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Derivation of dynamical integral inequalities based on two-dimensional time scales theory


The main goal of this paper is to set up some new estimates of a specific class of dynamic integral inequalities (DII) which are partially linear on a time scale \(\mathbb{T}\) with two independent variables. These, from the one hand, sum up and, on the other hand, offer a helpful method for both the qualitative and quantitative study of dynamic equations on time scales. Some applications are taken into consideration to show the validity of the fundamental results.

1 Introduction

Differential and integral inequalities have ended up being valuable instruments in investigating the differential and integral equations that are constructed by numerous analysts (see [117]). The analysis of the theory of time-scale dynamic equations, which goes back to its author Hilger [18], is a recent field of mathematics that has gained much interest. The trendy thought is to demonstrate an equation for a dynamic circumstance or a dynamic inequality wherein the area of the unknown characteristic is a presumed time scale \(\mathbb{T}\). The justification for considering time scales is to unify continuous and discrete inspection. Among diverse aspects of the concept, we observe that dynamic inequalities increase and unify different views of both difference and differential equations in an anticipated mode; see [1921] and the references therein. Pachpatte [22] initially unifies the existing fundamental inequality

$$ x(r)\leq b(r)+ \int _{r_{0}}^{r} h(u)x(u)\Delta u, \quad r\in \mathbb{T}, $$

provided with x, h being right-dense continuous functions, \(x\geq 0\).

After that in 2009, Li [23] achieved an integral inequality of the form

$$ x(r)\leq x_{0}+ \int _{r_{0}}^{r} \bigl[h(u)x(u)+m(u) \bigr]\Delta u+ \int _{r_{0}}^{r}g(u) \bigl[z(u,l)x(l)\Delta l \bigr] \Delta u, $$

where \(z(u,l)\geq 0\), \(z^{\Delta }(u,l)\geq 0\) for \(r,l\in \mathbb{T}\) and \(l\leq r\). Recently, Sun and Hassan [24] discovered a nonlinear integral inequality related to time scales given by

$$ x(r)\leq b(r)+j(r) \int _{r_{0}}^{r} \bigl[h(u)x(u)+g(u)x^{\xi } \bigl(\sigma (u)\bigr)-z(u)x^{ \psi }\bigl(\sigma (u)\bigr) \bigr]\Delta u, $$

where \(b, j, h, g, z:\mathbb{T}^{\kappa }\rightarrow \mathbb{R}_{+}\) are rd-continuous functions and \(\xi, \psi \) are positive constants with \(0<\xi <1<\psi \).

During the last couple of years, many researchers have proved a few integral inequalities utilizing dynamic time scale equations [2529]. In light of the above work, we proceed with our examination to acquire some new two-dimensional integral inequalities that are partially linear on time scales. The obtained results additionally supply a reachable device for the look at qualitative properties of solutions of integral and dynamic equations.

The rest of the paper is composed as follows. In Sect. 2, we describe principal relations and tentative lemmas that are strategic guides for our principle results. The hypothetical discussions with finishing up corollaries and remarks are gathered in Sect. 3. The last section is considered to delineate the uses of the theoretical investigations.

2 Essentials and lemmas on time scales

Without loss of generality, at some point of in this work, let time scales \(T^{\ast }\) and \(T^{\diamond }\) with delta differentiation operators \(\sigma _{1}, \sigma _{2}\) and \(\Delta _{1}, \Delta _{2}\) respectively, contain at least two points \(\zeta _{0},\xi \in T^{\ast }\), \(r_{0},\psi \in T^{\diamond }\), \(\xi >\zeta _{0}\), \(\psi >r_{0}\), \(T^{\ast }_{1}=[\zeta _{0},\infty )\cap T^{\ast }\), \(T^{\diamond }_{1}=[r_{0},\infty )\cap T^{\diamond }\), \(\varUpsilon =T^{\ast }\times T^{\diamond }\); \(x^{\Delta _{1}}(\zeta,r)\), \(x^{\Delta _{2}}(\zeta,r)\), and \(x^{\Delta _{1} \Delta _{2}}(\zeta,r) = x^{\Delta _{2} \Delta _{1}}(\zeta,r)\) are the delta derivatives of a function \(x(\zeta,r)\) with respect to \(\zeta,r\), and pr, respectively, for \(\zeta,r \in \mathbb{R}\); \(\mathbb{R}\) stands for the set of real numbers, \(\mathbb{R}_{+}=[0,\infty )\), \(j_{0}\in \mathbb{T}_{k}\), \(\mathbb{T}\in \mathbb{T}^{k}\), \(\mathbb{T}>\zeta _{0}\), \(C_{rd}\) is the set of all rd-continuous functions, defines the set of all regressive and rd-continuous functions and \(\Re ^{+}= \{ x\in \Re: 1+\varsigma (\zeta )x(\zeta )>0, \zeta \in \mathbb{T} \} \), \((x\oplus c)(\zeta ):=x(\zeta )+c(\zeta )+\varsigma (\zeta )x(\zeta )c( \zeta )\) for all \(\zeta \in \mathbb{T}^{k}\). On time scales, the user is supposed to be comfortable with the theory and basic ideas regarding the analytics. The monograph [30] is recommended for further details of time scale ideology.

Some important lemmas in this paper are as follows:

Lemma 2.1


Let \(\zeta _{0}\in \mathbb{T}^{k}\)and \(\varPi :\mathbb{T}\times \mathbb{T}^{k} \rightarrow \mathbb{R}\)be continuous at \((\zeta,\zeta )\), where \(\zeta >\zeta _{0}\)and \(\zeta \in \mathbb{T}^{k}\). Assume that \(\varPi ^{\Delta }(\zeta,\cdot )\)is rd-continuous on \([\zeta _{0},\sigma (\zeta )]_{\mathbb{T}}\)and for every \(\epsilon >0\), a neighborhood \(\varSigma ^{\ast }\)of ζ, independent of \(a\in [\zeta _{0},\sigma (\zeta )]_{\mathbb{T}}\), such that

$$ \bigl\vert \bigl[\varPi \bigl(\sigma (\zeta ),\eta \bigr)-\varPi (s,a)\bigr]- \varPi ^{\Delta }(\zeta,a)\bigl[ \sigma (\zeta )-s\bigr] \bigr\vert \leq \epsilon \bigl\vert \sigma (\zeta )-s \bigr\vert ,\quad s\in \varSigma ^{\ast }, $$

where \(\varPi ^{\Delta }\)symbolizes the derivative of Π w.r.t. the first variable, and so

$$ x(\zeta )= \int _{\zeta _{0}}^{\zeta }\varPi (\zeta,a)\Delta a $$


$$ x^{\Delta }(\zeta )= \int _{\zeta _{0}}^{\zeta }\varPi ^{\Delta }(\zeta,a) \Delta a+\varPi \bigl(\sigma (\zeta ),\zeta \bigr). $$

Lemma 2.2


Let \(z^{\ast }>0\), \(c^{\ast }>0\), \(\xi >0\), \(\psi >0\)be given, then for each \(x\geq 0\),

$$ zx^{\xi }-cx^{\psi }\leq \frac{z(\psi -\xi )}{(\psi -1)} \biggl( \frac{(\psi -1)c}{(\xi -1)z} \biggr)^{\frac{\xi -1}{\xi -\psi }}x $$

holds for the cases \(1<\xi <\psi \)or \(0<\psi <\xi <1\).

