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Comparative anatomy of the mouse and human ankle joint using Micro-CT: Utility of a mouse model to study human ankle sprains

  • The use of mouse models as a tool to study ankle sprain requires a basic understanding of the similarities and differences between human and mouse ankle joint anatomy. However, few studies have been conducted that address the merits and drawbacks of these differences in the functioning of joints. Twenty hindfoot specimens were obtained from 10 male C57BL/6J mice and scanned using micro-CT. The foot and ankle skeletal structures were reconstructed in three dimensions. Morphological parameters were then measured using a plane projection method and normalized data were compared with those of human ankles. There was no significant difference in the malleolar width, maximal tibial thickness, tibial arc length, trochlea tali arc length or trochlea tali width of the mouse specimens compared with the human model. However, a groove was observed on the talar dome in the mouse specimens which was not observed in humans, the talar dome being more symmetric. The mouse ankle was to a large extent able to mimic the mechanism of a human ankle and so a mouse model could be appropriate for expanding our understanding of ankle biomechanics in general. However, the structural differences in the talar dome in the mouse and human should not be ignored. Although there are some differences in the mouse and human ankle that cannot be ignored, compared to other animals, the human ankle is more similar to that of the mouse.

    Citation: Chao Gao, Zhi Chen, Yu Cheng, Junkun Li, Xiaowei Huang, Liangyi Wei, FanHe, Zong-ping Luo, Hongtao Zhang, Jia Yu. Comparative anatomy of the mouse and human ankle joint using Micro-CT: Utility of a mouse model to study human ankle sprains[J]. Mathematical Biosciences and Engineering, 2019, 16(4): 2959-2972. doi: 10.3934/mbe.2019146

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  • The use of mouse models as a tool to study ankle sprain requires a basic understanding of the similarities and differences between human and mouse ankle joint anatomy. However, few studies have been conducted that address the merits and drawbacks of these differences in the functioning of joints. Twenty hindfoot specimens were obtained from 10 male C57BL/6J mice and scanned using micro-CT. The foot and ankle skeletal structures were reconstructed in three dimensions. Morphological parameters were then measured using a plane projection method and normalized data were compared with those of human ankles. There was no significant difference in the malleolar width, maximal tibial thickness, tibial arc length, trochlea tali arc length or trochlea tali width of the mouse specimens compared with the human model. However, a groove was observed on the talar dome in the mouse specimens which was not observed in humans, the talar dome being more symmetric. The mouse ankle was to a large extent able to mimic the mechanism of a human ankle and so a mouse model could be appropriate for expanding our understanding of ankle biomechanics in general. However, the structural differences in the talar dome in the mouse and human should not be ignored. Although there are some differences in the mouse and human ankle that cannot be ignored, compared to other animals, the human ankle is more similar to that of the mouse.


    Stochastic nonlinear control is a hot topic because of its wide application in economic and engineering fields. The pioneer work is [1,2,3,4,5,6,7,8]. Specifically, [1,2,3] propose designs with quadratic Lyapunov functions coupled with weighting functions and [4,5,6,7,8] develop designs with quartic Lyapunov function, which are further developed by [9,10,11,12]. Recently, a class of stochastic systems (SSs) whose Jacobian linearizations may have unstable modes, has received much attention. Such systems are also called stochastic high-order nonlinear systems (SHONSs), which include a class of stochastic benchmark mechanical systems [13] as a special case. In this direction, [14] studies the state-feedback control with stochastic inverse dynamics; [15] develops a stochastic homogeneous domination method, which completely relaxes the order restriction required in [13], and investigates the output-feedback stabilization for SHONSs with unmeasurable states; [16] investigates the output-feedback tracking problem; [17] studies the adaptive state-feedback design for state-constrained systems. It should be emphasized that [13,14,15,16,17], only achieve stabilization in asymptotic sense (as time goes to infinity). However, many real applications appeals for prescribed-time stabilization, which permits the worker to prescribe the convergence times in advance.

    For the prescribed-time control, [18,19] design time-varying feedback to solve the regulation problems of normal-form nonlinear systems; [20] considers networked multi-agent systems; [21,22] investigates the prescribed-time design for linear systems in controllable canonical form; [23] designs the output-feedback controller for uncertain nonlinear strict-feedback-like systems. It should be noted that the results in [18,19,20,21,22,23] don't consider stochastic noise. For SSs, [24] is the first paper to address the stochastic nonlinear inverse optimality and prescribed-time stabilization problems; The control effort is further reduced in [25]; Recently, [26] studies the prescribed-time output-feedback for SSs without/with sensor uncertainty. It should be noted that [24,25,26] don't consider SHONSs. From practical applications, it is important to solves the prescribed-time control problem of SHONSs since it permits the worker to set the convergence times in advance.

