Research article Special Issues

Bifurcation analysis in a singular Beddington-DeAngelis predator-prey model with two delays and nonlinear predator harvesting

  • Received: 26 January 2019 Accepted: 14 March 2019 Published: 26 March 2019
  • In this paper, a differential algebraic predator-prey model including two delays, Beddington-DeAngelis functional response and nonlinear predator harvesting is proposed. Without considering time delay, the existence of singularity induced bifurcation is analyzed by regarding economic interest as bifurcation parameter. In order to remove singularity induced bifurcation and stabilize the proposed system, state feedback controllers are designed in the case of zero and positive economic interest respectively. By the corresponding characteristic transcendental equation, the local stability of interior equilibrium and existence of Hopf bifurcation are discussed in the different case of two delays. By using normal form theory and center manifold theorem, properties of Hopf bifurcation are investigated. Numerical simulations are given to demonstrate our theoretical results.

    Citation: Xin-You Meng, Yu-Qian Wu. Bifurcation analysis in a singular Beddington-DeAngelis predator-prey model with two delays and nonlinear predator harvesting[J]. Mathematical Biosciences and Engineering, 2019, 16(4): 2668-2696. doi: 10.3934/mbe.2019133

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  • In this paper, a differential algebraic predator-prey model including two delays, Beddington-DeAngelis functional response and nonlinear predator harvesting is proposed. Without considering time delay, the existence of singularity induced bifurcation is analyzed by regarding economic interest as bifurcation parameter. In order to remove singularity induced bifurcation and stabilize the proposed system, state feedback controllers are designed in the case of zero and positive economic interest respectively. By the corresponding characteristic transcendental equation, the local stability of interior equilibrium and existence of Hopf bifurcation are discussed in the different case of two delays. By using normal form theory and center manifold theorem, properties of Hopf bifurcation are investigated. Numerical simulations are given to demonstrate our theoretical results.


    Bone tumors, especially the benign tumors and tumor-like lesions were commonly located at the proximal femur, especially at the femoral head and neck [1]. The femoral head and neck endured the compression stress, shear force and torsion force of the hip, this special anatomic and biomechanical characteristic was very important for the overall mechanical transmission [2,3,4,5,6,7]. The normal bone, especially the trabecular bone might be destructed in the case of a tumor in the femoral head and neck, then pathological fracture might occur after a trauma, or gradual fatigue failures might occur over a long time. Besides, the blood supply to the femoral head and neck was fragile [8,9], and necrosis of the femoral head might occur after the invasion of the tumor or the operation of the surgery. The anterior approach, lateral approach, and posterior approach were the three main pathways for tumor of the femoral head and neck. Different surgical approach had different drilling site in the bone, and different drilling site meant different exposure of operative field and surgical operation [10,11,12,13,14,15], and different drilling site might influence the mechanical stability of the proximal femur differently.

    With the application of arthroscopic technique, the tumor cavity could be curetted directly under the arthroscopy by tunneling through the proximal cortex of the femur to the femoral neck medullary canal without opening the joint capsule, therefore the tumor could be curetted completely, and the recurrence rate would be reduced greatly [16,17,18]. Therefore, surgeons focused on which site for drilling would influence the biomechanics of the proximal femur minimally, and the biomechanical stability of which site after reconstruction would be maximum. In our review of the literature, there was few reports to compare the biomechanical influence of drilling in the anterior femoral neck to that in the lateral proximal femur, and there were few reports to compare the biomechanical influence on the proximal femur of the two different drilling sites after the internal fixation. To evaluate these influences from a clinical treatment view, biomechanical experiments of the specimen and finite element studies were done.

    Twelve paired formalin-fixed human cadaveric femora showing no deformities were obtained from Department of Human anatomy and histoembryology, Fudan University (average age: 79.9; range: 64–93 yrs.), leaving the bone devoid of any soft tissue.

    The femurs were grouped randomly into 2 groups of 6 pairs each, which were group 1 and group 2, and one of each pair of femora was grouped randomly to drill the hole in the anterior femoral neck (group 1 ADH and group 2 ADH), and the contralateral femur was assigned to drill the hole in the lateral of the proximal femur (group 1 LDH and group 2 LDH). The group 1 specimens had three stages during the experiment process, which were stage 1: Intact proximal femur (Figure 1a, b), stage 2: Drilled hole and curettage (Figure 1c, d), stage 3: Bone-grafting and fixation, with lag screws in anterior group or proximal femoral locking plate in lateral group (Figure 1e, f). While the group 2 specimens had two stages during the experiment process, which were stage 1: Intact proximal femur, stage 2: Drilled hole and curettage.

    Figure 1.  Models of group 1 femora had three stages during the experiment process. (a, b) stage 1: Intact proximal femur; (c, d) stage 2: Drilled hole and curettage; (e) stage 3: Bone-grafting and fixation with lag screws in anterior group and (f) stage 3: Bone-grafting and fixation with proximal femoral locking plate in lateral group.

    All the holes were oval-shaped, and we controlled the dimensions of these holes according to anatomical parameters of each femur, as to these holes in the anterior femoral neck, the length and width of the neck were designed as the two diameters of the oval (Figure 1c), then the bone was drilled according the elliptical column until the posterior cortex of the femoral neck to form an elliptical cylindrical bone defect. While to these holes in the lateral of the proximal femur, these holes were drilled on the lateral cortical bones intersected with the axis of the neck, and the thickness of this area and the width of the neck were designed as the two diameters of the oval (Figure 1d). Then the bone was drilled according the elliptical column until the junction of femoral head and neck to form an elliptical cylindrical bone defect too. Different femur had different hole.

    The specimens were kept moist with 0.9% NaCl saline solution during the whole preparation and testing process.

    All of the specimens of different stages were scanned with CT (Philips Brilliance 64 slice, Netherlands, slice thickness 0.65 mm) and X-ray from anterior-posterior and lateral.

    All femora were embedded distally in polymethylmethacrylate (PMMA) in a Materials Testing Machine (Instron e10000; USA) to mimic the weight of the femur during one-legged stance (angle between loading axis and the proximal shaft 15°) [19,20] (Figure 2). As to the axial loading testing, the load was applied to the most cranial portion of the femoral head in the plane spanned by the neck axis and the proximal femur axis, and 10 mm of the femoral head was embedded in a PMMA cup, simulating the acetabulum, for load distribution according reports [19,21]. As to the torsional stiffness testing, the femoral head was fixed with a structure of three claws in the materials testing machine to allow rotation orthogonally to the loading axis through the femoral head (Figure 2).

    Figure 2.  The angle between loading axis and the proximal shaft was 15° during the mechanical testing, which was in a one-legged stance.

    Finally, a vertical load was applied to femora of group 1 on stage 3 and femora of group 2 on stage 2 to create axial compression until complete catastrophic failure of these femora occurred. Peak force was defined as axial strength. The locations of failure were observed and analyzed to evaluate the biomechanical stability of the proximal femur of different models.