Lemma 2.3


Suppose \(x, z\in C_{rd}\), \(c\in \mathbb{R}_{+}\). Then

$$ x^{\Delta }(\zeta )\leq z(\zeta )x(\zeta )+c(\zeta ),\quad \zeta \in \mathbb{T}, $$


$$ x(\zeta )\leq x(\zeta _{0})e_{z}(\zeta,\zeta _{0})+ \int _{\zeta _{0}}^{ \zeta }e_{z}\bigl(\zeta,\sigma (a) \bigr)c(a)\Delta a,\quad \zeta \in \mathbb{T}. $$

Lemma 2.4


Assume that \(x, z, c\in C_{rd}([\zeta _{0},\infty )_{\mathbb{T}}, \mathbb{R}_{+})\), where z is nondecreasing and not identically zero. If

$$ x(\zeta )\leq z(\zeta )+ \int _{\zeta _{0}}^{\zeta }c(s)x(s)\Delta s,\quad \zeta \in [\zeta _{0},\infty )_{\mathbb{T}}, $$


$$ x(\zeta )\leq z(j)e_{c}(\zeta,\zeta _{0}),\quad \zeta \in [r_{0}, \infty )_{\mathbb{T}}. $$

3 Dynamic integral inequalities (DII) in two dimensions

Now we state and demonstrate our primary results:

Theorem 3.1

Suppose \(x, y, l, t, u, m\in C_{rd}(\varUpsilon,\mathbb{R}_{+})\), \(z, c\in C_{rd}(\varUpsilon, (0,\infty ))\), y is nondecreasing and not identically zero, \(\xi, \psi \)are positive constants, \(1<\xi <\psi \)or \(0<\psi <\xi <1\). Moreover, \(m\in C_{rd}(\varUpsilon,\mathbb{R}_{+})\)is nondecreasing in ζ, Π is defined as in Lemma 2.1such that \(\varPi ^{\Delta _{1}}(\zeta,r,o,\varrho )\geq 0\), \(\varPi ^{\Delta _{2}\Delta _{1}}(\zeta,r,o,\varrho )\geq 0\)for \(\zeta \geq o, r\geq \varrho \)and

$$\begin{aligned} x(\zeta,r)\leq{}& y(\zeta,r)+ \int _{\zeta _{0}}^{\zeta } \int _{r_{0}}^{r}l(o, \varrho )x(o,\varrho )\Delta \varrho \Delta o \\ &{}+t(\zeta,r) \int _{\zeta _{0}}^{\zeta } \int _{r_{0}}^{r}\varPi (\zeta,r,o, \varrho ) \bigl[u(o, \varrho )x(o,\varrho )+z(o,\varrho )x^{\xi }\bigl( \sigma (o),\varrho \bigr) \\ &{}-c(o,\varrho )x^{\psi }\bigl(\sigma (o),\varrho \bigr) \bigr] \Delta \varrho \Delta o \\ &{}+ \int _{\zeta _{0}}^{S}m(o,r)x(o,r)\Delta o, \quad (\zeta,r)\in \varUpsilon, \end{aligned}$$

provided with

$$ \mu (\zeta,r)\varTheta (\zeta,r)< 1,\qquad \int _{\zeta _{0}}^{S}m(o,r)e_{V \oplus W}(o,\zeta _{0})\Delta o< 1. $$


$$\begin{aligned} x(\zeta,r)\leq{}& y(\zeta,r)+ \frac{\int _{\zeta _{0}}^{S}m(o,r) [y(o,r)+\int _{\zeta _{0}}^{o}e_{V\oplus W}(o,\sigma (\tau ))D(\tau,r)\Delta \tau ]\Delta o}{1-\int _{\zeta _{0}}^{S}m(o,r)e_{V\oplus W}(o,\zeta _{0})\Delta o}e_{V \oplus W}( \zeta,\zeta _{0}) \\ &{}+ \int _{\zeta _{0}}^{S}m(o,r)e_{V\oplus W}\bigl(\tau, \sigma (o)\bigr)\Delta o, \end{aligned}$$


$$\begin{aligned} \varTheta (\zeta,r)={}&t^{\Delta _{1}}(\zeta,r) \int _{\zeta _{0}}^{ \sigma (\zeta )} \int _{r_{0}}^{r}\varPi \bigl(\sigma (\zeta ),r,o, \varrho \bigr) \bigl(u(o,\varrho )+H(o,\varrho ) \bigr)\Delta \varrho \Delta o \\ &{}+t(\zeta,r) \int _{\zeta _{0}}^{\zeta } \int _{r_{0}}^{r}\varPi ^{\Delta _{2} \Delta _{1}}(\zeta,r,o, \varrho )H(o,\varrho )\Delta \varrho \Delta o \\ &{}+ \int _{r_{0}}^{r}\varPi ^{\Delta _{1}}\bigl(\sigma ( \zeta ),r,\zeta,\varrho \bigr)H( \zeta,\varrho )\Delta \varrho, \end{aligned}$$
$$\begin{aligned} W(\zeta,r)={}& \int _{r_{0}}^{r}l(\zeta,\varrho )\Delta \varrho +t( \zeta,r) \int _{\zeta _{0}}^{\zeta } \int _{r_{0}}^{r}\varPi ^{\Delta _{2} \Delta _{1}}(\zeta,r,o, \varrho )u(o,\varrho )\Delta \varrho \Delta o \\ &{}+ \int _{r_{0}}^{r}\varPi ^{\Delta _{1}}\bigl(\sigma ( \zeta ),r,\zeta,\varrho \bigr)u( \zeta,\varrho )\Delta \varrho, \end{aligned}$$
$$\begin{aligned} \eta (\zeta,r)={}& \int _{r_{0}}^{r}l(\zeta,\varrho )y(\zeta,\varrho ) \Delta \varrho +t^{\Delta _{1}}(\zeta,r) \int _{\zeta _{0}}^{\sigma (j)} \int _{r_{0}}^{r}\varPi \bigl(\sigma (\zeta ),r,o, \varrho \bigr) \bigl(u(o,\varrho )y(o, \varrho ) \\ &{}+H(o,\varrho )y\bigl(\sigma (o), \varrho \bigr) \bigr)\Delta \varrho \Delta o \\ &{}+t(\zeta,r) \int _{\zeta _{0}}^{\zeta } \int _{r_{0}}^{r}\varPi ^{\Delta _{2} \Delta _{1}}(\zeta,r,o, \varrho ) \bigl(u(o,\varrho )y(o,\varrho )+H(o, \varrho )y\bigl(\sigma (o),\varrho \bigr) \bigr) \Delta \varrho \Delta o \\ &{}+ \int _{r_{0}}^{r}\varPi ^{\Delta _{1}}\bigl(\sigma ( \zeta ),r,\zeta, \varrho \bigr) \bigl(u(\zeta,\varrho )y(\zeta,\varrho )+H(\zeta, \varrho )y\bigl( \sigma (\zeta ),\varrho \bigr) \bigr)\Delta \varrho, \end{aligned}$$
$$\begin{aligned} H(\zeta,r)={}&\frac{z(\zeta,r)(\psi -\xi )}{(\psi -1)} \biggl( \frac{(\psi -1)c(\zeta,r)}{(\xi -1)z(\zeta,r)} \biggr)^{ \frac{\xi -1}{\xi -\psi }}, \end{aligned}$$
$$\begin{aligned} V(\zeta,r)={}& \frac{\varTheta (\zeta,r)}{1-\mu (\zeta,r) \varTheta (\zeta,r)}, D( \zeta,r)=\bigl(1+\mu (\zeta,r) V(\zeta,r)\bigr)\eta (\zeta,r). \end{aligned}$$


