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Research article Special Issues

Geomatics, soft computing, and innovative simulator: prediction of susceptibility to landslide risk

  • Received: 31 December 2023 Revised: 07 April 2024 Accepted: 17 April 2024 Published: 20 May 2024
  • Landslides represent a growing threat among the various morphological processes that cause damage to territories. To address this problem and prevent the associated risks, it is essential to quickly find adequate methodologies capable of predicting these phenomena in advance. The following study focuses on the implementation of an experimental WebGIS infrastructure designed and built to predict the susceptibility index of a specific presumably at-risk area in real time (using specific input data) and in response to extreme weather events (such as heavy rain). The climate data values are calculated through an innovative and experimental atmospheric simulator developed by the authors, which is capable of providing data on meteorological variables with high spatial precision. To this end, the terrain is represented through cellular automata, implementing a suitable neural network useful for producing the desired output. The effectiveness of this methodology was tested on two debris flow events that occurred in the Calabria region, specifically in the province of Reggio Calabria, in 2001 and 2005, which caused extensive damage. The (forecast) results obtained with the proposed methodology were compared with the (known) historical data, confirming the effectiveness of the method in predicting (and therefore signaling the possibility of an imminent landslide event) a higher susceptibility index than the known one and one provided (to date) by the Higher Institute for Environmental Protection and Research (ISPRA), validating the result obtained through the actual subsequent occurrence of a landslide event in the area under investigation. Therefore, the method proposed today is not aimed at predicting the local movement of a small landslide area, but is primarily aimed at predicting the change or improving the variation of the landslide susceptibility index to compare the predicted value with the current one provided by the relevant bodies (ISPRA), thus signaling an alert for the entire area under investigation.

    Citation: Vincenzo Barrile, Emanuela Genovese, Francesco Cotroneo. Geomatics, soft computing, and innovative simulator: prediction of susceptibility to landslide risk[J]. AIMS Geosciences, 2024, 10(2): 399-418. doi: 10.3934/geosci.2024021

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  • Landslides represent a growing threat among the various morphological processes that cause damage to territories. To address this problem and prevent the associated risks, it is essential to quickly find adequate methodologies capable of predicting these phenomena in advance. The following study focuses on the implementation of an experimental WebGIS infrastructure designed and built to predict the susceptibility index of a specific presumably at-risk area in real time (using specific input data) and in response to extreme weather events (such as heavy rain). The climate data values are calculated through an innovative and experimental atmospheric simulator developed by the authors, which is capable of providing data on meteorological variables with high spatial precision. To this end, the terrain is represented through cellular automata, implementing a suitable neural network useful for producing the desired output. The effectiveness of this methodology was tested on two debris flow events that occurred in the Calabria region, specifically in the province of Reggio Calabria, in 2001 and 2005, which caused extensive damage. The (forecast) results obtained with the proposed methodology were compared with the (known) historical data, confirming the effectiveness of the method in predicting (and therefore signaling the possibility of an imminent landslide event) a higher susceptibility index than the known one and one provided (to date) by the Higher Institute for Environmental Protection and Research (ISPRA), validating the result obtained through the actual subsequent occurrence of a landslide event in the area under investigation. Therefore, the method proposed today is not aimed at predicting the local movement of a small landslide area, but is primarily aimed at predicting the change or improving the variation of the landslide susceptibility index to compare the predicted value with the current one provided by the relevant bodies (ISPRA), thus signaling an alert for the entire area under investigation.



    In [4] the authors obtained the following generalization of Montgomery identity for quantum calculus.

    Lemma 1. [4] (Quantum Montgomery identity) Let f:[a,b]R, be an arbitrary function with daqf quantum integrable on [a,b], then the following quantum identity holds:

    f(x)1babaf(t)daqt=(ba)10Kq,x(t)Daqf(tb+(1t)a)d0qt (1.1)

    where Kq,x(t) is defined by

    Kq,x(t)={qt,0txaba,qt1,xaba<t1. (1.2)

    Using this identity, the authors have obtained two Ostrowski type inequalities for quantum integrals and applied it in several special cases.

    Unfortunately, in the proof of this lemma an error is made when calculating the integrals involving the kernel Kq,x(t) on the interval [xaba,1]. Also, in the proofs of Theorem 3 and Theorem 4 a small mistake related to the convexity of |Daqf|r is made.