    In order to simulate natural hip articulation, the femoral head was not stabilized but was free to rotate within the PMMA cup during the axial loading. This mode of loading was actually a combination of axial compression and bending, which has been reported [19], since the load was applied off the axis of the femur shaft.

    For torsion testing, every card slot of the three was screwed tightly onto the surface of the femoral head averagely for stabilization. The vertical axis of twist was through the femoral head, which was different from some reports which was through the long axis of the femoral shaft [22,23,24,25]. Figure 2 depicted the experimental setup for torsional loading, the set-up in axial loading was similar, except that a PMMA cup was used at the femoral head instead of card slots.

    In order to keep the femora remained in the linear–elastic regime before the ultimate axial loading failure testing, the axial stiffness was determined by vertically applying a vertical displacement of 1 mm maximum using displacement control 1.5 mm/min during the axial loading testing. The machine was programmed to cease loading once 1 mm of displacement was reached, i.e., a maximum displacement criterion. While during the ultimate loading failure testing, the displacement control 1.5 mm/min was used until the loading failed.

    Similarly, in order to keep the bones remained in the linear–elastic regime during torsion testing, torsional stiffness was determined by applying a maximum 7.5 Nm torque axial preload = 0.1 kN, pretorque = 0 Nm at the femoral head using angular displacement control 0.25 deg/ s in rotation. The machine was programmed to cease torque application using this maximum torque criterion.

    To prevent permanent deformation or microcracks which might occur in a given loading, we monitored the load-displacement curve and torque-angle curve during the mechanical testing, if the curve became nonlinear suddenly, it meant the bone was no longer in a linear elastic regime, and if it happened before the axial loading failure testing, these data of this femur would be abandoned.

    The serial CT images of the femur were acquired from one of the twelve paired formalin-fixed human cadaveric femora on stage 1. The slice thickness of the CT images was 0.65 mm in a 512 × 512 matrix. The DICOM data were imported into Mimics 17.0 software (Materialise, Belgium) to reconstruct the geometry of the femur. The femur bone was segmented into 2 partitions, the cortical layer and cancellous core, using a threshold of 600 Hounsfield units [26]. The material of the cortical and cancellous bone was assumed homogeneous and isotropic.

    Two types of fixation/implants were modeled and simulated: Proximal lateral femur Locking Plate with 4.5 mm locking screw (PFLP) and 6.5 mm partially threaded cancellous screws. Three dimensional models of plate and screws were drawn according to the manufacturers' specifications using software UG NX 8.5 (SIEMENS Corp., Germany). The locking plate was modeled from a 4.5 mm plate (Kanghui, China) and the locking screws were modeled as 4.5 mm diameter solid cylinders. The partially threaded cancellous screws were modeled as 6.5 mm diameter.

    Two different oval shaped models were drawn to intersect with the intact femur FE model according to the methods of the specimen preparation, thus FE models of ADH and LDH were simulated (Figure 3a, b). Similarly, a model of ADH with bone-grafting and fixation (ADBF) and a model of LDH with bone-grafting and fixation (LDBF) were simulated by Boolean operation with PFLP or three 6.5 mm partially threaded cancellous screws (Figure 3c, d).

    Figure 3.  (a): FE model of ADH; (b): FE model of LDH; (c): FE model of ADBF; (d): FE model of LDBF; (f): The mesh for LDH model.

    These models were processed by Geomagic Studio 2014 (3D System Inc., Rock Hill, SC, USA) and then, were input to the FE software ANSYS Workbench 15 (ANSYS Corp., USA), thus these models were assembled and meshed (Figure 3f). Due to the ease and robustness of performing automatic meshing, local and adaptive refinement with tetrahedral elements, linear tetrahedral elements were often used in the literature [27,28]. The 10-node tetrahedral element was a high-order form of a 4-node tetrahedral element, and its element boundary was a curved surface, which could mesh the structural irregular model well, while 8-node hexahedron element was often used to mesh the structural regular model [29]. We used the 10-node tetrahedral element to hand with multiple femoral interfaces in FE analysis [30]. The numbers of nodes and elements of femora, bone grafts and metallic implants were shown in Table 1. A mesh convergence test was conducted so that the deviation was less than 2%.

    Table 1.  Numbers of nodes and elements of different models.
    Model Intact femur ADH LDH ADBF Bone graft in ADBF 3 screws LDBF Bone graft in LDBF PFLP
    nodes 43805 40375 42493 146940 5182 79415 216142 4369 164287
    elements 25480 22981 24163 88187 3026 47807 133244 2477 103814

     | Show Table
    DownLoad: CSV

    For the bone tissues, the constitutive elastic/plastic model was used [31]. Compared with a high Young's modulus of the fresh-frozen specimens [32], the formalin-fixed bones were reported to show a significantly lower Young's modulus compared to the fresh-frozen specimens [33], so we assigned a lower Young's modulus to the cortical bone of our FE model, and the material parameters of cancellous bone of the femur and implants were adopted from previous published reports [20,34,35,36,37,38,39] (Table 2). As to the bone grafts, we assigned a mechanical property of cancellous bone to them to simulate the mechanical testing and clinical operation. All contact pairs including bone grafts to femurs, metallic implants to femurs, metallic implants to bone grafts, were assigned with 0.3 coefficient of friction [40,41], except that the locking plate-locking screws interfaces were tied.

    Table 2.  Material properties of cortical and cancellous bone, and titanium alloy.
    Material Young's modulus (MPa) Poisson's ratio
    Cortical bone 5000 0.3
    Cancellous bone 840 0.2
    titanium alloy implants 110000 0.33

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    For both torsional and axial loading, the distal bone was rigidly fixed i.e., zero displacement boundary condition to a distance of 25 cm below the proximal end. For the torsional loading scenario, coupling contact between the loading spot above the femur head and the femur head was assumed, and the spot was constrained in all degrees of freedom except the rotation. We marked a dot on the femoral head, and the angle of internal rotation of this dot was calculated automatically by ANSYS after the femoral head was rotated internally, and this angle was considered to the angle of internal rotation proximal femur. Then a torque of 7.5 Nm, perpendicular to the top surface of the spot was then applied, and the torsional stiffness was calculated by dividing the applied torque by the angular displacement of the loading spot.

    For the axial loading scenario, frictionless sliding contact between the loading spot and the femur head was assumed, and the spot was prevented from moving in all degrees of freedom except vertical displacement. We assumed the quality of an adult was 60 kg, according to the report published [42], a vertical load of 1.56 kN (2.6 times of the weight) was applied to the spot, and the axial stiffness was calculated by dividing the applied load by the vertical displacement of the spot.

    To facilitate comparison between specimens of different length, the measured and FE predicted axial (kN/mm) and torsional stiffnesses (Nm/deg) were converted to effective axial (kN) and torsional rigidities (Nm2/deg), as has been done by previous investigators [20,43,44]. Simply stated, rigidity was a product of a stiffness timed femur length.