Employing Lemma 2.2 in (1), we get

$$\begin{aligned} x(\zeta,r)\leq{}& y(\zeta,r)+ \int _{\zeta _{0}}^{\zeta } \int _{r_{0}}^{r}l(o, \varrho )x(o,\varrho )\Delta \varrho \Delta o \\ &{}+t(\zeta,r) \int _{\zeta _{0}}^{\zeta } \int _{r_{0}}^{r}\varPi (\zeta,r,o, \varrho ) \bigl[u(o, \varrho )x(o,\varrho )+H(o,\varrho )x\bigl(\sigma (o), \varrho \bigr) \bigr]\Delta \varrho \Delta o \\ &{}+ \int _{\zeta _{0}}^{S}m(o,r)x(o,r)\Delta o, \\ \leq{}& y(\zeta,r)+A(\zeta,r), \end{aligned}$$

where \(H(\zeta,r)\) is as in (7) and a nondecreasing function \(A(\zeta,r)\) is defined by

$$\begin{aligned} A(\zeta,r)={}& \int _{\zeta _{0}}^{\zeta } \int _{r_{0}}^{r}l(o,\varrho )x(o, \varrho )\Delta \varrho \Delta o \\ &{}+t(\zeta,r) \int _{\zeta _{0}}^{\zeta } \int _{r_{0}}^{r}\varPi (\zeta,r,o, \varrho ) \bigl[u(o, \varrho )x(o,\varrho )+H(o,\varrho )x\bigl(\sigma (o), \varrho \bigr) \bigr]\Delta \varrho \Delta o \\ &{}+ \int _{\zeta _{0}}^{S}m(o,r)x(o,r)\Delta o \end{aligned}$$


$$ A(\zeta _{0},r)= \int _{\zeta _{0}}^{S}m(o,r)x(o,r)\Delta o. $$

From Lemma 2.1 and by using the delta derivative (10) with respect to j, we deduce

$$\begin{aligned} &A^{\Delta _{1}}(\zeta,r)\\ &\quad \leq \int _{r_{0}}^{r}l(\zeta,\varrho )x( \zeta,\varrho ) \Delta \varrho \\ &\qquad{}+t^{\Delta _{1}}(\zeta,r) \int _{\zeta _{0}}^{\sigma (\zeta )} \int _{r_{0}}^{r} \varPi \bigl(\sigma (\zeta ),r,o, \varrho \bigr) \bigl[u(o,\varrho )x(o,\varrho )+H(o, \varrho )x\bigl(\sigma (o), \varrho \bigr) \bigr]\Delta \varrho \Delta a \\ &\qquad{}+t(\zeta,r) \int _{\zeta _{0}}^{\zeta } \int _{r_{0}}^{r}\varPi ^{\Delta _{2} \Delta _{1}}(\zeta,r,o, \varrho ) \bigl[u(o,\varrho )x(o,\varrho )+H(o, \varrho )x\bigl(\sigma (o),\varrho \bigr) \bigr]\Delta \varrho \Delta a \\ &\qquad{}+t(\zeta,r) \int _{r_{0}}^{r}\varPi ^{\Delta _{1}}\bigl(\sigma ( \zeta ),r, \zeta,\varrho \bigr) \bigl[u(\zeta,\varrho )x(\zeta,\varrho )+H(\zeta, \varrho )x\bigl(\sigma (\zeta ),\varrho \bigr) \bigr]\Delta \varrho, \end{aligned}$$

where, using (9) in the last inequality, we get

$$\begin{aligned} A^{\Delta _{1}}(\zeta,r)\leq{}& \int _{r_{0}}^{r}l(\zeta,\varrho ) \bigl(y(\zeta,\varrho )+A(\zeta,\varrho ) \bigr)\Delta v \\ &{}+t^{\Delta _{1}}(\zeta,r) \int _{\zeta _{0}}^{\sigma (\zeta )} \int _{r_{0}}^{r} \varPi \bigl(\sigma (\zeta ),r,o, \varrho \bigr) \bigl[u(o,\varrho ) \bigl(y(o, \varrho ) +A(o,\varrho ) \bigr) \\ &{}+H(o, \varrho ) \bigl(y\bigl(\sigma (o), \varrho \bigr)+A\bigl(\sigma (o),\varrho \bigr) \bigr) \bigr]\Delta \varrho \Delta o \\ &{}+t(\zeta,r) \int _{\zeta _{0}}^{\zeta } \int _{r_{0}}^{r}\varPi ^{\Delta _{2} \Delta _{1}}(\zeta,r,o, \varrho ) \bigl[u(o,\varrho ) \bigl(y(o,\varrho )+A(o, \varrho ) \bigr) \\ &{}+H(o, \varrho ) \bigl(y\bigl(\sigma (o),\varrho \bigr)+A\bigl(\sigma (o), \varrho \bigr) \bigr) \bigr]\Delta \varrho \Delta o \\ &{}+t(\zeta,r) \int _{r_{0}}^{r}\varPi ^{\Delta _{1}}\bigl(\sigma ( \zeta ),r, \zeta,\varrho \bigr) \bigl[u(\zeta,\varrho ) \bigl(y(\zeta,\varrho )+A( \zeta,\varrho ) \bigr) \\ &{}+H(\zeta,\varrho ) \bigl(y\bigl(\sigma (\zeta ), \varrho \bigr)+A\bigl(\sigma (\zeta ),\varrho \bigr) \bigr) \bigr]\Delta \varrho, \end{aligned}$$

