Assessment of tooth devitalization as a risk factor for enamel and dentin functional overload using mathematical modeling
- 作者: Olesova E.А.1, Arytyunov S.D.2, Nekrasova E.A.1, Bersanova M.R.1, Olesov E.E.1
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隶属关系:
- State Research Center — Burnasyan Federal Medical Biophysical Center of Federal Medical Biological Agency
- Russian University of Medicine
- 期: 卷 29, 编号 2 (2025)
- 页面: 120-126
- 栏目: Experimental and Theoretical Investigations
- ##submission.dateSubmitted##: 04.02.2025
- ##submission.dateAccepted##: 20.02.2025
- ##submission.datePublished##: 29.04.2025
- URL: https://rjdentistry.com/1728-2802/article/view/653465
- DOI: https://doi.org/10.17816/dent653465
- ID: 653465
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详细
Background: Cracks and fractures of devitalized teeth caused by functional overload are common in dental practice, necessitating an assessment of the stress-strain state of intact and devitalized tooth tissues under similar loading conditions.
Aim: An experimental comparison of the stress-strain state of intact and devitalized hard tooth tissues and the surrounding bone tissue using mathematical modeling.
Methods: A 3D mathematical modeling of the stress-strain state of a mandibular segment with an intact and devitalized tooth was performed. A vertical and oblique (45°) load of 150 N was applied; the maximum stress and its location in the enamel, dentin, cortical bone, and cancellous bone were analyzed by comparing them to the respective strength limits.
Results: Devitalized hard tissues are subjected to a higher stress than intact teeth, especially when an oblique load is applied, by 49.3, 11.0, and 13.1% (86.186, 31.371, and 5.037 MPa) for the enamel, cortical bone, and cancellous bone, respectively. When a vertical load is applied, tooth devitalization increases the stress in the enamel and cancellous bone of the socket by 33.1 and 29.2% (51.147 and 1.953 MPa), respectively. Devitalized dentin shows almost no changes in stress under a vertical load due to the deterioration of physical properties (and, thus, a decrease in the strength limit), whereas an oblique load results in a decrease of 28.1%. Functional load in a devitalized tooth results in stress values close to the strength limit in the enamel (under a vertical and oblique load) and dentin (under an oblique load). Periapical resorption and root apex resection further increase the stress.
Conclusion: Tooth devitalization increases the stress in the enamel and bone tissues, especially under an oblique load. Despite the reduced stress in devitalized dentin caused by a decrease in its mechanical strength, stress values under an oblique load are close to the dentin strength limit in the tooth neck area. Due to tooth devitalization, the stress in the enamel exceeds its strength limit under both oblique and vertical loads (in the tooth neck area and along the occlusal surface, respectively). Periapical resorption and root apex resection cause a similar increase in the stress in the enamel compared to a devitalized tooth under both loads, as well as in the cortical bone under an oblique load.
全文:
Background
Over the long term after root canal treatment, root cracks and fractures are frequently observed under normal masticatory function, indicating reduced dentin strength resulting from changes in its physical and mechanical properties [1–3]. In some cases, this complication can be managed with post-retained restorations. However, restoration of the crown’s integrity does not eliminate the risk of recurrent root fracture.
Therefore, the magnitude and distribution of functional stresses and their relationship to dentin strength in devitalized (nonvital) teeth under functional loading, compared with intact teeth, remain a subject of considerable scientific interest.
Three-dimensional mathematical modeling provides a highly detailed assessment of the stress–strain behavior of dental hard tissues [4–7]. It is essential that such models account for the actual ultimate strength values of dentin and restorative materials. Although the available data on the physical and mechanical properties of dental hard tissues remain limited and sometimes inconsistent, several studies have demonstrated a significant reduction in dentin ultimate strength in devitalized teeth compared with intact teeth, which is critical for accurate interpretation of mathematical modeling outcomes [8, 9].
Aim
This work aimed to experimentally compare the stress–strain behavior of dental hard tissues in intact and devitalized teeth, as well as in the surrounding alveolar bone, using mathematical modeling.
Methods
A baseline three-dimensional mathematical model of a mandibular premolar was constructed, including enamel, dentin, and the surrounding cortical and cancellous bone, preserving their natural anatomical proportions. The model variants included an intact tooth, a devitalized tooth, a tooth with periapical bone resorption, and a tooth after apicoectomy (see Fig. 1).
Fig. 1. Three-dimensional mathematical model of a single-rooted mandibular tooth (premolar) under unfavorable biomechanical conditions: a, intact tooth; b, tooth with periapical bone resorption; c, tooth after apicoectomy.
