Editorial Type:
Article Category: Research Article
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Online Publication Date: 01 Mar 2007

Biomechanical Analysis of Maxillary Expansion in CLP Patients

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Page Range: 280 – 287
DOI: 10.2319/0003-3219(2007)077[0280:BAOMEI]2.0.CO;2
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Abstract

Objective: To carry out a comparative biomechanical analysis of maxillary low force expansion using the quadhelix appliance in cleft and noncleft patients. We also intended to determine whether a sufficient transverse skeletal effect could be achieved among cleft patients using the quadhelix appliance.

Materials and Methods: Three finite element models of the viscerocranium and neurocranium were established in which a transverse expansion of the maxilla using a quadhelix (transverse force of 2 N) was simulated.

Results: The skeletal effects at the anatomic structures of the midface and the cranial base were far more marked in the simulation models with clefts compared to the morphologically normal state. The highest expansions were measured for bilateral cleft palates. Thus, the expansion measured at the supraorbital margin was 4.7 μstrain with a bilateral cleft, 2.1 μstrain with a unilateral cleft, and only 0.2 μstrain with the morphologically normal state. For bilateral and also for unilateral bone clefts, the skeletal effect of a maxillary low force expansion with a quadhelix on the anatomical structures of the viscerocranium and neurocranium is very much larger than is the case for individuals without clefts.

Conclusion: In the presence of a continuous cleft in the jaw and palate area, orthodontic forces (quadhelix) are apparently already sufficient to allow a skeletal expansion of the maxilla. Maxillary expansion using the quadhelix appliance represents a reasonable alternative to using conventional rapid maxillary expansion appliances among cleft patients.

INTRODUCTION

The objective of a maxillary expansion is to bring about a transverse skeletal expansion of the maxilla,1 while avoiding any dental side effects wherever possible.2 In order to achieve this skeletal effect, the use of a stable maxillary expansion appliance is necessary for patients who do not suffer from clefts in the jaw and palate area.13 This special equipment should be able to produce high forces of up to 120 N4–7 in order to create an opening of the median palatal suture and a lateral bending of the maxillary structures. Unlike the situation with noncleft individuals, skeletal stability in the transverse direction is reduced8 in cleft palate patients because of the special anatomical situation in the jaw and palate area, which can even lead occasionally to a collapse of lateral segments in the medial direction.8–12

With cleft palate patients, an indication for a transverse maxillary expansion often exists because the maxilla is excessively narrow.810–13 Unlike noncleft patients, the necessary skeletal widening of the maxilla with cleft patients is not carried out, according to some authors, using a conventional rapid maxillary expansion appliance, but rather using a quadhelix apparatus10–13 that is only able to generate orthodontic14 transverse forces up to 5 N. According to Reitan,14 forces in this area are well able to induce a dental effect, but for a skeletal effect, higher orthopedic forces14 that should be greater than 5 N are required. Biomechanical studies on the special anatomical situation with cleft patients have not been published in the literature up until now, and expansions induced by quadhelix therapy in the skeletal structures of the viscerocranium and neurocranium also remain unexplained.

The goal of the present study was therefore to carry out a comparative biomechanical analysis of maxillary low force expansion and quadhelix apparatus-induced expansion among cleft and noncleft individuals using a finite element method (FEM). Another goal was to clarify how effective the skeletal effect of the quadhelix appliance is among patients with a cleft jaw and palate and whether the quadhelix appliance represents a reasonable alternative to using conventional rapid maxillary expansion equipment among cleft patients.

MATERIALS AND METHODS

For carrying out comparative simulations, three finite element models of the viscerocranium and neurocranium were generated (Figure 1). The first simulation model revealed no clefts in the jaw or palate area, the second featured a bilateral cleft, and the third featured a unilateral cleft formation on the left side (Figure 1).