    In the present paper we prove that the identity (1.1) and, thus, all of the consequent results are incorrect and provide corrections for these results.

    The q-derivative of a function f:[a,b]R for q0,1 (see [5] or [2] for a=0) is given by

    Daqf(x)=f(x)f(a+q(xa))(1q)(xa),forxa,b]Daqf(a)=limxaDaqf(x)

    We say that f:[a,b]R is q-differentiable if limxaDaqf(x) exists. The q-derivative is a discretization of the ordinary derivative and if f is a differentiable function then ([1,3])

    limq1 Daqf(x)=f(x).

    Further, the q-integral of f is defined by

    xaf(t)daqt=(1q)(xa)k=0qkf(a+qk(xa)), x[a,b].

    If the series on the right hand-side is convergent, then the q-integral xaf(t)daqt exists and f:[a,b]R is said to be q-integrable on [a,x]. If f is continuous on [a,b] the series (1q)(xa)k=0qkf(a+qk(xa)) tends to the Riemann integral of f as q1 ([1], [3])

    limq1xaf(t)daqt=xaf(t)dt.

    If ca,x the q-integral is defined by

    xcf(t)daqt=xaf(t)daqtcaf(t)daqt.

    Obviously, the q-integral depends on the values of f at the points outside the interval of integration and an important difference between the definite q-integral and Riemann integral is that even if we are integrating a function over the interval [c,x], a<c<x<b, for q-integral we have to take into account its behavior at t=a as well as its values on [a,x]. This is the main reason for mistakes made in [4] since in the proof of Lemma 1 the following error was made:

    1xabaKq,x(t)Daqf(tb+(1t)a)d0qt=10(qt1)Daqf(tb+(1t)a)d0qtxaba0(qt1)Daqf(tb+(1t)a)d0qt.

    But Kq,x(t)(qt1) for t[0,1] or for t[0,xaba], so the equality does not hold.

    Now, we give a proof that the quantum Montgomery identity (1.1) is not correct, since it does not hold for all x[a,b]. As we shall see, the identity (1.1) is valid only if x=a+qm+1(ba) for some mN{0}. We have

    (ba)10Kq,x(t)Daqf(tb+(1t)a)d0qt=(ba)(1q)k=0qkKq,x(qk)Daqf(a+qk(ba)).

    For q0,1 let mN{0} be such that

    qm+1xaba<qm,

    in other words

    m=logqxaba1.

    Then

    Kq,x(qk)={qk+11,km,qk+1,km+1,

    and

    (ba)(1q)k=0qkKq,x(qk)Daqf(a+qk(ba))=(ba)(1q)(mk=0qk(qk+11)f(a+qk(ba))f(a+qk+1(ba))(1q)qk(ba)+k=m+1qk(qk+1)f(a+qk(ba))f(a+qk+1(ba))(1q)qk(ba))=mk=0(f(a+qk(ba))f(a+qk+1(ba)))+k=0qk+1(f(a+qk(ba))f(a+qk+1(ba)))=f(a+qm+1(ba))f(b)+k=0qk+1(f(a+qk(ba))f(a+qk+1(ba))).

    If we put S=k=0qkf(a+qk(ba))=1(1q)(ba)baf(t)daqt, we have

    k=0(qk+1)(f(a+qk(ba))f(a+qk+1(ba)))=qS(Sf(b))

    and

    1babaf(t)daqt+(ba)10Kq,x(t)Daqf(tb+(1t)a)d0qt=1babaf(t)daqt+(f(a+qm+1(ba))f(b))+qS(Sf(b))=(1q)S+f(a+qm+1(ba))f(b)+qSS+f(b)=f(a+qm+1(ba))

    which is obviously not equal to f(x), unless x=a+qm+1(ba).

    This is no surprise since Jackson integral takes into account only f(a+qk(xa)) for kN{0}. Thus, we have proved the next lemma which is a corrected version of Lemma 1 from [4].

    Lemma 2. (Quantum Montgomery identity) Let f:[a,b]R, be an arbitrary function with Daqf quantum integrable on [a,b], then for all xa,b the following quantum identity holds:

    f(a+qlogqxaba(ba))1babaf(t)daqt=(ba)10Kq,x(t)Daqf(tb+(1t)a)d0qt

    where Kq,x(t) is defined by

    Kq,x(t)={qt,0txaba,qt1,xaba<t1.