so that

$$\begin{aligned} &A^{\Delta _{1}}(\zeta,r)\\ &\quad \leq \int _{r_{0}}^{r}l(\zeta,\varrho )y( \zeta,\varrho ) \Delta \varrho + \int _{r_{0}}^{r}l(\zeta,\varrho )A( \zeta,\varrho ) \Delta \varrho \\ &\qquad{}+t^{\Delta _{1}}(\zeta,r) \int _{\zeta _{0}}^{\sigma (\zeta )} \int _{r_{0}}^{r} \varPi \bigl(\sigma (\zeta ),r,o, \varrho \bigr) \bigl[u(o,\varrho )y(o,\varrho )+H(o, \varrho )y\bigl(\sigma (o), \varrho \bigr) \bigr]\Delta \varrho \Delta o \\ &\qquad{}+A\bigl(\sigma (\zeta ),r\bigr) \biggl[t^{\Delta _{1}}(\zeta,r) \int _{\zeta _{0}}^{ \sigma (\zeta )} \int _{r_{0}}^{r}\varPi \bigl(\sigma (\zeta ),r,o, \varrho \bigr) \bigl(u(o,\varrho )+H(o,\varrho ) \bigr)\Delta \varrho \Delta o \biggr] \\ &\qquad{}+t(\zeta,r) \int _{\zeta _{0}}^{\zeta } \int _{r_{0}}^{r}\varPi ^{\Delta _{2} \Delta _{1}}(p,r,o,v) \bigl[u(o,\varrho )y(o,\varrho )+H(o,\varrho )y\bigl( \sigma (o),\varrho \bigr) \bigr]\Delta \varrho \Delta o \\ &\qquad{}+t(\zeta,r) \int _{\zeta _{0}}^{\zeta } \int _{r_{0}}^{r}\varPi ^{\Delta _{2} \Delta _{1}}(\zeta,r,o, \varrho )u(o,\varrho )A(o,\varrho )\Delta \varrho \Delta o \\ &\qquad{}+t(\zeta,r) \int _{\zeta _{0}}^{\zeta } \int _{r_{0}}^{r}\varPi ^{\Delta _{2} \Delta _{1}}(\zeta,r,o, \varrho )H(o,\varrho )A\bigl(\sigma (o),\varrho \bigr) \Delta \varrho \Delta o \\ &\qquad{}+t(\zeta,r) \int _{r_{0}}^{r}\varPi ^{\Delta _{1}}\bigl(\sigma ( \zeta ),r, \zeta,\varrho \bigr) \bigl[u(\zeta,\varrho )y(\zeta,\varrho )+H(\zeta, \varrho )y\bigl(\sigma (\zeta ),\varrho \bigr) \bigr]\Delta \varrho \\ &\qquad{}+t(\zeta,r) \int _{r_{0}}^{r}\varPi ^{\Delta _{1}}\bigl(\sigma ( \zeta ),r, \zeta,\varrho \bigr)u(\zeta,\varrho )A(\zeta,\varrho )\Delta \varrho \\ &\qquad{}+t(\zeta,r) \int _{r_{0}}^{r}\varPi ^{\Delta _{1}}\bigl(\sigma ( \zeta ),r, \zeta,\varrho \bigr)H(\zeta,\varrho )A\bigl(\sigma (\zeta ),\varrho \bigr)\Delta \varrho, \end{aligned}$$

which leads to

$$\begin{aligned} &A^{\Delta _{1}}(\zeta,r) \\ &\quad \leq\biggl[t^{\Delta _{1}}(\zeta,r) \int _{ \zeta _{0}}^{\sigma (\zeta )} \int _{r_{0}}^{r}\varPi \bigl(\sigma (\zeta ),r,o, \varrho \bigr) \bigl(u(o,\varrho )+H(o,\varrho ) \bigr)\Delta \varrho \Delta o \\ &\qquad{}+t(\zeta,r) \int _{\zeta _{0}}^{\zeta } \int _{r_{0}}^{r}\varPi ^{\Delta _{2} \Delta _{1}}(\zeta,r,o, \varrho )H(o,\varrho )\Delta \varrho \Delta o \\ &\qquad{}+t(\zeta,r) \int _{r_{0}}^{r}\varPi ^{\Delta _{1}}\bigl(\sigma ( \zeta ),r, \zeta,\varrho \bigr)H(\zeta,\varrho )\Delta \varrho \biggr] A\bigl( \sigma ( \zeta ),\varrho \bigr) \\ &\qquad{}+ \biggl[ \int _{r_{0}}^{r}l(\zeta,\varrho )\Delta \varrho +t( \zeta,r) \int _{\zeta _{0}}^{\zeta } \int _{r_{0}}^{r}\varPi ^{\Delta _{2}\Delta _{1}}( \zeta,r,o, \varrho )u(o,\varrho )\Delta \varrho \Delta o \\ &\qquad{}+t(\zeta,r) \int _{r_{0}}^{r}\varPi ^{\Delta _{1}}\bigl(\sigma ( \zeta ),r, \zeta,\varrho \bigr)u(\zeta,\varrho )\Delta \varrho \biggr]A(\zeta,r)+ \int _{r_{0}}^{r}l(\zeta,\varrho )y(\zeta,\varrho ) \Delta \varrho \\ &\qquad{}+t^{\Delta _{1}}(\zeta,r) \int _{\zeta _{0}}^{\sigma (\zeta )} \int _{r_{0}}^{r} \varPi \bigl(\sigma (\zeta ),r,o, \varrho \bigr) \bigl[u(o,\varrho )y(o,\varrho )+H(o, \varrho )y\bigl(\sigma (o), \varrho \bigr) \bigr]\Delta \varrho \Delta o \\ &\qquad{}+t(\zeta,r) \int _{\zeta _{0}}^{\zeta } \int _{r_{0}}^{r}\varPi ^{\Delta _{2} \Delta _{1}}(\zeta,r,o, \varrho ) \bigl[u(o,\varrho )y(o,\varrho )+H(o, \varrho )y\bigl(\sigma (o),\varrho \bigr) \bigr]\Delta \varrho \Delta o \\ &\qquad{}+t(\zeta,r) \int _{r_{0}}^{r}\varPi ^{\Delta _{1}}\bigl(\sigma ( \zeta ),r, \zeta,\varrho \bigr) \bigl[u(\zeta,\varrho )y(\zeta,\varrho )+H(\zeta, \varrho )y\bigl(\sigma (\zeta ),\varrho \bigr) \bigr]\Delta \varrho \\ &\quad\leq \varTheta (\zeta,r)A\bigl(\sigma (\zeta ),r\bigr)+W(\zeta,r)A(\zeta,r)+ \eta (\zeta,r), \end{aligned}$$