Figure 1. Finite element model (a) without a bone cleft, (b) with a bilateral bone cleft, and (c) with a unilateral left-sided bone cleftFigure 1. Finite element model (a) without a bone cleft, (b) with a bilateral bone cleft, and (c) with a unilateral left-sided bone cleftFigure 1. Finite element model (a) without a bone cleft, (b) with a bilateral bone cleft, and (c) with a unilateral left-sided bone cleft
Figure 1. Finite element model (a) without a bone cleft, (b) with a bilateral bone cleft, and (c) with a unilateral left-sided bone cleft

Citation: The Angle Orthodontist 77, 2; 10.2319/0003-3219(2007)077[0280:BAOMEI]2.0.CO;2

All three finite elements models were derived from the skull of a 20-year-old male adult that was available as a precise anatomic plastic model (Somso, Coburg, Germany). The surface of this anatomic skull model was digitalized using a three-dimensional scanner supplied by Minolta (Langenhagen, Germany), cleaned of irregular surfaces using Rapidform™ software (Inus Technology Inc, Seoul, South Korea), matched, smoothed, and then transferred into a virtual computer aided design (CAD) model consisting of bilinear non-uniform rational B-spline (NURBS) patches. The course of the bony clefts was modeled afterwards in the area of the jaw and the palate interactively, just as the inner part of the maxillary sinus was.

For applying the transversely acting forces of the quadhelix, the first upper molars were considered in the simulation model (Figure 1). The anatomic model variants generated by this procedure were imported into Design Space™ (Ansys Inc, Canonsburg, Pa) software, where they were cross-linked three-dimensionally to form a finite element model, only with parabolic tetrahedral elements being employed. The topology of element SOLID 187 was tetrahedral, with 4 nodes at each corner, 6 lines between the corners, and 6 nodes that halved each line, so each tetrahedral element consisted of 10 nodes. SOLID 187 had a quadratic displacement behavior and was well suited to modeling irregular meshes. The simulations could then be carried out after assignment of the material properties and thresholds (Table 1).

Table 1. Properties of Experimental Parameters

          Table 1.

For all comparative calculations, an orthodontic transverse force of 2 N was applied to each palatal side of the first upper molars, which corresponded to the force delivered by a moderately activated quadhelix apparatus. Except for the anatomical cleft form, all experimental conditions were kept constant with all calculations (Table 1). After completion of the calculations, the comparative expansions appearing (in μstrain) were recorded in tabular form and the relationships between the expansions for the individual cleft forms were visualized in diagrammatic form with Design Space software using an interactive tool at previously defined anatomical points of the midface and cranial base (Table 2). The distribution of the expansions above the anatomical structures of the viscerocranium and neurocranium could be represented in all three dimensions using false-color coding (Figures 2 through 4) and comparably with one another for the individual cleft forms.

Table 2. Measured Strains at the Anatomical Structures of the Midface and the Cranial Base in Simulation Models With a Bilateral Cleft, a Unilateral Cleft, and No Cleft

          Table 2.
Figure 2. Level and distribution of the measured expansions after a 2-N transverse loading of the simulation model without a bone cleftFigure 2. Level and distribution of the measured expansions after a 2-N transverse loading of the simulation model without a bone cleftFigure 2. Level and distribution of the measured expansions after a 2-N transverse loading of the simulation model without a bone cleft
Figure 2. Level and distribution of the measured expansions after a 2-N transverse loading of the simulation model without a bone cleft

Citation: The Angle Orthodontist 77, 2; 10.2319/0003-3219(2007)077[0280:BAOMEI]2.0.CO;2

RESULTS

The smallest expansions for all the measurement points in the midface were measured with the simulation model featuring no cleft. The differences in measurements between the cleft and noncleft models were almost considerable (Table 2). At the nasofrontal suture, the measured expansion in the noncleft model was 0.3 μstrain (Figures 2 and 5), whereas in the model with bilateral cleft formation the value at 8.2 μstrain was 27-fold higher (Figures 3 and 5). For the simulation model with a unilateral cleft, the measured expansions (Figures 4 and 5) at the nasofrontal suture were 4.0 μstrain (cleft side) and 3.7 μstrain (healthy side). At the supraorbital margin (Figure 6) the expansion in the simulation model without cleft formation was 0.2 μstrain, whereas in the models with cleft formation it was 4.7 μstrain (bilateral), 2.1 μstrain (unilateral, cleft side) and 2.1 μstrain (unilateral, healthy side).