The mechanical properties of the analyzed tissues and restorative materials were based on published data regarding their elastic modulus, Poisson’s ratio, and ultimate tensile strength, which are lower than the corresponding compressive strength values (see Table 1). For modeling purposes, the ultimate strength of dentin was set at 104 MPa for intact and 30 MPa for devitalized teeth.
Table 1. Mechanical properties of dental hard tissues
Tissue / material | Elastic modulus (E), MPa | Poisson’s ratio | Ultimate tensile strength, MPa |
Enamel | 81 700 | 0.28 | 42.1 |
Dentin | 23 300 | 0.31 | 104 |
Devitalized dentin | 2600 | 0.31 | 30 |
Cortical bone | 20 500 | 0.32 | 150 |
Cancellous bone | 3500 | 0.34 | 15 |
Stress distribution and the magnitude of stresses in the modeled tissues and restorative materials were analyzed under vertical and oblique loading of 150 N using color-coded stress maps and quantitative stress scales in SolidWorks (Dassault Systèmes, France) (see Figs. 2 and 3).
Fig. 2. Functional stress distribution in the tooth and surrounding bone tissue under vertical loading in unfavorable biomechanical conditions (devitalized tooth): a, enamel; b, dentin; c, cortical bone; d, cancellous bone.
Fig. 3. Functional stress distribution in the tooth and surrounding bone tissue under oblique loading in unfavorable biomechanical conditions (devitalized tooth): a, enamel; b, dentin; c, cortical bone; d, cancellous bone.
Comparative analysis of stress values across the different modeling variants was performed in Excel 2019 (Microsoft, USA) using Student’s t-test; differences were considered statistically significant at p < 0.05.
Results
Under vertical loading, the highest stresses in the intact tooth and its surrounding alveolar socket were observed in the enamel, reaching 34.204 MPa along the occlusal surface (see Table 2). In dentin, stresses up to 9.174 MPa were recorded above the pulp chamber, beneath the enamel layer of the occlusal surface. In cortical bone, the maximum stresses were distributed along the lower third of the tooth socket and its projection on the mandibular cortical plate (5.066 MPa), whereas in cancellous bone, stresses concentrated near the tooth apex (1.382 MPa).
Table 2. Maximum stress values under functional loading of a devitalized tooth (MPa)
Test object | Intact tooth | Devitalized tooth | Periapical bone resorption | Apicoectomy |
Enamel (v) | 34.204 | 51.147 | 57.360 | 57.360 |
Enamel (o) | 43.705 | 86.186 | 110.489 | 110.505 |
Dentin (v) | 9.174 | 8.622 | 7.971 | 7.971 |
Dentin (o) | 56.469 | 40.625 | 36.792 | 36.790 |
Cortical bone (v) | 5.066 | 4.955 | 5.418 | 5.419 |
Cortical bone (o) | 27.909 | 31.371 | 47.968 | 47.969 |
Cancellous bone (v) | 1.382 | 1.953 | 1.871 | 1.872 |
Cancellous bone (o) | 4.375 | 5.037 | 5.107 | 5.111 |
Note: v, vertical load; o, oblique load.
Oblique loading substantially increased stresses in all hard tissues of the tooth: up to 43.705 MPa in enamel, 56.469 MPa in dentin, 27.909 MPa in cortical bone, and 4.375 MPa in cancellous bone. The areas of maximum stress shifted as follows: along the cervical region in enamel; in the middle third of the root in dentin; in the transition zone between the vertical and basal surfaces of the mandible in cortical bone; and in the cervical portions of the interalveolar septa in cancellous bone.
The hard tissues of the devitalized tooth were exposed to greater stresses than those of the intact tooth, particularly under oblique loading: by 49.3%, 11.0%, and 13.1% (86.186, 31.371, and 5.037 MPa) in the enamel, cortical bone, and cancellous bone, respectively. Under vertical loading, tooth devitalization increased stresses in enamel and cancellous bone by 33.1% and 29.2% (51.147 and 1.953 MPa, respectively). In devitalized dentin, due to the deterioration of its physical properties and consequent reduction of ultimate strength, stresses remained nearly unchanged under vertical loading and decreased by 28.1% under oblique loading.
A clinically common condition, periapical bone resorption, compared with a devitalized tooth without resorption, resulted in increased enamel stress—by 10.8% under vertical and 22.0% under oblique loading (57.360 and 110.489 MPa, respectively)—and in cortical bone under oblique loading by 34.6% (47.968 MPa). Under vertical loading with periapical resorption, stress values in enamel, dentin, cortical bone, and cancellous bone were 57.360, 7.971, 5.418, and 1.871 MPa, respectively. Under oblique loading, the corresponding stresses increased to 110.489, 36.792, 47.968, and 5.107 MPa, respectively.