    The data were analyzed by SAS software version 9.4 (SAS Institute, Cary, NC). Continuous variables with normal distribution were presented as mean (standard deviation [SD]); non-normal variables were reported as median (interquartile range [IQR]). Means of 2 continuous normally distributed variables were compared by independent samples Student's t test. Wilcoxon signed-rank test were used, respectively, to compare means of 2 and 3 or more groups of variables not normally distributed. P < 0.05 was considered statistically significant.

    The data of measured stiffnesses and rigidities of the cadaveric specimens were shown in Tables 3-5.

    Table 3.  Axial stiffnesses of group 1 femora in stage 1, stage 2 and stage 3 in mechanical testing (N/mm).
    Model Total(Mean ± SD) ADH(Mean ± SD) LDH(Mean ± SD)
    Stage1: Intact femur 702.39 ± 197.43 726.34 ± 118.61 678.44 ± 256.16
    Stage2: Drilled hole 590.87 ± 204.66 613.15 ± 136.84 568.60 ± 268.77
    Stage3: Drilling, bone-grafting and fixation 824.31 ± 348.79 672.70 ± 271.51 975.92 ± 372.50

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    Table 4.  Torsional rigidity of group 1 femora in stage 1, stage 2 and stage 3 in mechanical testing (Nm2/deg).
    Model Total(Mean ± SD) ADH(Mean ± SD) LDH(Mean ± SD)
    stage1: Intact femur 1.95 ± 0.63 1.80 ± 0.51 2.10 ± 0.74
    stage2: Drilled hole 1.52 ± 0.46 1.35 ± 0.37 1.70 ± 0.51
    stage3: Drilling, bone-grafting and fixation 1.74 ± 0.59 1.57 ± 0.67 1.90 ± 0.50

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    Table 5.  Rigidities of group1 femora in stage 3 and group 2 specimens in stage 2 (N).
    LDH(P25–P75) ADH(P25–P75)
    Group 1 4826.81(3142.69–6841.98) 3004.14(1581.14–3919.93)
    Group 2 4160.87(2240.18–5063.75) 2218.87(1165.55–4131.96)

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    Group 1 cadaveric femurs on stage 1 were stiffer (P = 0.0005) in axial compression than group 1 cadaveric femurs on stage 2, with P = 0.0313 in group 1 ADH and P = 0.0313 in group 1 LDH respectively, and the degree of decline made no statistical significance (P = 0.9715). And group 1 cadaveric femurs on stage 3 were stiffer (P = 0.0269) than group 1 cadaveric femurs on stage 2 in axial compression, with P = 0.0313 in group1 LDH, but P = 0.1294 in group 1 ADH. There was no statistical significance between the axial stiffnesses of group 1 femurs on stage 1 and stage 3 (P = 0.1514), with P = 0.6875 in group 1 ADH, but group 1 LDH cadaveric femurs on stage 3 were stiffer (P = 0.0313) in axial compression than group 1 cadaveric femurs on stage 1.

    Similarly, in torsion the group 1 cadaveric femurs on stage 1 were stiffer (P = 0.0005) than the cadaver femurs on stage 2, with P = 0.03 in group 1 ADH and P = 0.03 in group 1 LDH respectively, and the degree of decline made no statistical significance (P = 0.8697). While there was no statistical significance between the group 1 cadaveric femurs on stage 3 and stage 2 (P = 0.1294) in torsion, with P = 0.4375 in group 1 ADH and P = 0.22 in group 1 LDH respectively.

    Although the medians of axial strength of group 1 cadaveric femurs, both of group 1 ADH and group 1 LDH, were much bigger than group 2 cadaveric femurs on stage 2, and the medians of axial strength of LDH cadaveric femurs, both of group 1 and group 2, were much bigger than ADH cadaveric femurs, there was no statistical significance between the axial strength of group 1 cadaveric femurs on stage 3 and group 2 on stage 2 (P = 0.2247), with P = 0.5276 in ADH and P = 0.2264 in LDH respectively (Figure 4).

    Figure 4.  The Box-plot showed that the axial strength of LDH model was much bigger than that of ADH model, and the axial strength of LDBF model was much bigger than that of ADBF model, even though there were no statistical difference.

    Due to the difficulty to achieve a lot of human cadaveric femora at one time, no femora on stage 1 were axial loaded to failure, so we referred to literatures [32,45], which showed that the fracture lines of intact femora began from the super-lateral region between the femoral head and neck, then went down straightly, and stopped on the lesser trochanter, with the lesser trochanter fractured (Figure 5a, b). And the fracture lines of the axial loading failure of group 2 ADH after drilling hole were similar to the fracture line on stage 1 (Figure 5c, d). While the fracture lines of the axial loading failure of group 2 LDH on stage 2 were on the lateral proximal femur, which went across the lateral cortical window and stopped on the lesser trochanter, with the lesser trochanter fractured too (Figure 5e, f).

    Figure 5.  (a, b): The fracture line of intact femora, which began from the super-lateral region between the femoral head and neck, then went down straightly, and stopped on the lesser trochanter, the lesser trochanter was not involved; (c, d): The fracture line of the axial loading failure of group 2 ADH on stage 2 was similar to the fracture line of intact femora; (e, f): The fracture lines of the axial loading failure of group 2 LDH on stage 2, which was located on the lateral proximal femur, went across the cortical window and stopped on the lesser trochanter, with the lesser trochanter fractured.

    When it came to the group 1 ADH on stage 3 and group 1 LDH on stage 3, the locations of the axial loading failure of were similar, and the fracture lines began from the super-lateral region between the femoral head and neck, then went down straightly, and stopped above the lesser trochanter, with the lesser trochanter not involved (Figure 6). All of fracture lines of the axial loading failure of group 1 ADH on stage 3, group 2 ADH on stage 2 and group 2 LDH on stage 2 went across the cortical window.

    Figure 6.  The fracture lines of the axial loading failure of group 1 ADH on stage 3 (a, b) and group 1 LDH on stage 3 (c, d) were similar, which began from the super-lateral region between the femoral head and neck, then went down straightly, and stopped above the lesser trochanter, with the lesser trochanter not involved.

    For the axial loading, equivalent (von-Mises) stress nephograms under axial loading were shown in Figure 7, and the results were shown in Table 6. The results showed that the axial stiffness of model of LDH was smaller than that of the intact proximal femur model, and the axial stiffness of model of ADH were smaller than that of model of LDH. Compared to the different drilling models respectively, the axial stiffness of LDBF model increased much more than that of ADBF model, even more stiff than the intact proximal femur model, and this trend was similar to the biomechanical testing of specimens. Only the location of the von-Mises stress in ADBF model was in the super-lateral region between the femoral head and neck, which were consistent with the site of axial loading failure in ADBF model in mechanical testing, none of the locations of the von-Mises stress in the rest of FE models were consistent with the site of axial loading failure in relevant model respectively in mechanical testing, which meant the locations of the von-Mises stress were consistent with the sites of axial loading failure in 20% models in Mechanical testing.