    In Theorem 3 and Theorem 4 from [4] the authors have used the identity (1.1) to derive Ostrowski type inequalities for functions f for which Daqf is quantum integrable on [a,b] and |Daqf|r, r1 is a convex function. Since these inequalities depends on the validity of Lemma 1, our discussion invalidates all the results from [4].

    More precisely, in all the inequalities an additional assumption x=a+qm(ba) for some mN{0} should be added. In Theorems 3 and 4 |Daqf(a)|r and |Daqf(b)|r should be swapped, since in the proofs of Theorem 3 and Theorem 4, when applying the convexity of |Daqf|r the following mistake was made

    |Daqf(tb+(1t)a)|rt|Daqf(a)|r+(1t)|Daqf(b)|r.

    Lastly, the integral K4(a,b,x,q) is incorrectly computed and should read:

    K4(a,b,x,q)=1q1+q(bxba)+q1+q(bxba)2.

    The main goal of this paper was to point out that some results in [4] are not correct. We have concentrated on Lemma 3 (Quantum Montgomery identity). The statement of that Lemma is not correct as we have shown. We also found and analyzed the mistake in the proof of Lemma 3.

    However, we went one step further and stated and proved the correct version of Lemma 3 (it is Lemma 2 in our paper). We have also explained how can all inequalities derived from Quantum Montgomery identity be corrected.

    Domagoj Kovačević was supported by the QuantiXLie Centre of Excellence, a project co financed by the Croatian Government and European Union through the European Regional Development Fund-the Competitiveness and Cohesion Operational Programme (Grant KK.01.1.1.01.0004).

    The authors declare that they have no competing interests.

    After our Correction was accepted we were contacted by the first author of [4], Professor Kunt, who suggested an alternate way to correct the results of [4].

    The incorrect version of Montgomery identity from [4]

    f(x)1babaf(t)daqt=(ba)10Kq,x(t)Daqf(tb+(1t)a)d0qt

    can be fixed in two ways: either by changing the left hand side or by changing the right hand side of this equation. In Lemma 2 we showed how to fix the identity by correcting the left hand side. This makes it easier to salvage the rest of results in [4], as all the results remain valid with the added assumption that x=a+qm(ba) for some mN{0}.

    Professor Kunt suggested correcting the right hand side of this equation to obtain the identity:

    f(x)1babaf(t)daqt=(ba)[xaba0qtDaqf(tb+(1t)a)d0qt+1xaba(qt1)Daqf(tb+(1t)a)d0qt].  ()

    By doing so, the proofs of all the remaining results have to be corrected as the bound used

    |1xaba(qt1)Daqf(tb+(1t)a)d0qt|1xaba|(qt1)Daqf(tb+(1t)a)|d0qt

    does not hold for q-integrals in general. This is discussed, for example, on page 12 in [1,Section 1.3.1,Remark (ii)].

    When xaba=qm or equivalently x=a+qm(ba) for some mN{0} the bound above does hold, which is why there is no need to change the rest of the results in [4] if one takes our approach. Nevertheless, we list below the results that can be obtained using identity (3.1). The results below are due to Professor Kunt.

    Theorem 3 in [4] should be as follows:

    Theorem 3. Let f:[a,b]R be an arbitrary function with Daqf is quantum integrable on [a,b]. If |Daqf|r, r1 is a convex function, then the following quantum integral inequality holds:

    |f(x)1babaf(t)daqt|(ba)[(11+q)11r[|Daqf(b)|r1(1+q)(1+q+q2)+|Daqf(a)|rq1+q+q2]1r+(xaba)[|Daqf(b)|r(xaba)11+q+|Daqf(a)|r(1(xaba)11+q)]1r] (3.1)

    for all x[a,b].