Figure 5. Expansions measured at different structures of the midface with simulation of maxillary expansion without a bone cleft, with a bilateral bone cleft, and with a unilateral bone cleftFigure 5. Expansions measured at different structures of the midface with simulation of maxillary expansion without a bone cleft, with a bilateral bone cleft, and with a unilateral bone cleftFigure 5. Expansions measured at different structures of the midface with simulation of maxillary expansion without a bone cleft, with a bilateral bone cleft, and with a unilateral bone cleft
Figure 5. Expansions measured at different structures of the midface with simulation of maxillary expansion without a bone cleft, with a bilateral bone cleft, and with a unilateral bone cleft

Citation: The Angle Orthodontist 77, 2; 10.2319/0003-3219(2007)077[0280:BAOMEI]2.0.CO;2

Figure 3. Level and distribution of the measured expansions after a 2-N transverse loading of the simulation model with a bilateral bone cleftFigure 3. Level and distribution of the measured expansions after a 2-N transverse loading of the simulation model with a bilateral bone cleftFigure 3. Level and distribution of the measured expansions after a 2-N transverse loading of the simulation model with a bilateral bone cleft
Figure 3. Level and distribution of the measured expansions after a 2-N transverse loading of the simulation model with a bilateral bone cleft

Citation: The Angle Orthodontist 77, 2; 10.2319/0003-3219(2007)077[0280:BAOMEI]2.0.CO;2

Figure 4. Level and distribution of the measured expansions after a 2-N transverse loading of the simulation model with a left-sided unilateral bone cleftFigure 4. Level and distribution of the measured expansions after a 2-N transverse loading of the simulation model with a left-sided unilateral bone cleftFigure 4. Level and distribution of the measured expansions after a 2-N transverse loading of the simulation model with a left-sided unilateral bone cleft
Figure 4. Level and distribution of the measured expansions after a 2-N transverse loading of the simulation model with a left-sided unilateral bone cleft

Citation: The Angle Orthodontist 77, 2; 10.2319/0003-3219(2007)077[0280:BAOMEI]2.0.CO;2

Figure 6. Expansions measured at different structures of the cranial base with simulation of maxillary expansion without a bone cleft, with a bilateral bone cleft, and with a unilateral bone cleftFigure 6. Expansions measured at different structures of the cranial base with simulation of maxillary expansion without a bone cleft, with a bilateral bone cleft, and with a unilateral bone cleftFigure 6. Expansions measured at different structures of the cranial base with simulation of maxillary expansion without a bone cleft, with a bilateral bone cleft, and with a unilateral bone cleft
Figure 6. Expansions measured at different structures of the cranial base with simulation of maxillary expansion without a bone cleft, with a bilateral bone cleft, and with a unilateral bone cleft

Citation: The Angle Orthodontist 77, 2; 10.2319/0003-3219(2007)077[0280:BAOMEI]2.0.CO;2

However, at the measurement points in the infraorbital margin and the zygomaticoalveolar crest, the differences between cleft and noncleft models were clearly smaller (Figure 5). Thus, at the zygomaticoalveolar crest in the finite element model without cleft formation, 5.2 μstrain was measured, whereas for the model with a bilateral cleft the measurement was 7.6 μstrain, and with the unilateral cleft it was 7.0 μstrain (cleft side) and 6.4 μstrain (healthy side). The differences at the zygomaticofrontal suture between the noncleft and the cleft models, however, were once again distinct. The highest expansions in the midface were always registered in the simulation model with bilateral cleft jaw and palate (Table 2). In the unilateral cleft model, however, expansions were lower than those measured with the bilateral cleft (Table 2), but usually higher than those in the model without cleft formation. In the simulation model with the left-sided cleft, there were usually slightly higher expansions on the cleft side than was the case on the side that was not clefted (Figure 5). The picture with the anatomical structures of the cranial base was similar to that seen with the midface. Here as well, the lowest expansions were measured in the simulation model without clefting (Table 2; Figure 6). Examples included the optic foramen, the superior orbital fissure, and the oval foramen (Figures 2 and 6). Unlike the midface, the maximum values at the structures of the cranial base occurred both with the bilateral cleft model and with the unilateral cleft model (Figure 6). For almost all measurement points at the cranial base, the expansion on the cleft side was only slightly higher than the value measured on the nonaffected side (Table 2; Figure 6).

DISCUSSION

The FEM is a well-proven mathematical instrument for studying orthodontic problems.15–17 The simulation models used in this case represent a simplified idealization of reality. The more differentiated and the more extensive the finite element model, the more precise and more realistic are the simulation results.

The geometric precision of depiction for the simulation models of the facial skull has been improved increasingly over the last years. Whereas in 1994 with Miyasaka-Hiraga et al18 the finite elements model of the skull consisted of 1776 single elements, the model of Iseri et al16 in 1998, which consisted of 2349 individual elements, was already more differentiated. The geometric precision increased further in the paper of Jafari et al17 who introduced a simulation model of the skull with 6951 elements in 2003. Compared to the FEM models of the skull available up until now, the degree of anatomic differentiation was considerably improved in this paper, so that even finely-detailed anatomical structures, such as the foramina of the cranial base, could be considered in the mathematical model.