    Figure 7.  Equivalent (von-Mises) stress nephograms of the intact femur FE model (a), FE model of ADH (b), FE model of LDH (c), FE model of ADBF (d) and FE model of LDBF (e) under axial loading with 1560N, and red arrows showed the areas of the max von-Mises stress.
    Table 6.  The axial stiffness, von-Mises stress, the maximum principal stress, the maximum sheer stress, and the equivalent elastic strain in different models under axial loading with 1560N.
    Models axial stiffness(N/mm) von-Mises stress(MPa) the maximum principal stress(MPa) the maximum sheer stress(MPa) the equivalent elastic strain(mm/mm)
    Max location Max location Max location Max location
    Intact femur 1409.214 20.724 COLT 10.757 COFN 10.654 COLT 4.370E-03 CAFN
    ADH 1203.704 57.747 COFN 46.850 COFN 29.493 COFN 1.471E-02 CAFN
    LDH 1313.131 22.193 COFN 20.500 COGT 12.057 COFN 7.317E-03 CAFN
    ADBF 1326.531 37.246 COFH 20.824 COGT 20.388 COFH 4.478E-02 CAFH
    LDBF 1675.618 29.420 COFS 11.182 COFN 14.891 COFS 7.103E-03 COFN
    *COFH: Cortical bone of femoral head, CAFH: Cancellous bone of femoral head, COFN: Cortical bone of femoral neck, CAFN: Cancellous bone of femoral neck, COGT: Cortical bone of greater trochanter of femur, COLT: Cortical bone of lesser trochanter of femur, COFS: Cortical bone of femoral shaft.

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    The maximum principal stress nephograms under axial loading were shown in Figure 8, and the locations of the maximum principal stress were consistent with the sites of axial loading failure in 80% models in Mechanical testing. The locations of the maximum principal stress in intact model and ADH model were in the super-lateral region between the femoral head and neck, which were consistent with these sites of axial loading failure in intact and ADH model in mechanical testing. And the location of the maximum principal stress in LDH model was in the lateral window of proximal femur, and it changed to the super-lateral region between the femoral head and neck in LDBF model, which were consistent with these sites of axial loading failure in LDH and LDBF model. While the location of the maximum principal stress in ADBF model was in the lateral window of proximal femur, which was different from these sites of axial loading failure in ADBF model in mechanical testing.

    Figure 8.  The maximum principal stress nephograms of the intact femur FE model (a), FE model of ADH (b), FE model of LDH (c), FE model of ADBF (d) and FE model of LDBF (e) under axial loading with 1560N, and red arrows showed the areas of the maximum principal stress.

    The maximum principal strain nephograms under axial loading were shown in Figure 9. All locations of the maximum principal strain of the five models were consistent with each site of axial loading failure of relevant model, which meant the locations of the maximum principal strain were consistent with the sites of axial loading failure in 100% models in Mechanical testing.

    Figure 9.  The maximum principal strain nephograms of the intact femur FE model (a), FE model of ADH (b), FE model of LDH (c), FE model of ADBF (d) and FE model of LDBF (e) under axial loading with 1560N, and red arrows showed the areas of the maximum principal strain.

    For the torsional loading, equivalent (von-Mises) stress nephograms were shown in Figure 10, and the results were shown in Table 7, which showed that the torsional stiffness of LDH model and ADH model were smaller than that of the intact proximal femur model, which was consistent with biomechanical testing of specimens.

    Figure 10.  Equivalent (von-Mises) stress nephograms of the intact femur FE model (a), FE model of ADH (b), FE model of LDH (c), FE model of ADBF (d) and FE model of LDBF (e) under torsional loading with 7.5 Nm, and red arrows showed the areas of the maximum von-Mises stress.
    Table 7.  The angle of internal rotation, von-Mises stress, the maximum principal stress, the maximum sheer stress, and the equivalent elastic strain in different models under the torsional loading with 7.5 Nm.
    Models von-Mises stress(MPa) the maximum principal stress(MPa) the maximum sheer stress(MPa) the equivalent elastic strain(mm/mm)
    angle of internal rotation(°) Max location Max location Max location Max location
    Intact femur 0.484 5.688 COFN 5.618 COFN 2.879 COFN 1.14E-03 COFN
    ADH 0.575 28.653 COFN 28.963 COFN 14.429 COFN 5.75E-03 CAFN
    LDH 0.490 7.396 COGT 6.938 COGT 3.798 COGT 2.11E-03 CAGT
    ADBF 0.552 11.543 CAFH 10.817 COFN 5.943 CAFH 1.39E-02 CAFH
    LDBF 0.589 6.868 COFN 6.567 COFN 3.646 COFN 2.00E-03 IB
    *CAFH: Cancellous bone of femoral head, COFN: Cortical bone of femoral neck, CAFN: Cancellous bone of femoral neck, COGT: Cortical bone of greater trochanter of femur, CAGT: Cancellous bone of greater trochanter of femur, IB: implanted bone

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    The femur was not only the most common long bone affected by cancerous metastasis, but also very common affected by benign tumors and tumor-like lesions, especially the proximal femur. Femoral tumor defects would affect the biomechanical stability, even fracture pathologically. Research showed that for a diaphyseal defect that destroyed 50% of the cortex, strength reductions of between 60 and 90% could occur pathologic fracture [46]. Another mechanical testing with human cadaver femurs showed that when the size of defected femoral necks reached 55%, the strength would decrease greatly [47]. Prior researches showed that many factors played a role in pathological fractures, besides the biomechanical properties of the bone itself, the size of the lesion [48,49], the shape [50], the type of lesion [51,52], and the defect site [21,45] were closely related too.

    Sivasundaram R created circular tumor-like defects of 40 mm diameter proximally in the subtrochanteric region on the Anterior (n = 5), Posterior (n = 5), Medial (n = 5), and Lateral (n = 5) sides of 20 synthetic femurs, and intact femurs (n = 4) served as a control group, to examine the risk of pathological fracture with respect to the anterior, posterior, medial, and lateral surfaces on which a proximal tumor defect was located on the femur. The results showed that the Medial tumor-like defect group resulted in statistically lower stiffness values compared with Intact femurs and had lower strength than Anterior and Posterior groups in axial failure [45].

    Similarly, Kaneko TS [53] found that defect site affected hip strength greatly. Lytic defects, modeled as spherical voids, were simulated at various locations within twelve matched pairs of human cadaveric proximal femora neck, and 564 finite element models were created to quantify the effect of location of femoral neck metastases on hip strength under single-limb stance loading, and the effectiveness of a proposed minimally invasive surgical repair technique for restoring hip strength was evaluated too. Defects in the inferomedial aspect of the neck and in the dense trabecular bone near the base of the femoral head had the greatest effect, with hip strengths 23 to 72% and 43 to 64% that of the intact strength, respectively, for 20 mm diameter defects.