    Proof. Using convexity of |Daqf|r, we have that

    |Daqf(tb+(1t)a)|rt|Daqf(b)|r+(1t)|Daqf(a)|r. (3.2)

    By using (), quantum power mean inequality and (3.2), we have that

    |f(x)1babaf(t)daqt| (3.3)
    =(ba)|xaba0qtDaqf(tb+(1t)a)d0qt+1xaba(qt1)Daqf(tb+(1t)a)d0qt|=(ba)|10(qt1)Daqf(tb+(1t)a)d0qt+xaba0Daqf(tb+(1t)a)d0qt|(ba)|10(qt1)Daqf(tb+(1t)a)d0qt|+|xaba0Daqf(tb+(1t)a)d0qt|
    (ba)[10(1qt)|Daqf(tb+(1t)a)|d0qt+xaba0|Daqf(tb+(1t)a)|d0qt]
    (ba)[(101qtd0qt)11r(10(1qt)|Daqf(tb+(1t)a)|rd0qt)1r+(xaba0d0qt)11r(xaba0|Daqf(tb+(1t)a)|rd0qt)1r](ba)[(10(1qt)d0qt)11r×(|Daqf(b)|r10(1qt)td0q+|Daqf(a)|r10(1qt)(1t)d0qt)1r+(xaba0d0qt)11r×(|Daqf(b)|rxaba0td0qt+|Daqf(a)|rxaba0(1t)d0qt)1r]

    On the other hand, calculating the following quantum integrals we have

    10(1qt)d0qt=(1q)n=0qn(1qn+1)=(1q)[11qq1q2]=11+q, (3.4)
    10(1qt)td0qt=(1q)n=0qn[(1qn+1)qn]=(1q)[11q2q1q3]=11+qq1+q+q2=1(1+q)(1+q+q2), (3.5)
    10(1qt)(1t)d0qt=101qtd0qt10(1qt)td0qt=11+q1(1+q)(1+q+q2)=q1+q+q2, (3.6)
    xaba0d0qt=(1q)(xaba)n=0qn=xaba, (3.7)
    xaba0td0qt=(1q)(xaba)n=0qn(qn(xaba))=(xaba)211+q, (3.8)
    xaba0(1t)d0qt=xaba0d0qtxaba0td0qt=xaba(xaba)211+q=(xaba)[1(xaba)11+q]. (3.9)

    Using (3.4)–(3.9) in (3.3), we have (3.1).

    Theorem 4 in [4] should be as follows:

    Theorem 4. Let f:[a,b]R be an arbitrary function with Daqf is quantum integrable on [a,b]. If |Daqf|r, r>1 and 1r+1p=1 is convex function, then the following quantum integral inequality holds:

    |f(x)1babaf(t)daqt| (3.10)
    (ba)[(10(1qt)pd0qt)1p(|Daqf(b)|r11+q+|Daqf(a)|rq1+q)1r+(xaba)[|Daqf(b)|r(xaba)11+q+|Daqf(a)|r(1(xaba)11+q)]1r]

    for all x[a,b].

    Proof. By using () and quantum Hölder inequality, we have

    |f(x)1babaf(t)daqt|(ba)|10(qt1)Daqf(tb+(1t)a)d0qt|+|xaba0Daqf(tb+(1t)a)d0qt|(ba)[10(1qt)|Daqf(tb+(1t)a)|d0qt+xaba0|Daqf(tb+(1t)a)|d0qt](ba)[(10(1qt)pd0qt)1p(10|Daqf(tb+(1t)a)|rd0qt)1r+(xaba0d0qt)1p(xaba0|Daqf(tb+(1t)a)|rd0qt)1r](ba)[(10(1qt)pd0qt)1p(10[t|Daqf(b)|r+(1t)|Daqf(a)|r]d0qt)1r+(xaba0d0qt)1p(xaba0[t|Daqf(b)|r+(1t)|Daqf(a)|r]d0qt)1r](ba)[(10(1qt)pd0qt)1p(|Daqf(b)|r10td0qt+|Daqf(a)|r10(1t)d0qt)1r+(xaba0d0qt)1p(|Daqf(b)|rxaba0td0qt+|Daqf(a)|rxaba0(1t)d0qt)1r]=(ba)[(10(1qt)pd0qt)1p(|Daqf(b)|r11+q+|Daqf(a)|rq1+q)1r+(xaba)[|Daqf(b)|r(xaba)11+q+|Daqf(a)|r(1(xaba)11+q)]1r].

    We conclude this section by noting that the bounds obtained in the original paper [4] which, as we have previously shown, do hold with the added assumption x=a+qm(ba) for some mN{0}, are tighter than the bounds obtained above by Professor Kunt. Professor Kunt's bounds, however, hold for all x[a,b].



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