The simulation models of the facial skull and the cranial base used in the present paper consisted of approximately 30,000 individual elements with approximately 50,000 nodes (Table 1). Despite this relatively differentiated illustration of the complex skull geometry, the present results allow only basic statements to be made about the different expansions upon transverse enlargement of the maxilla, because this still represents merely an artificial simulation model. Only simplified material properties that were based upon averaged values and taken from the literature18–20 were used.

Maxillary expansion using the quadhelix apparatus is usually carried out only in mixed dentition,10–12 ie, at a time point when individual morphology greatly varies depending on the skeletal age of the patient.21 In order to eliminate this age-dependent variability as a distorting factor in the simulations, all measurements were carried out in the present study on a simulation model of a 20-year-old adult, because the variability of the anatomical structures is smaller at this age than it is during the mixed dentition phase. The systematic error arising from this, however, must be considered when interpreting the results.

Future simulation studies should endeavor to compute the distribution of expansions for different individual and age-dependent anatomic states. The present simulations clearly showed that if a cleft jaw and palate are not present, the maxillary expansion with the quadhelix apparatus cannot achieve a relevant skeletal effect at the more remote structures of the midface and the cranial base (Table 2; Figures 5 and 6). One must therefore assume that this treatment is only locally effective and leads only to a dental and not to a skeletal effect. However, the situation in which a cleft is present in the bone area of the jaw and hard palate is different. If orthodontic forces are applied using the quadhelix apparatus, skeletal effects do also arise at remote structures in the midface and the cranial base (Table 2; Figures 5 and 6). The calculations allow us to conclude that among patients with a unilateral or bilateral cleft, the use of a quadhelix appliance leads not only to a dental, but also to a skeletal effect.

The results reported here therefore represent an experimental confirmation of the clinical studies of Tindlund and Rygh10–12 and Rygh and Tindlund.13 Both authors were able to show the good clinical efficiency of the quadhelix apparatus in several papers studying maxillary expansion among cleft patients.10–13 In place of the quadhelix appliance, our results suggest that other equipment can also be used to generate moderate transverse forces in cleft patients. Alternatives to the quadhelix apparatus include, for example, the compound palatal arch22 and the modified maxillary expansion apparatus that only produces moderate forces upon activation of a special nickel-titanium expansion screw.23 According to the present results, the use of a rapid maxillary expansion appliance with forces of 120 N457 is not necessary among cleft patients because orthodontic forces of below 5 N already suffice to achieve a skeletal effect in the midface and the cranial base.

CONCLUSIONS

  • In the presence of a continuous cleft in the jaw and palate area, orthodontic forces (quadhelix) already suffice to bring about a skeletal widening of the maxilla.

  • Maxillary expansion using the quadhelix appliance therefore represents a reasonable alternative to using conventional rapid maxillary expansion appliances among cleft patients.

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Copyright: Edward H. Angle Society of Orthodontists
<bold>Figure 1.</bold>
Figure 1.

Finite element model (a) without a bone cleft, (b) with a bilateral bone cleft, and (c) with a unilateral left-sided bone cleft


<bold>Figure 2.</bold>
Figure 2.

Level and distribution of the measured expansions after a 2-N transverse loading of the simulation model without a bone cleft


<bold>Figure 5.</bold>
Figure 5.

Expansions measured at different structures of the midface with simulation of maxillary expansion without a bone cleft, with a bilateral bone cleft, and with a unilateral bone cleft


<bold>Figure 3.</bold>
Figure 3.

Level and distribution of the measured expansions after a 2-N transverse loading of the simulation model with a bilateral bone cleft


<bold>Figure 4.</bold>
Figure 4.

Level and distribution of the measured expansions after a 2-N transverse loading of the simulation model with a left-sided unilateral bone cleft


<bold>Figure 6.</bold>
Figure 6.

Expansions measured at different structures of the cranial base with simulation of maxillary expansion without a bone cleft, with a bilateral bone cleft, and with a unilateral bone cleft


Contributor Notes

Corresponding author: Dr Christof Holberg, Department of Orthodontics, University of Munich, Goethestrasse 70, Munich, Bavaria 80336, Germany (christof.holberg@med.uni-muenchen.)

Accepted: 01 May 2006
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