    All of these researches focused on predicting the risk of pathological fracture to simulated lesions in femoral neck and head, while our research focused on the treatment to simulate drilling and curettage in different sites.

    Our mechanical testing results and FE results showed that the simulated operation of drilling for curettage decreased the axial stiffness and torsional stiffness of the intact proximal femur greatly, which suggested that the operation of bone-grafting and fixation were needed both in the model of ADH and LDH. But there was no statistical difference on the degree of the decline between different drilling sites, and there was no statistical difference between the model of ADH and LDH on the axial rigidity too. The axial loading failure testing on the intact femur was not performed because each one femur of each pair was used to simulated the model of ADH and the other femur of each pair was used to simulated the model of LDH.

    Clinically, although autogenous nonvascularized fibula graft was used for lesions in the proximal femur after curettage and cryosurgery, higher incidence rate of the pathological fractures was reported with autogenous nonvascularized fibula graft compared to internal fixation. Four cases in sixteen presented with pathological fractures was reported with autogenous nonvascularized fibula graft after curettage and cryosurgery [54], while Nakamura T [14] suggested compression hip screw and synthetic bone graft as a safe and effective method for the treatment of the benign bone tumors including femoral neck lesion, all patients were allowed full weight-bearing with 12 weeks after surgery with no pathological fracture. Though endoprosthetic replacement was reported to be used in treatment of the benign femoral neck lesion, it was considered to be more suitable for agammaessive and recurrent lesions and served as an effective measure after internal fixation failure [55].

    Although treatment of lesions of the proximal femur with internal fixation was suggested to lessen the risk of additional surgery [56], few basic researches on the stability after treatment on the lesion in the proximal femur were reported. We studied the stability of bone-grafting and fixation after curettage in different drilling sites. Although the simulated operation of bone-grafting and fixation in different drilling models increased the axial stiffness and torsional stiffness in mechanical testing, only in case of implanting bones and fixation for the lateral cortical window increased the axial stiffness greatly and made a statistical difference, even more stiff than the intact proximal femur model. The mechanical testing results suggested that only in case of drilling in the lateral cortex, the proximal femur could be more stable after the treatment of implanting bones and fixation.

    FE analysis results showed that the simulated operation of bone-grafting and fixation increased the axial stiffness and torsional stiffness too. Compared with the axial stiffness of LDH model, the axial stiffness of LDBF model increased 362.487 N/mm (1675.618–1313.131 N/mm), which meant the operation of bone-grafting and fixation increased 27.82% of the axial stiffness of LDH model. When it came to the ADBF model, the axial stiffness of ADBF model increased 122.827 N/mm (1326.531–1203.704 N/mm) to the axial stiffness of ADH model, which meant the operation of bone-grafting and fixation increased 10.20% of the axial stiffness of ADH model. The increasing extent of axial stiffness of LDBF model from stage 3 to stage 2 (27.82%) was nearly three times more than that of ADBF model from stage 3 to stage 2 (10.20%). Although the fixation type might play a part, different drilling sites were the main reason, because the axial stiffness of ADBF model was only 1.02% bigger than that of LDH model, while the axial stiffness of LDBF model was 26.32% bigger than that of ADBF model, even 18.90% bigger than that of intact proximal femur model.

    The fracture line of axial loading in a single leg standing position of both new fresh-frozen intact proximal femurs [32] and intact third generation composite femurs [45] started from the tensional side of femur, which started from the super-lateral region between the femoral head and neck, then went down straightly, and stopped above the lesser trochanter, the lesser trochanter was not involved. While the fracture line of axial loading in both group 2 LDH and ADH on stage 2 went across the opening cortical window and stopped on the lesser trochanter, with the lesser trochanter fractured, which suggested that the operation of drilling decreased the axial stability of the femur. The fracture lines of axial loading in both Group1 LDH and ADH on stage 3 were similar to the intact proximal femur, with the lesser trochanter was not involved. [32,45], which suggested that the operation of bone-grafting and fixation increased the axial stability of the femur with cortical drilled and curettage.

    As to the facture location predicted by FE analysis, Dragomir-Daescu's experiment showed fracture patterns of the FEA (83% agreement) correlated well with experimental data [57]. Yosibash's FE analysis showed that their predicted locations were accurate in 8 out of 14 fracture locations [54,58]. In Derikx's experiment, the FE ranking of load to failure corresponded very well with the actual experimental ranking (τ = 0.87; p < 0.001), and the location of the fracture was correctly predicted in the femora with metastatic lesions, while in intact femora there was a difference between the predicted and actual location of the fractures [59].

    As we knew, the von Mises stress, the Drucker–Prager, maximum principal strain and maximum principal stress were used as 'yield criterions' to predict the 'yield' or 'fracture' load by FE analyses [60,61,62,63]. Zohar Yosibash [64] suggested that the surface average of the 'maximum principal strain' criterion in conjunction with the orthotropic FE model best predicted both the yield force and fracture location compared with other criteria. The surface average of the 'von Mises stress' criterion in conjunction with our FE models only predicted 20% fracture locations in our mechanical testing successfully, and the surface average of the 'maximum principal stress' criterion in conjunction with our FE models predicted 80% fracture locations in our mechanical testing successfully. When it came to the 'maximum principal strain' criterion, the locations of the maximum principal strain were consistent with the sites of axial loading failure in 100% models in Mechanical testing, which suggested that our research was consistent with Zohar Yosibash's study, and our FE models were reliable.

    Due to the difficulty in obtaining a sufficient number of fresh-frozen human cadaveric femora at one time, we chose formalin-fixed specimens for our mechanical testing as previous researches [65,66], though the stiffness of the formalin-fixed femora might be weaker than the fresh-frozen femora, the formalin-fixed femora could also show the trend of drilling hole and fixing with bone graft and internal fixation very well. Another limitation was the FE-modeling of only one specimen, and the results of FE analysis had a certain reference value for our clinical operation.

    Despite these limitations, the results of this study confirmed that the operation of drilling and curettage decreased the stability of the proximal femur significantly, and the operation of bone-grafting and fixation after drilling in the lateral proximal femur increased the stability of the proximal femur significantly compared with drilling in the anterior femur neck. Our research suggested that the drilling site should be operated in the lateral proximal femur to get a bigger stability of the operation of drilling and bone-grafting and fixation for benign lesions in femoral head and neck.

    This work was supported by the National Natural Science Foundation of China, Grant No. 61876109.

    There are no conflicts of interest.