with \(\varTheta (\zeta,r)\), \(W(\zeta,r)\), \(\eta (\zeta,r)\) defined as in (4), (5), and (6). From (8), we obtain

$$ \varTheta (\zeta,r)=\frac{V(\zeta,r)}{1+\mu (\zeta,r)V(\zeta,r)}. $$

In view of (12) and (13), we obtain

$$\begin{aligned} A^{\Delta _{1}}(\zeta,r)&\leq \varTheta (\zeta,r) \bigl(A(\zeta,r)+ \mu ( \zeta,r)A^{\Delta _{1}}(\zeta,r) \bigr)+W(\zeta,r)A(\zeta,r)+ \eta (\zeta,r) \\ &\leq \frac{V(\zeta,r)}{1+\mu (\zeta,r)V(\zeta,r)} \bigl(A(\zeta,r)+ \mu (\zeta,r)A^{\Delta _{1}}(\zeta,r) \bigr)+W(\zeta,r)A(\zeta,r)+ \eta (\zeta,r), \end{aligned}$$

which yields

$$ \frac{1}{1+\mu (\zeta,r)V(\zeta,r)}A^{\Delta _{1}}(\zeta,r)\leq \frac{V(\zeta,r)+W(\zeta,r)+\mu (\zeta,r) V(\zeta,r)W(\zeta,r)}{1+\mu (\zeta,r)V(\zeta,r)}A( \zeta,r)+\eta (\zeta,r), $$


$$\begin{aligned} A^{\Delta _{1}}(\zeta,r)\leq {}&\bigl(V(\zeta,r)+W(\zeta,r)+\mu ( \zeta,r) V(\zeta,r)W(\zeta,r) \bigr)A(\zeta,r) \\ &{}+ \bigl(1+\mu (\zeta,r)V( \zeta,r) \bigr)\eta (\zeta,r) \\ \leq{}& (V\oplus W) (\zeta,r)A(\zeta,r)+D(\zeta,r). \end{aligned}$$

Here \(D(\zeta,r)\) is as in (8). As we know that \(A(\zeta,r)\) is rd-continuous and \(V\oplus W\in \Re ^{+}\). Therefore, inequality (14) with the use of Lemma 2.3 and (11) implies the estimate

$$ A(\zeta,r)\leq A(\zeta _{0},r)e_{V\oplus W}(\zeta, \zeta _{0})+ \int _{ \zeta _{0}}^{\zeta }e_{V\oplus W}\bigl(\tau,\sigma (o) \bigr)D(o,r)\Delta o. $$

Substituting (9) and (15) on the right side of (11), we have

$$ A(\zeta _{0},r)\leq \frac{\int _{\zeta _{0}}^{S}m(o,r) [y(o,r)+\int _{\zeta _{0}}^{o}e_{V\oplus W}(o,\sigma (\tau ))D(\tau,r)\Delta \tau ) ]\Delta o}{1-\int _{\zeta _{0}}^{S}m(o,r)e_{V\oplus W}(o,\zeta _{0})\Delta o}, $$

and, from (9), (15), and (16), we get the required bound in (3). □

A useful corollary of Theorem 3.1 with \(m(\zeta,r)=0\) can be obtained as follows:

Corollary 3.2

Under the same assumptions on \(x, y, l,t, u, z, c, \xi, \psi, \varPi, \varTheta, V, W, \eta \), and H in Theorem 3.1, the inequality

$$\begin{aligned} &x(\zeta,r) \\ &\quad \leq y(\zeta,r)+ \int _{\zeta _{0}}^{\zeta } \int _{r_{0}}^{r}l(o, \varrho )x(o,\varrho )\Delta \varrho \Delta o +t(\zeta,r) \int _{ \zeta _{0}}^{\zeta } \int _{r_{0}}^{r}\varPi (\zeta,r,o,\varrho ) \\ &\qquad{}\times \bigl[u(o,\varrho )x(o,\varrho )+z(o,\varrho )x^{\xi }\bigl( \sigma (o), \varrho \bigr)-c(o,\varrho )x^{\psi }\bigl(\sigma (o),\varrho \bigr) \bigr]\Delta \varrho \Delta o,\quad (\zeta,r)\in \varUpsilon, \end{aligned}$$


$$\begin{aligned} x(\zeta,r)\leq y(\zeta,r)+ \int _{\zeta _{0}}^{\zeta }e_{V\oplus W}\bigl( \tau,\sigma (o) \bigr)D(o,r)\Delta o, \end{aligned}$$

If \(\varPi (\zeta,r,o,\varrho )=1\) in Theorem 3.1, we can produce the following corollary:

Corollary 3.3

Suppose that \(x, y, l,t, u, m, z, c, \xi, \psi \)and H are same as in Theorem 3.1. If

$$\begin{aligned} x(\zeta,r)\leq{}& y(\zeta,r)+ \int _{\zeta _{0}}^{\zeta } \int _{r_{0}}^{r}l(o, \varrho )x(o,\varrho )\Delta \varrho \Delta o \\ &{}+t(\zeta,r) \int _{\zeta _{0}}^{\zeta } \int _{r_{0}}^{r} \bigl[u(o, \varrho )x(o,\varrho )+z(o, \varrho )x^{\xi }\bigl(\sigma (o),\varrho \bigr)-c(o, \varrho )x^{\psi }\bigl(\sigma (o),\varrho \bigr) \bigr]\Delta \varrho \Delta o \\ &{}+ \int _{\zeta _{0}}^{S}m(o,r)x(o,r)\Delta o, \quad(\zeta,r)\in \varUpsilon, \end{aligned}$$


$$\begin{aligned} x(\zeta,r)\leq{}& y(\zeta,r)+ \frac{\int _{\zeta _{0}}^{S}m(a,r) [y(o,r)+\int _{\zeta _{0}}^{o}e_{V_{1}\oplus W_{1}}(o,\sigma (\tau ))D_{1}(\tau,r)\Delta \tau ]\Delta o}{1-\int _{\zeta _{0}}^{S}m(o,r)e_{V_{1}\oplus W_{1}}(o,\zeta _{0})\Delta o}e_{V_{1} \oplus W_{1}}(\zeta,\zeta _{0}) \\ &{}+ \int _{\zeta _{0}}^{S}m(o,r)e_{V_{1}\oplus W_{1}}\bigl(\tau, \sigma (o)\bigr) \Delta o, \end{aligned}$$