The mathematical model of a devitalized tooth after apicoectomy showed no significant differences in stress magnitudes in tooth and bone tissues compared with the model featuring periapical resorption. Under vertical loading, maximum stresses in enamel, dentin, cortical bone, and cancellous bone were 57.360, 7.971, 5.419, and 1.872 MPa, respectively; under oblique loading, they were 110.505, 36.790, 47.969, and 5.111 MPa, respectively.
The stress distribution pattern in the devitalized tooth differed from that in the intact tooth only within dentin under vertical loading: stresses persisted in the cervical area but disappeared beneath the enamel layer of the occlusal surface.
Compared with a devitalized tooth, periapical bone resorption altered the stress distribution only in cancellous bone under vertical loading, where stresses were concentrated along the upper boundary of the periapical cavity.
The stress distribution patterns across all analyzed tissues were nearly identical in the models with periapical bone resorption and apicoectomy.
Discussion
Analysis of stress values across the modeled teeth showed that functional loading of a devitalized tooth resulted in enamel stress levels approaching its ultimate strength under both vertical and oblique loading, and in dentin under oblique loading. Periapical bone resorption further increased stress levels. Oblique loading was particularly detrimental to the stress–strain behavior of the tooth and surrounding alveolar bone.
The patterns revealed through mathematical modeling are consistent with clinical observations, confirming the applicability of this method for individualized prediction of the biomechanical consequences of dental interventions affecting the hard tissues of the tooth.
Conclusion
From a biomechanical perspective, tooth devitalization negatively affects the strength of hard dental tissues. Devitalization increases stresses in enamel and bone tissue, particularly under oblique loading. Despite a reduction in dentin stress caused by a decrease in its mechanical strength, the stress values in a devitalized tooth under oblique loading approach the dentin ultimate strength in the cervical region. As a result of tooth devitalization, enamel stresses exceed its ultimate strength under both oblique and vertical loads—at the cervical area and along the occlusal surface, respectively. Periapical bone resorption and apicoectomy similarly increase enamel stress compared with a devitalized tooth under both loading conditions and also raise cortical bone stress under oblique loading.
Additional information
Author contributions: E.A. Olesova: methodology, formal analysis; S.D. Arutyunov: conceptualization, writing—review & editing; E.A. Nekrasova: writing—original draft; M.R. Bersanova: validation, data curation; E.E. Olesov: investigation. All the authors approved the version of the manuscript to be published and agreed to be accountable for all aspects of the work, ensuring that questions related to the accuracy or integrity of any part of the work are appropriately investigated and resolved.
Ethics approval: Not applicable.
Funding sources: No funding.
Disclosure of interests: The authors have no relationships, activities, or interests for the last three years related to for-profit or not-for-profit third parties whose interests may be affected by the content of the article.
Statement of originality: No previously published material (text, images, or data) was used in this work.
Data availability statement: All data generated during this study are available in this article.
Generative AI: No generative artificial intelligence technologies were used to prepare this article.
Provenance and peer-review: This paper was submitted unsolicited and reviewed following the standard procedure. The peer review process involved two external reviewers, a member of the editorial board, and the in-house scientific editor.
作者简介
Emilia Olesova
State Research Center — Burnasyan Federal Medical Biophysical Center of Federal Medical Biological Agency
编辑信件的主要联系方式.
Email: emma.olesova@mail.ru
ORCID iD: 0000-0003-4511-6317
SPIN 代码: 5767-9158
俄罗斯联邦, Moscow
Sergey Arytyunov
Russian University of Medicine
Email: sd.arutyunov@mail.ru
ORCID iD: 0000-0001-6512-8724
SPIN 代码: 1052-4131
MD, Dr. Sci. (Medicine), Professor
俄罗斯联邦, MoscowEkaterina Nekrasova
State Research Center — Burnasyan Federal Medical Biophysical Center of Federal Medical Biological Agency
Email: ekaterina233@mail.ru
ORCID iD: 0000-0003-0380-0575
SPIN 代码: 4291-2151
俄罗斯联邦, Moscow
Makka Bersanova
State Research Center — Burnasyan Federal Medical Biophysical Center of Federal Medical Biological Agency
Email: bersanova99@bk.ru
ORCID iD: 0009-0004-6150-148X
俄罗斯联邦, Moscow
Egor Olesov
State Research Center — Burnasyan Federal Medical Biophysical Center of Federal Medical Biological Agency
Email: olesov_georgiy@mail.ru
ORCID iD: 0000-0001-9165-2554
SPIN 代码: 8924-3520
MD, Dr. Sci. (Medicine), Professor
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