    [1] M. Kot, Elements of Mathematical Biology, Cambridge University Press, Cambridge, 2001.
    [2] S. Levin, T. Hallam and J. Cross, Applied Mathematical Ecology, Springer, New York, 1990.
    [3] R. May, Stability and Complexity in Model Ecosystems, Princeton University Press, Princeton, 1993.
    [4] C. Ji, D. Jing and N. Shi, A note on a predator-prey model with modified Leslie-Gower and Holling-type II schemes with stochastic perturbatio, J. Math. Anal. Appl., 377 (2011), 435–440.
    [5] T. Kar and H. Matsuda, Global dynamics and controllability of a harvested prey-predator system with Holling type III functional response, Nonlinear Anal. Hybrid Syst., 1 (2007), 59–67.
    [6] X. Meng, J. Wang, H. Huo, Dynamical behaviour of a nutrient-plankton model with Holling type IV, delay, and harvesting, Discrete Dyn. Nat. Soc., 2018 (2018), Article ID 9232590.
    [7] X. Meng, H. Huo, H. Xiang, et al., Stability in a predator-prey model with Crowley-Martin function and stage structure for prey, Appl. Math. Comput., 232 (2014), 810–819.
    [8] W. Yang, Diffusion has no influence on the global asymptotical stability of the Lotka-Volterra pre-predator model incorporating a constant number of prey refuges, Appl. Math. Comput., 223 (2013), 278–280.
    [9] Y. Zhu and K.Wang, Existence and global attractivity of positive periodic solutions for a predatorprey model with modified Leslie-Gower Holling-type II schemes, J. Math. Anal. Appl., 384 (2011), 400–408.
    [10] J. Liu, Dynamical analysis of a delayed predator-prey system with modified Leslie-Gower and Beddington-DeAngelis functional response, Adv. Difference Equ., 2014 (2014), 314–343.
    [11] X. Liu and Y. Wei, Dynamics of a stochastic cooperative predator-prey system with Beddington- DeAngelis functional response, Adv. Difference Equ., 2016 (2016), 21–39.
    [12] C. Li, X. Guo and D. He, An impulsive diffusion predator-prey system in three-species with Beddington-DeAngelis response, J. Appl. Math. Comput., 43 (2013), 235–248.
    [13] T. Ivanov and N. Dimitrova, A predator-prey model with generic birth and death rates for the predator and Beddington-DeAngelis functional response, Math. Comput. Simulat., 133 (2017), 111–123.
    [14] Q. Meng and L. Yang, Steady state in a cross-diffusion predator-prey model with the Beddington- DeAngelis functional response, Nonlinear Anal.: Real World Appl., 45 (2019), 401–413.
    [15] W. Liu, C. Fu and B. Chen, Hopf bifurcation and center stability for a predator-prey biological economic model with prey harvesting, Commun. Nonlinear Sci. Numer. Simul., 17 (2012), 3989– 3998.
    [16] F. Conforto, L. Desvillettes and C. Soresina, About reaction-diffusion systems involving the Holling-type II and the Beddington-DeAngelis functional responses for predator-prey models, Nonlinear Differ. Equ. Appl., 25 (2018), 24.
    [17] X. Sun, R. Yuan and L. Wang, Bifurcations in a diffusive predator-prey model with Beddington- DeAngelis functional response and nonselective harvesting, J. Nonlinear Sci., 29 (2019), 287–318.
    [18] J. Beddington, Mutual interference between parasites or predators and its effect on searching efficiency, J. Anim. Ecol., 44 (1975), 331–340.
    [19] D. DeAngilis, R. Goldstein and R. Neill, A model for tropic interaction, Ecology, 56 (1975), 881–892.
    [20] H. Freedman, Deterministic Mathematical Models in Population Ecology, Marcel Dekker, New York, 1980.
    [21] G. Seifert, Asymptotical behavior in a three-component food chain model, Nonlinear Anal. Theory Methods Appl., 32 (1998), 749–753.
    [22] C. Liu, Q. Zhang, X. Zhang, et al., Dynamical behavior in a stage-structured differential-algebraic prey-predator model with discrete time delay and harvesting, J. Comput. Appl. Math., 231 (2009), 612–625.
    [23] X. Meng, H. Huo, X. Zhang, et al., Stability and hopf bifurcation in a three-species system with feedback delays, Nonlinear Dyn., 64 (2011), 349–364.
    [24] X. Meng and Y. Wu, Bifurcation and control in a singular phytoplankton-zooplankton-fish model with nonlinear fish harvesting and taxation, Int. J. Bifurcat. Chaos, 28 (2018), 1850042(24 pages).
    [25] H. Xiang, Y. Wang and H. Huo, Analysis of the binge drinking models with demographics and nonlinear infectivity on networks, J. Appl. Anal. Comput., 8 (2018), 1535–1554.
    [26] K. Chakraborty, M. Chakraboty and T. Kar, Bifurcation and control of a bioeconomic model of a prey-predator system with a time delay, Nonlinear Anal. Hybrid Syst., 5 (2011), 613–625.
    [27] W. Liu, C. Fu and B. Chen, Hopf birfucation for a predator-prey biological economic system with Holling type II functional response, J. Franklin Inst., 348 (2011), 1114–1127.
    [28] G. Zhang, B. Chen, L. Zhu, et al., Hopf bifurcation for a differential-algebraic biological economic system with time delay, Appl. Math. Comput, 218 (2012), 7717–7726.
    [29] T. Faria, Stability and bifurcation for a delayed predator-prey model and the effect of diffusion, J. Math. Anal. Appl., 254 (2001), 433–463.
    [30] G. Zhang, Y. She and B. Chen, Hopf bifurcation of a predator prey system with predator harvesting and two delays, Nonlinear Dyn., 73 (2013), 2119–2131.
    [31] J. Zhang, Z. Jin, J. Yan, et al., Stability and Hopf bifurcation in a delayed competition system, Nonlinear Anal. Theory Methods Appl., 70 (2009), 658–670.
    [32] Z. Lajmiri, R. K. Ghaziani and I. Orak, Bifurcation and stability analysis of a ratio-dependent predator-prey model with predator harvesting rate, Chaos Soliton Fract., 106 (2018), 193–200.
    [33] M. Liu, X. He and J. Yu, Dynamics of a stochastic regime-switching predator-prey model with harvesting and distributed delays, Nonlinear Anal. Hybrid Syst., 28 (2018), 87–104.
    [34] T. Das, R. Mukerjee and K. Chaudhuri, Harvesting of a prey-predator fishery in the presence of toxicity, Appl. Math. Model., 33 (2009), 2282–2292.