where \(V_{1}(\zeta,r)= \frac{\varTheta _{1}(\zeta,r)}{1-\mu (\zeta,r) \varTheta _{1}(\zeta,r)}, D_{1}(\zeta,r)=(1+\mu (\zeta,r) V_{1}(\zeta,r))\eta _{1}( \zeta,r)\),

$$\begin{aligned} &\varTheta _{1}(\zeta,r)=t^{\Delta _{1}}(\zeta,r) \int _{\zeta _{0}}^{ \sigma (\zeta )} \int _{r_{0}}^{r} \bigl(u(o,\varrho )+H(o,\varrho ) \bigr)\Delta \varrho \Delta o+t(\zeta,r) \int _{r_{0}}^{r}H(\zeta, \varrho )\Delta \varrho, \\ &W_{1}(\zeta,r)= \int _{r_{0}}^{r}l(\zeta,\varrho )\Delta \varrho +t( \zeta,r) \int _{r_{0}}^{r}u(\zeta,\varrho )\Delta \varrho, \\ &\eta _{1}(\zeta,r)= \int _{r_{0}}^{r}l(\zeta,\varrho )y(\zeta, \varrho ) \Delta v\varrho \\ &\phantom{\eta _{1}(\zeta,r)=}{}+t^{\Delta _{1}}(\zeta,r) \int _{\zeta _{0}}^{ \sigma (\zeta )} \int _{r_{0}}^{r} \bigl(u(o,\varrho )y(o,\varrho )+H(o, \varrho )y\bigl(\sigma (\varrho ),o\bigr) \bigr)\Delta \varrho \Delta o \\ &\phantom{\eta _{1}(\zeta,r)=}{}+t(\zeta,r) \int _{r_{0}}^{r} \bigl(u(\zeta,\varrho )y(\zeta, \varrho )+H(\zeta,\varrho )y\bigl(\sigma (\zeta ),\varrho \bigr) \bigr)\Delta \varrho. \end{aligned}$$

Remark 3.4

Theorem 3.1 yields Lemma 3.1 of [33] by taking \(x(\zeta,r)=u(t), y(\zeta,r)=m(t)\), \(t(\zeta,r)=l(t), l(\zeta,r)=z(\zeta,r)=c(\zeta,r)=m(\zeta,r)=0\), \(\varPi (\zeta,r,o,\varrho )=1\), \(u(\zeta,r)=n(t)\) for fixed r and \(m(t)\) being a nondecreasing function.

Remark 3.5

As a distinctive case with r fixed, Theorem 3.1 reduces to Theorem 5 of [34] if we put \(x(\zeta,r)=x^{\beta }(t)\), \(\beta \geq 1\) being a constant, \(y(\zeta,r)=a(t), l(\zeta,r)=b(t), t(\zeta,r)=1, z(\zeta,r)=1, u( \zeta,r)=m(\zeta,r)=c(\zeta,r)=0\), \(\varPi (\zeta,r,o,\varrho )=1\), \(x(\sigma (\zeta ),r)=L(t, x(\tau (s)))\) and \(\xi =1\).

Theorem 3.6

Assume that \(x, y, l, t, u, m, z, c, \xi, \psi, \varPi, \varPi ^{\Delta _{1}}, \varPi ^{ \Delta _{2} \Delta _{1}}\)and H are as in Theorem 3.1. Also let

$$\begin{aligned} x(\zeta,r)\leq{}& y(\zeta,r)+ \int _{\zeta _{0}}^{\zeta } \int _{r_{0}}^{r}l(o, \varrho )x\bigl(\sigma (o),\varrho \bigr)\Delta \varrho \Delta o \\ &{}+t(\zeta,r) \int _{\zeta _{0}}^{\zeta } \int _{r_{0}}^{r}\varPi (\zeta,r,o, \varrho ) \bigl[u(o, \varrho )x(o,\varrho )+z(o,\varrho )x^{\xi }\bigl( \sigma (o),\varrho \bigr) \\ &{}-c(o,\varrho )x^{\psi }\bigl(\sigma (o),\varrho \bigr) \bigr] \Delta \varrho \Delta o \\ &{}+t(S,R) \int _{\zeta _{0}}^{S} \int _{r_{0}}^{R}\varPi (\zeta,r,o, \varrho ) \bigl[u(o,\varrho )x(o,\varrho )+z(o,\varrho )x^{\xi }\bigl( \sigma (o), \varrho \bigr) \\ &{}-c(o,\varrho )x^{\psi }\bigl(\sigma (o),\varrho \bigr) \bigr] \Delta \varrho \Delta o, \end{aligned}$$

for \((p,r)\in \varUpsilon \). If

$$\begin{aligned} \varOmega &= \int _{\zeta _{0}}^{\zeta } \int _{r_{0}}^{r}\varPi (\zeta,r,o, \varrho ) \bigl[u(o, \varrho )e_{V_{2}\oplus W_{2}}(o,\zeta _{0})+H(o, \varrho )e_{V_{2}\oplus W_{2}} \bigl(\sigma (o),\zeta _{0}\bigr) \bigr]\Delta \varrho \Delta o \\ &< \frac{1}{t(\zeta,r)}, \end{aligned}$$


$$\begin{aligned} x(\zeta,r)&\leq \frac{y(S,R)}{1-\varOmega t(S,R)}e_{V_{2}\oplus W_{2}}( \zeta,\zeta _{0}), \end{aligned}$$