    Motivated by the above discussions, this paper studies the prescribed-time design for SSs with high-order structure. The contributions include:

    1) This paper proposes new prescribed-time design for SHONSs. Since Jacobian linearizations of such a system possibly have unstable modes, all the prescribed-time designs in [24,25,26] are invalid. New design and analysis tools should be developed.

    2) This paper develops a more practical design than those in [13,14,15,16,17]. Different from the designs in [13,14,15,16,17] where only asymptotic stabilization can be achieved, the design in this paper can guarantee that the closed-loop system is prescribed-time mean-square stable, which is superior to those in [13,14,15,16,17] since it permits the worker to prescribe the convergence times in advance without considering the initial conditions.

    The remainder of this paper is organized as follows. In Section 2, the problem is formulated. In Section 3, the controller is designed and the stability analysis is given. Section 4 uses an example to explain the validity of the prescribed-time design. The conclusions are collected in Section 6.

    Consider the following class of SHONSs

    dx1=xp2dt+φT1(x)dω, (2.1)
    dx2=udt+φT2(x)dω, (2.2)

    where x=(x1,x2)TR2 and uR are the system state and control input. p1 is an odd integral number. The functions φi:R2Rm are smooth in x with φi(0)=0, i=1,2. ω is an m-dimensional independent standard Wiener process.

    The assumptions we need are as follows.

    Assumption 1. There is a constant c>0 such that

    |φ1(x)|c|x1|p+12, (2.3)
    |φ2(x)|c(|x1|p+12+|x2|p+12). (2.4)

    We introduce the function:

    μ(t)=(Tt0+Tt)m,t[t0,t0+T), (2.5)

    where m2 is an integral number. Obviously, the function μ(t) is monotonically increasing on [t0,t0+T) with μ(t0)=1 and limtt0+Tμ(t)=+.

    Our control goal is to design a prescribed-time state-feedback controller, which guarantees that the closed-loop system has an almost surely unique strong solution and is prescribed-time mean-square stable.

    In the following, we design a time-varying controller for system (2.1)–(2.2) step by step.

    Step 1. In this step, our goal is to design the virtual controller x2.

    Define V1=14ξ41, ξ1=x1, from (2.1), (2.3) and (2.5) we have

    LV1(ξ1)=ξ31xp2+32ξ21|φ1|2ξ31xp2+32c2ξp+31ξ31(xp2xp2)+ξ31xp2+32c2μpξp+31. (3.1)

    Choosing

    x2=μ(2+32c2)1/pξ1μα1ξ1, (3.2)

    which substitutes into (3.1) yields

    LV1(ξ1)2μpξp+31+ξ31(xp2xp2), (3.3)

    where α1=(2+32c2)1/p.

    Step 2. In this step, our goal is to design the actual controller u.

    Define ξ2=xkx2, from (3.2) we get

    ξ2=x2+μα1ξ1. (3.4)

    By using (2.1)–(2.2) and (3.4) we get

    dξ2=(u+mTμ1+1/mα1ξ1+μα1xp2)dt+(φT2+μα1φT1)dω. (3.5)

    We choose the following Lyapunov function

    V2(ξ1,ξ2)=V1(ξ1)+14ξ42. (3.6)

    It follows from (3.3), (3.5)–(3.6) that

    LV22μpξp+31+ξ31(xp2xp2)+ξ32(u+mTμ1+1/mα1ξ1+μα1xp2)+32ξ22|φ2+μα1φ1|2. (3.7)

    By using (3.4) we have

    ξ31(xp2xp2)|ξ1|3|ξ2|(xp12+xp12)|ξ1|3|ξ2|((β1+1)μp1αp11ξp11+β1ξp12)=(β1+1)μp1αp11|ξ1|p+2|ξ2|+β1|ξ1|3|ξ2|p, (3.8)

    where

    β1=max{1,2p2}. (3.9)

    By using Young's inequality we get

    (β1+1)μp1αp11|ξ1|p+2|ξ2|13μpξp+31+13+p(3+p3(2+p))(2+p)((β1+1)αp11)p+3μ3ξp+32 (3.10)

    and

    β1|ξ1|3|ξ2|p13μpξ3+p1+pp+3(3+p9)3/pβ(3+p)/p1μ3ξp+32. (3.11)

    Substituting (3.10)–(3.11) into (3.8) yields

    ξ31(xp2xp2)23μpξp+31+(pp+3(p+39)3/pβ(p+3)/p1+1p+3(p+33(p+2))(p+2)((β1+1)αp11)p+3)μ3ξp+32. (3.12)

    From (2.3), (2.4), (3.2) and (3.4) we have

    |φ2+μα1φ1|22|φ2|2+2μ2α21|φ1|24c2(|x1|1+p+|x2|1+p)+2c2α21μ2|x1|1+pβ2μ1+p|ξ1|p+1+4c22p|ξ2|1+p, (3.13)

    where

    β2=4c2(1+2pαp+11)+2c2α21. (3.14)