    [35] R. Gupta and P. Chandra, Bifurcation analysis of modied Leslie-Gower predator-prey model with Michaelis-Menten type prey harvesting, J. Math. Anal. Appl., 398 (2013), 278–295.
    [36] P. Srinivasu, Bioeconomics of a renewable resource in presence of a predator, Nonlinear Anal. Real World Appl., 2 (2001), 497–506.
    [37] G. Lan, Y. Fu, C. Wei, et al., Dynamical analysis of a ratio-dependent predator-prey model with Holling III type functional response and nonlinear harvesting in a random environment, Adv. Differ. Equ., 2018 (2018), 198.
    [38] R. Gupta and P. Chandra, Dynamical complexity of a prey-predator model with nonlinear predator harvesting, Discrete Contin. Dyn. Syst. Ser. B, 20 (2015), 423–443.
    [39] J. Liu and L. Zhang, Bifurcation analysis in a prey-predator model with nonlinear predator harvesting, J. Franklin Inst., 353 (2016), 4701–4714.
    [40] K. Chakraborty, S. Jana and T. Kar, Global dynamics and bifurcation in a stage structured preypredator fishery model with harvesting, Appl. Math. Comput., 218 (2012), 9271–9290.
    [41] H. Gordon, The economic theory of a common property resource: the fishery, Bull. Math. Biol., 62 (1954), 124–142.
    [42] C. Liu, Q. Zhang and X. Duan, Dynamical behavior in a harvested differential-algebraic preypredator model with discrete time delay and stage structure, J. Franklin Inst., 346 (2009), 1038– 1059.
    [43] X. Zhang and Q. Zhang, Bifurcation analysis and control of a class of hybrid biological economic models, Nonlinear Anal. Hybrid Syst., 3 (2009), 578–587.
    [44] C. Liu, N. Lu, Q. Zhang, et al., Modelling and analysis in a prey-predator system with commercial harvesting and double time delays, J. Appl. Math. Comput., 281 (2016), 77–101.
    [45] M. Li, B. Chen and H. Ye, A bioeconomic differential algebraic predator-prey model with nonlinear prey harvesting, Appl. Math. Model., 42 (2017), 17–28.
    [46] P. Leslie and J. Gower, The properties of a stochastic model for the predator prey type of interaction between two species, Biometrika, 47 (1960), 219–234.
    [47] R. Cantrell and C. Cosner, On the dynamics of predator-prey models with the Beddington- DeAngelis functional response, J. Math. Anal. Appl., 257 (2001), 206–222.
    [48] L. Dai, Singular Control System, Springer, New York, 1989.
    [49] V. Venkatasubramanian, H. Schattler and J. Zaborszky, Local bifurcations and feasibility regions in differential-algebraic systems, IEEE Trans. Automat. Control, 40 (1995), 1992–2013.
    [50] Q. Zhang, C. Liu and X. Zhang, A singular bioeconomic model with diffusion and time delay, J. Syst. Sci. Complex., 24 (2011), 277–190.
    [51] J. Hale, Theory of Functional Differential Equations, Springer, New York, 1997.
    [52] B. Hassard, N. Kazarinoff and Y. Wan, Theory and Applications of Hopf Bifurcation, Cambridge University Press, Cambridge, 1981.
    [53] J. Guckenheimer and P. Holmes, Nonlinear Oscillations, Dynamical Systems, and Bifurcations of Vector Fields, Springer, New York, 1983.
    [54] Y. Kuang, Delay Differential Equations with Applications in Population Dynamics, Academic Press, New York, 1993.
    [55] H. Freedman and V. S. H. Rao, The trade-off between mutual interference and time lags in predator-prey systems, Bull. Math. Biol., 45 (1983), 991–1004.
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    41. Yasir Habib, Enjun Xia, Shujahat Haider Hashmi, Zeeshan Fareed, Non-linear spatial linkage between COVID-19 pandemic and mobility in ten countries: A lesson for future wave, 2021, 14, 18760341, 1411, 10.1016/j.jiph.2021.08.008
    42. Xiang Ren, Clifford P. Weisel, Panos G. Georgopoulos, Modeling Effects of Spatial Heterogeneities and Layered Exposure Interventions on the Spread of COVID-19 across New Jersey, 2021, 18, 1660-4601, 11950, 10.3390/ijerph182211950
    43. Jingli Ren, Haiyan Wang, 2023, 9780443186790, 173, 10.1016/B978-0-44-318679-0.00012-0
    44. Kevin D. Dayaratna, Drew Gonshorowski, Mary Kolesar, Hierarchical Bayesian spatio-temporal modeling of COVID-19 in the United States, 2022, 0266-4763, 1, 10.1080/02664763.2022.2069232
    45. Mustafa Tevfik KARTAL, Özer DEPREN, Serpil KILIÇ DEPREN, Do Monetary Policy Measures Affect Foreign Exchange Rates during the COVID-19 Pandemic? Evidence from Turkey, 2021, 1307-5705, 175, 10.46520/bddkdergisi.987416
    46. Faray Majid, Aditya M. Deshpande, Subramanian Ramakrishnan, Shelley Ehrlich, Manish Kumar, Analysis of epidemic spread dynamics using a PDE model and COVID-19 data from Hamilton County OH USA, 2021, 54, 24058963, 322, 10.1016/j.ifacol.2021.11.194
    47. Jingli Ren, Haiyan Wang, 2023, 9780443186790, 129, 10.1016/B978-0-44-318679-0.00011-9
    48. Bastien Reyné, Quentin Richard, Christian Selinger, Mircea T. Sofonea, Ramsès Djidjou-Demasse, Samuel Alizon, Jacek Banasiak, Non-Markovian modelling highlights the importance of age structure on Covid-19 epidemiological dynamics, 2022, 17, 0973-5348, 7, 10.1051/mmnp/2022008
    49. R. Matusik, A. Nowakowski, Control of COVID-19 transmission dynamics, a game theoretical approach, 2022, 110, 0924-090X, 857, 10.1007/s11071-022-07654-6
    50. Tao Zheng, Yantao Luo, Xinran Zhou, Long Zhang, Zhidong Teng, Spatial dynamic analysis for COVID-19 epidemic model with diffusion and Beddington-DeAngelis type incidence, 2023, 22, 1534-0392, 365, 10.3934/cpaa.2021154
    51. Rajat Verma, Takahiro Yabe, Satish V. Ukkusuri, Spatiotemporal contact density explains the disparity of COVID-19 spread in urban neighborhoods, 2021, 11, 2045-2322, 10.1038/s41598-021-90483-1
    52. Zipei Fan, Chuang Yang, Zhiwen Zhang, Xuan Song, Yinghao Liu, Renhe Jiang, Quanjun Chen, Ryosuke Shibasaki, Human Mobility-based Individual-level Epidemic Simulation Platform, 2022, 8, 2374-0353, 1, 10.1145/3491063