so that

$$\begin{aligned} & \varTheta _{2}(\zeta,r)= \int _{r_{0}}^{r} l(\zeta,\varrho )\Delta \zeta +t^{\Delta _{1}}(\zeta,r) \int _{\zeta _{0}}^{\sigma (\zeta )} \int _{r_{0}}^{r}\varPi \bigl(\sigma (\zeta ),r,o, \varrho \bigr) \bigl(u(o,\varrho )+H(o, \varrho ) \bigr)\Delta \varrho \Delta o \\ &\phantom{\varTheta _{2}(\zeta,r)=}{}+t(\zeta,r) \int _{\zeta _{0}}^{\zeta } \int _{r_{0}}^{r}\varPi ^{\Delta _{2} \Delta _{1}}(\zeta,r,o, \varrho )H(o,\varrho )\Delta \varrho \Delta o \\ &\phantom{\varTheta _{2}(\zeta,r)=}{}+ \int _{r_{0}}^{r}\varPi ^{\Delta _{1}}\bigl(\sigma ( \zeta ),r,\zeta,v\bigr)H( \zeta,\varrho )\Delta \varrho, \end{aligned}$$
$$\begin{aligned} & W_{2}(\zeta,r)=t(\zeta,r) \int _{\zeta _{0}}^{\zeta } \int _{r_{0}}^{r} \varPi ^{\Delta _{2}\Delta _{1}}(\zeta,r,o, \varrho )u(o,\varrho ) \Delta \varrho \Delta o \\ &\phantom{W_{2}(\zeta,r)=}{}+ \int _{r_{0}}^{r}\varPi ^{\Delta _{1}}\bigl(\sigma ( \zeta ),r,\zeta,\varrho \bigr)u(\zeta,\varrho )\Delta \varrho, \end{aligned}$$
$$\begin{aligned} & V_{2}(\zeta,r)= \frac{\varTheta _{2}(\zeta,r)}{1-\mu (\zeta,r) \varTheta _{2}(\zeta,r)}. \end{aligned}$$


Inequality (17), by applying Lemma 2.2, gives

$$\begin{aligned} x(\zeta,r)={}& y(\zeta,r)+ \int _{\zeta _{0}}^{\zeta } \int _{r_{0}}^{r}l(o, \varrho )x\bigl(\sigma (o),\varrho \bigr)\Delta \varrho \Delta o \\ &{}+t(\zeta,r) \int _{\zeta _{0}}^{\zeta } \int _{r_{0}}^{r}\varPi (\zeta,r,o, \varrho ) \bigl[u(o, \varrho )x(o,\varrho )+z(o,\varrho )x^{\xi }\bigl( \sigma (o),\varrho \bigr) \\ &{}-c(o,\varrho )x^{\psi }\bigl(\sigma (o),\varrho \bigr) \bigr] \Delta \varrho \Delta o \\ &{}+t(S,R) \int _{\zeta _{0}}^{S} \int _{r_{0}}^{R}\varPi (\zeta,r,o, \varrho ) \bigl[u(o,\varrho )x(o,\varrho )+z(o,\varrho )x^{\xi }\bigl( \sigma (o), \varrho \bigr) \\ &{}-c(o,\varrho )x^{\psi }\bigl(\sigma (o),\varrho \bigr) \bigr] \Delta \varrho \Delta o \\ \leq{}& y(\zeta,r)+ \int _{\zeta _{0}}^{\zeta } \int _{r_{0}}^{r}l(o, \varrho )x\bigl(\sigma (o),\varrho \bigr)\Delta \varrho \Delta o \\ &{}+t(\zeta,r) \int _{\zeta _{0}}^{\zeta } \int _{r_{0}}^{r}\varPi (\iota,r,o, \varrho ) \bigl[u(o, \varrho )x(o,\varrho )+H(o,\varrho )x\bigl(\sigma (o), \varrho \bigr) \bigr]\Delta \varrho \Delta o \\ &{}+t(S,R) \int _{\zeta _{0}}^{S} \int _{r_{0}}^{R}\varPi (\zeta,r,o, \varrho ) \bigl[u(o,\varrho )x(o,\varrho )+H(o,\varrho )x\bigl(\sigma (o), \varrho \bigr) \bigr]\Delta \varrho \Delta o. \end{aligned}$$

Denote \(A_{1}(\zeta,r)\) a nondecreasing function as

$$\begin{aligned} A_{1}(\zeta,r)={}& y(S,R)+ \int _{\zeta _{0}}^{\zeta } \int _{r_{0}}^{r}l(o, \varrho )x\bigl(\sigma (o),\varrho \bigr)\Delta \varrho \Delta o \\ &{}+t(\zeta,r) \int _{\zeta _{0}}^{\zeta } \int _{r_{0}}^{r}\varPi (\zeta,r,o, \varrho ) \bigl[u(o, \varrho )x(o,\varrho )+H(o,\varrho )x\bigl(\sigma (o), \varrho \bigr) \bigr]\Delta \varrho \Delta o \\ &{}+t(S,R) \int _{\zeta _{0}}^{S} \int _{r_{0}}^{R}\varPi (S,R,o,\varrho ) \bigl[u(o, \varrho )x(o,\varrho )+H(o,\varrho )x\bigl(\sigma (o),\varrho \bigr) \bigr]\Delta \varrho \Delta o, \end{aligned}$$

then, from (23) and (24), we get

$$ x(\zeta,r)\leq A_{1}(\zeta,r) $$


$$\begin{aligned} A_{1}(\zeta _{0},r)={}&y(S,R)+t(S,R) \int _{\zeta _{0}}^{S} \int _{r_{0}}^{R} \varPi (S,R,o,\varrho ) \bigl[u(o, \varrho )x(o,\varrho ) \\ &{}+H(o,\varrho ))x\bigl( \sigma (o),\varrho \bigr) \bigr] \Delta \varrho \Delta o. \end{aligned}$$

Using Lemma 2.1 and delta differentiation (24) with respect to j, we have

$$\begin{aligned} &A_{1}^{\Delta _{1}}(\zeta,r) \\ &\quad \leq \int _{r_{0}}^{r}l(\zeta,\varrho )x\bigl( \sigma (\zeta ),\varrho \bigr)\Delta \varrho \\ &\qquad{}+t^{\Delta _{1}}(\zeta,r) \int _{\zeta _{0}}^{\sigma (\zeta )} \int _{r_{0}}^{r} \varPi \bigl(\sigma (\zeta ),r,o, \varrho \bigr) \bigl[u(o,\varrho )x(o,\varrho )+H(o, \varrho )x\bigl(\sigma (o), \varrho \bigr) \bigr]\Delta \varrho \Delta o \\ &\qquad{}+t(\zeta,r) \int _{\zeta _{0}}^{\zeta } \int _{r_{0}}^{r}\varPi ^{\Delta _{2} \Delta _{1}}(\zeta,r,o, \varrho ) \bigl[u(o,\varrho )x(o,\varrho )+H(o, \varrho )x\bigl(\sigma (o),\varrho \bigr) \bigr]\Delta \varrho \Delta o \\ &\qquad{}+t(\zeta,r) \int _{r_{0}}^{r}\varPi ^{\Delta _{1}}\bigl(\sigma ( \zeta ),r, \zeta,\varrho \bigr) \bigl[u(p,\varrho )x(p,\varrho )+H(p,\varrho )x \bigl( \sigma (\zeta ),\varrho \bigr) \bigr]\Delta \varrho. \end{aligned}$$