    By using (3.13) we get

    32ξ22|φ2+μα1φ1|213μpξ3+p1+(23+p(p+33(1+p))(1+p)/2(32β2)(3+p)/2+6c22p)μ3(1+p)/2ξp+32. (3.15)

    It can be inferred from (3.7), (3.12) and (3.15) that

    LV2μpξp+31+ξ32(u+mTμ1+1/mα1ξ1+μα1xp2)+β3μ3(p+1)/2ξp+32, (3.16)

    where

    β3=p3+p(3+p9)3/pβ(3+p)/p1+13+p(p+33(p+2))(p+2)((β1+1)αp11)3+p+23+p(p+33(1+p))(1+p)/2(32β2)(3+p)/2+6c22p. (3.17)

    We choose the controller

    u=mTμ1+1/mα1ξ1μα1xp2(1+β3)μ3(p+1)/2ξp2, (3.18)

    then we get

    LV2μpξp+31μ3(p+1)/2ξp+32. (3.19)

    Now, we describe the main stability analysis results for system (2.1)–(2.2).

    Theorem 1. For the plant (2.1)–(2.2), if Assumption 1 holds, with the controller (3.18), the following conclusions are held.

    1) The plant has an almost surely unique strong solution on [t0,t0+T);

    2) The equilibrium at the origin of the plant is prescribed-time mean-square stable with limtt0+TE|x|2=0.

    Proof. By using Young's inequality we get

    14μξ41μpξp+31+β4μ3, (3.20)
    14μξ42μ3(p+1)/2ξp+32+β4μ3, (3.21)

    where

    β4=p1p+3(3+p4)4/(p1)(14)(3+p)/(p1). (3.22)

    It can be inferred from (3.19)–(3.21) that

    LV214μξ4114μξ42+2β4μ3=μV2+2β4μ3. (3.23)

    From (2.1), (2.2) and (3.18), the local Lipschitz condition is satisfied by the plant. By (3.23) and using Lemma 1 in [24], the plant has an almost surely unique strong solution on [t0,t0+T), which shows that conclusion 1) is true.

    Next, we verify conclusion 2).

    For each positive integer k, the first exit time is defined as

    ρk=inf{t:tt0,|x(t)|k}. (3.24)

    Choosing

    V=ett0μ(s)dsV2. (3.25)

    From (3.23) and (3.25) we have

    LV=ett0μ(s)ds(LV2+μV2)2β4μ3ett0μ(s)ds. (3.26)

    By (3.26) and using Dynkin's formula we get

    EV(ρkt,x(ρkt))=Vn(t0,x0)+E{ρktt0LV(x(τ),τ)dτ}Vn(t0,x0)+2β4tt0μ3eτt0μ(s)dsdτ. (3.27)

    Using Fatou Lemma, from (3.27) we have

    EV(t,x)Vn(t0,x0)+2β4tt0μ3eτt0μ(s)dsdτ,t[t0,t0+T). (3.28)

    By using (3.25) and (3.28) we get

    EV2ett0μ(s)ds(Vn(t0,x0)+2β4tt0μ3eτt0μ(s)dsdτ),t[t0,t0+T). (3.29)

    By using (3.6) and (3.29) we obtain

    limtt0+TE|x|2=0. (3.30)

    Consider the prescribed-time stabilization for the following system

    dx1=x32dt+0.1x21dω, (4.1)
    dx2=udt+0.2x1x2dω, (4.2)

    where p1=3, p2=1. Noting 0.2x1x20.1(x21+x22), Assumption 1 is satisfied.

    Choosing

    μ(t)=(11t)2,t[0,1), (4.3)

    According to the design method in Section 3, we have

    u=3μ1.5x11.5μx3257μ6(x2+1.5μx1)3 (4.4)

    In the practical simulation, we select the initial conditions as x1(0)=6, x2(0)=5. Figure 1 shows the responses of (4.1)–(4.4), from which we can obtain that limtt0+TE|x1|2=limtt0+TE|x2|2=0, which means that the controller we designed is effective.

    Figure 1.  The responses of closed-loop system (4.1)–(4.4).

    This paper proposes a new design method of prescribed-time state-feedback for SHONSs. the controller we designed can guarantee that the closed-loop system has an almost surely unique strong solution and the equilibrium at the origin of the closed-loop system is prescribed-time mean-square stable. The results in this paper are more practical than those in [13,14,15,16,17] since the design in this paper permits the worker to prescribe the convergence times in advance without considering the initial conditions.

    There are some related problems to investigate, e.g., how to extend the results to multi-agent systems [27], impulsive systems [28,29,30] or more general high-order systems [31,32,33,34].

    This work is funded by Shandong Provincial Natural Science Foundation for Distinguished Young Scholars, China (No. ZR2019JQ22), and Shandong Province Higher Educational Excellent Youth Innovation team, China (No. 2019KJN017).

    The authors declare there is no conflict of interest.



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