    53. Bulut Boru, M. Emre Gursoy, Forecasting Daily COVID-19 Case Counts Using Aggregate Mobility Statistics, 2022, 7, 2306-5729, 166, 10.3390/data7110166
    54. Myrsini Ntemi, Ioannis Sarridis, Constantine Kotropoulos, An Autoregressive Graph Convolutional Long Short-Term Memory Hybrid Neural Network for Accurate Prediction of COVID-19 Cases, 2023, 10, 2329-924X, 724, 10.1109/TCSS.2022.3167856
    55. Radosław Matusik, Andrzej Nowakowski, Dual ɛ -closed-loop Nash equilibrium method to study pandemic by numerical analysis, 2023, 107, 2470-0045, 10.1103/PhysRevE.107.044202
    56. Abdul Hamid Ganie, Mashael M. AlBaidani, Adnan Khan, A Comparative Study of the Fractional Partial Differential Equations via Novel Transform, 2023, 15, 2073-8994, 1101, 10.3390/sym15051101
    57. Peng Wang, Jinliang Huang, Difang Huang, A data-driven framework to assess population dynamics during novel coronavirus outbreaks: A case study on Xiamen Island, China, 2023, 18, 1932-6203, e0293803, 10.1371/journal.pone.0293803
    58. Ryan Benjamin, Reproduction number projection for the COVID-19 pandemic, 2023, 2023, 2731-4235, 10.1186/s13662-023-03792-2
    59. Jacob Derrick, Ben Patterson, Jie Bai, Jin Wang, A Mechanistic Model for Long COVID Dynamics, 2023, 11, 2227-7390, 4541, 10.3390/math11214541
    60. Yueran Qi, Yang Feng, Jixuan Wu, Zhaohui Sun, Maoying Bai, Chengcheng Wang, Hai Wang, Xuepeng Zhan, Junyu Zhang, Jing Liu, Jiezhi Chen, An Efficient and Robust Partial Differential Equation Solver by Flash-Based Computing in Memory, 2023, 14, 2072-666X, 901, 10.3390/mi14050901
    61. Ugo Avila-Ponce de León, Angel G. C. Pérez, Eric Avila-Vales, Modeling the SARS-CoV-2 Omicron variant dynamics in the United States with booster dose vaccination and waning immunity, 2023, 20, 1551-0018, 10909, 10.3934/mbe.2023484
    62. Shiqian Nie, Xiaochun Lei, A time-dependent model of the transmission of COVID-19 variants dynamics using Hausdorff fractal derivative, 2023, 629, 03784371, 129196, 10.1016/j.physa.2023.129196
    63. Farhan Saleem, Saadia Hina, Irfan Ullah, Ammara Habib, Alina Hina, Sana Ilyas, Muhammad Hamid, Impacts of irregular and strategic lockdown on air quality over Indo-Pak Subcontinent: Pre-to-post COVID-19 analysis, 2024, 178, 09600779, 114255, 10.1016/j.chaos.2023.114255
    64. İlknur Nina Paslanmaz Uluğ, Cem Sefa Sütcü, Digital Literacy and Awareness of User Location Privacy: What People in Turkey Know About Google COVID-19 Community Mobility Reports?, 2023, 2719-4795, 83, 10.31743/sanp.16189
    65. Jixiao Wang, Chong Wang, The coming Omicron waves and factors affecting its spread after China reopening borders, 2023, 23, 1472-6947, 10.1186/s12911-023-02219-y
    66. Moritz Schäfer, Peter Heidrich, Thomas Götz, Modelling the spatial spread of COVID-19 in a German district using a diffusion model, 2023, 20, 1551-0018, 21246, 10.3934/mbe.2023940
    67. Xu 栩 Zhang 张, Yu-Rong 玉蓉 Song 宋, Ru-Qi 汝琦 Li 李, Prediction of ILI following the COVID-19 pandemic in China by using a partial differential equation, 2024, 33, 1674-1056, 110201, 10.1088/1674-1056/ad6f90
    68. Yukio Ohsawa, Yi Sun, Kaira Sekiguchi, Sae Kondo, Tomohide Maekawa, Morihito Takita, Tetsuya Tanimoto, Masahiro Kami, Risk Index of Regional Infection Expansion of COVID-19: Moving Direction Entropy Study Using Mobility Data and Its Application to Tokyo, 2024, 10, 2369-2960, e57742, 10.2196/57742
    69. Anindya Sen, Nathaniel T. Stevens, N. Ken Tran, Rishav R. Agarwal, Qihuang Zhang, Joel A. Dubin, Forecasting daily COVID-19 cases with gradient boosted regression trees and other methods: evidence from U.S. cities, 2023, 11, 2296-2565, 10.3389/fpubh.2023.1259410
    70. Niketa Ukaj, Christian Hellmich, Stefan Scheiner, Aging Epidemiology: A Hereditary Mechanics–Inspired Approach to COVID-19 Fatality Rates, 2024, 150, 0733-9399, 10.1061/JENMDT.EMENG-7640
    71. F. Assadiki, K. Hattaf, N. Yousfi, Global stability of fractional partial differential equations applied to the biological system modeling a viral infection with Hattaf time-fractional derivative, 2024, 11, 23129794, 430, 10.23939/mmc2024.02.430
    72. Logan Street, Deepak Antony David, Chunyan Liu, Shelley Ehrlich, Manish Kumar, Subramanian Ramakrishnan, Nonlinear Model Predictive Control for Mitigating Epidemic Spread using a Partial Differential Equation Based Compartmental Dynamic Model, 2024, 58, 24058963, 366, 10.1016/j.ifacol.2025.01.062
    73. Md Mahmudul Islam, Taj Azarian, Shaurya Agarwal, Sobur Ali, Capturing the Impact of Vaccination and Human Mobility on the Evolution of COVID-19 Pandemic, 2025, 29, 2168-2194, 2318, 10.1109/JBHI.2024.3514106
    74. Sangwan Lee, Sugie Lee, Devina Widya Putri, Multifaceted associations between built environments and POI visit patterns by trip purposes, 2025, 161, 02642751, 105903, 10.1016/j.cities.2025.105903
    75. Aljawhara H. Almuqrin, Sherif M. E. Ismaeel, C. G. L. Tiofack, A. Mohamadou, Badriah Albarzan, Weaam Alhejaili, Samir A. El-Tantawy, Solving fractional physical evolutionary wave equations using advanced techniques, 2025, 2037-4631, 10.1007/s12210-025-01320-w
    76. Péter Bucsky, How Reliable Is Google And Facebook Mobility Data?, 2024, 12, 13395130, 1, 10.26552/tac.C.2024.2.1
    77. Y. Attia Ben Cherifa, A. Rejeb Bouzgarrou, C. Claramunt, H. Rejeb, Re-appropriation of public spaces in the Tunisian city of Sousse post COVID-19 pandemic, 2025, 1754-9175, 1, 10.1080/17549175.2025.2503720
    78. Weaam Alhejaili, Adnan Khan, Amnah S. Al-Johani, Samir A. El-Tantawy, Novel Approximations to the Multi-Dimensional Fractional Diffusion Models Using the Tantawy Technique and Two Other Transformed Methods, 2025, 9, 2504-3110, 423, 10.3390/fractalfract9070423
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