN) is a self-adherent bandage made from a porous, non-woven polyester material, with strands of urethane coated with a cohesive substance. Co sticks only to itself and not to the skin, and provides sustained compression.[17] In soft tissue injuries, it is recommended that 30 cm of the Co be unwound and allowed to relax because if applied directly from the roll, the tension will be too great. Mendlowitz[18] reported the mean digital arterial systolic blood pressure in adults to be 100 mmHg, with a pressure range of 84 to 120 mmHg. Based on their experience using digital tourniquets on patients in a clinical setting, Shaw et al.[19] reported pressures of 150 mmHg to be “very adequate” to maintain hemostasis.

Tuncali et al.[20] reported a method for estimation of the arterial occlusion pressure; according to these principles the pressure necessary to prevent digital blood flow ranges from 110 to 140 mmHg. In this study, the average pressures in the rolled and untightened bandage group along the live finger were significantly higher than those for the adult finger model. Therefore, dressing materials are not intended to be rolled up on the finger in the clinical setting. Additionally, measured pressures in the child finger model (479.7 ± 420.8 mmHg, P < 0.001) were significantly higher than those for the adult finger model (80.5 ± 32.1 mmHg). These results support the need for great caution when using rolled bandages in children. The pressures with the use of Co were relatively higher than those for rolled Ph, which is thought to be due to the thickness of the dressing. The thickness of Co (2 mm) is thicker than that of Ph (1 mm) when unrolled, and therefore it becomes much thicker when rolled. Therefore, great caution is needed to prevent rolling of Co dressings.

In the current study, pressures were measured on a clay model as well as human model. In the human model, limb elevation is an important method used for the prevention of post-dressing limb edema. Limb elevation plays a role in the reduction of finger swelling and improving circulation. The same cannot be done in the clay model. Because all data was obtained based on the clay model instead of live fingers, it cannot be claimed that the data mimics the clinical situation perfectly. This is a limitation of this study.

This study was performed to prevent an over-tightening of bandages in fingers and to make the reader aware of the necessity to anchor the bandage above the wrist. In conclusion, when applying pressure dressings to fingers, great caution is needed to prevent rolling-up which can create a tourniquet effect.

Authors’ contributions

Concept design: K. Hwang

Literature search: K. Hwang

Measurement of the pressure: H.J. Kim

Manuscript’s preparation: H.J. Kim, K. Hwang

Manuscript’s review: K. Hwang

This paper is made from the a thesis entitled “The Measurement of the Pressures Applied by Self-adherent Bandages to Prevent the Ischemic Damage of the Fingers” by Han Joon Kim, A THESIS Submitted to the faculty of INHA UNIVERSITY in partial fulfillment of the requirements for the degree of MASTER OF SCIENCE, Aug, 2014.

Financial support and sponsorship

This study was funded by a grant from National Research Foundation of Korea (NRF-2017-005787).

Conflicts of interest

There are no conflicts of interest.

Patient consent

Not applicable.

Ethics approval

All the procedures followed were in accordance with the ethical standards of the responsible committee on human experimentation (institutional or regional) and with the Helsinki Declaration when reporting studies on human beings.

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Kim HJ, Hwang K. Pressures secondary to circumferential digital dressings in clay models. Plast Aesthet Res 2017;4:41-8. http://dx.doi.org/10.20517/2347-9264.2016.94

AMA Style

Kim HJ, Hwang K. Pressures secondary to circumferential digital dressings in clay models. Plastic and Aesthetic Research. 2017; 4: 41-8. http://dx.doi.org/10.20517/2347-9264.2016.94

Chicago/Turabian Style

Kim, Han Joon, Kun Hwang. 2017. "Pressures secondary to circumferential digital dressings in clay models" Plastic and Aesthetic Research. 4: 41-8. http://dx.doi.org/10.20517/2347-9264.2016.94

ACS Style

Kim, HJ.; Hwang K. Pressures secondary to circumferential digital dressings in clay models. Plast. Aesthet. Res. 2017, 4, 41-8. http://dx.doi.org/10.20517/2347-9264.2016.94

About This Article

This is an open access article distributed under the terms of the Creative Commons Attribution-NonCommercial-ShareAlike 3.0 License (http://creativecommons.org/licenses/by-nc-sa/3.0/), which allows others to remix, tweak and build upon the work non-commercially, as long as the author is credited and the new creations are licensed under the identical terms.

Author Biographies

Dr. Kun Hwang is currently a Fellowship Professor, Department of Plastic Surgery, Inha University School of Medicine and Inha University Hospital. More information could be found at: http://orcid.org/0000-0002-1994-2538.

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