The above inequality with the help of (25) takes the form of

$$\begin{aligned} & A_{1}^{\Delta _{1}}(\zeta,r) \\ &\quad \leq \int _{r_{0}}^{r}l(\zeta,\varrho )A_{1}\bigl( \sigma (\zeta ),\varrho \bigr)\Delta \varrho \\ &\qquad{}+t^{\Delta _{1}}(\zeta,r) \int _{\zeta _{0}}^{\sigma (\zeta )} \int _{r_{0}}^{r} \varPi \bigl(\sigma (\zeta ),r,o, \varrho \bigr) \bigl[u(o,\varrho )A_{1}(o, \varrho )+H(o,\varrho )A_{1}\bigl(\sigma (o),\varrho \bigr) \bigr]\Delta \varrho \Delta o \\ &\qquad{}+t(\zeta,r) \int _{\zeta _{0}}^{\zeta } \int _{r_{0}}^{r}\varPi ^{\Delta _{2} \Delta _{1}}(\zeta,r,o, \varrho ) \bigl[u(o,\varrho )A_{1}(o,\varrho )+H(o, \varrho )A_{1}\bigl(\sigma (o),\varrho \bigr) \bigr]\Delta \varrho \Delta o \\ &\qquad{}+t(\zeta,r) \int _{r_{0}}^{r}\varPi ^{\Delta _{1}}\bigl(\sigma ( \zeta ),r, \zeta,\varrho \bigr) \bigl[u(\zeta,\varrho )A_{1}(\zeta, \varrho )+H( \zeta,\varrho )A_{1}\bigl(\sigma (\zeta ),\varrho \bigr) \bigr]\Delta \varrho \\ &\quad \leq \varTheta _{2}(\zeta,r)A_{1}\bigl(\sigma (\zeta ),r \bigr)+W_{2}(\zeta,r)A_{1}( \zeta,r), \end{aligned}$$

with \(\varTheta _{2}(\zeta,r)\), \(W_{2}(\zeta,r)\) as in (20) and (21), respectively. It can be observed from (22) that

$$ \varTheta _{2}(\zeta,r)= \frac{V_{2}(\zeta,r)}{1+\mu (\zeta,r)V_{2}(\zeta,r)}. $$

Substituting (28) in (27), we acquire

$$\begin{aligned} A_{1}^{\Delta _{1}}(\zeta,r)&\leq \varTheta _{2}(\zeta,r) \bigl(A_{1}( \zeta,r)+\mu (\zeta,r)A_{1}^{\Delta _{1}}( \zeta,r) \bigr)+W_{2}( \zeta,r)A_{1}(\zeta,r) \\ &\leq \frac{V_{2}(\zeta,r)}{1+\mu (\zeta,r)V_{2}(\zeta,r)} \bigl(A_{1}( \zeta,r)+\mu ( \zeta,r)A_{1}^{\Delta _{1}}(\zeta,r) \bigr)+W_{2}( \zeta,r)A_{1}(\zeta,r), \end{aligned}$$

which implies

$$\begin{aligned} A_{1}^{\Delta _{1}}(\zeta,r)\leq{}& \bigl(V_{2}(\zeta,r)+W_{2}(\zeta,r)+ \mu (\zeta,r) V_{2}(\zeta,r)W_{2}(\zeta,r) \bigr)A_{1}( \zeta,r) \\ &{}+ \bigl(1+\mu (\zeta,r)V_{2}(\zeta,r) \bigr) \\ \leq{}& (V_{2}\oplus W_{2}) (\zeta,r)A_{1}( \zeta,r). \end{aligned}$$

Since \(A_{1}(\zeta,r)\) is rd-continuous and \(V_{2}\oplus W_{2}\in \Re ^{+}\), inequality (29), with Lemma 2.4, (25) and (26), produces

$$\begin{aligned} A_{1}(\zeta,r)\leq {}&A_{1}(\zeta _{0},r)e_{V_{2}\oplus W_{2}}(\zeta, \zeta _{0}) \\ \leq{}& \biggl\{ y(S,R)+t(S,R) \int _{\zeta _{0}}^{S} \int _{r_{0}}^{R}\varPi (S,R,o, \varrho ) \bigl[u(o, \varrho )A_{1}(o,\varrho ) \\ &{}+H(o,\varrho ))A_{1}\bigl( \sigma (o),\varrho \bigr) \bigr]\Delta \varrho \Delta o \biggr\} e_{V_{2} \oplus W_{2}}(\zeta, \zeta _{0}) \\ ={}&B(S,R) e_{V_{2}\oplus W_{2}}(\zeta,\zeta _{0}), \end{aligned}$$


$$\begin{aligned} B(S,R)={}&y(S,R) \\ &{}+t(S,R) \int _{\zeta _{0}}^{S} \int _{r_{0}}^{R}\varPi (S,R,o, \varrho ) \bigl[u(o, \varrho )A_{1}(o,\varrho )+H(o,\varrho ))A_{1}\bigl( \sigma (o),\varrho \bigr) \bigr]\Delta \varrho \Delta o \\ \leq{}& y(S,R)+t(S,R) \int _{\zeta _{0}}^{S} \int _{r_{0}}^{R}\varPi (S,R,o, \varrho ) \\ &{}\times \bigl[u(o,\varrho )B(S,R) e_{V_{2}\oplus W_{2}}(o,\zeta _{0})+H(o, \varrho ))B\bigl(\sigma (S),R\bigr) e_{V_{2}\oplus W_{2}}\bigl(\sigma (o),\zeta _{0}\bigr) \bigr]\Delta \varrho \Delta o \\ \leq {}&\frac{y(S,R)}{1-\varOmega t(S,R)}. \end{aligned}$$

Here Ω is defined as in (18). The conclusion in (19) can be achieved from (25), (30), and (31). Details are omitted. □

Remark 3.7

If \(x(\zeta,r)=u^{\beta }(x,y), y(\zeta,r)=c\), \(c>0\), \(t(\zeta,r)=0, l(\zeta,r)=f(x,y), x(\sigma (\zeta ),r)=\omega (u( \tau _{1}(t), \tau _{2}(t)))\), then Theorem 3.6 can be transformed into the inequality of Theorem 2.14 stated by Zheng et al. [35].

Remark 3.8

If \(x(\zeta,r)=x(\sigma (\zeta ),r)=u(t,s), y(p,r)=a(t,s), l(\zeta,r)=b(t,s)\) and \(t(\zeta,r)=0\), then we can conveniently reach Theorem 1 of [36] from Theorem 3.6.

Theorem 3.9

Let \(x, y, l, u, z, c, H, \xi \)and ψ be as in Theorem 3.1. In addition, suppose \(m\in C_{rd}(\varUpsilon \times \varUpsilon,\mathbb{R}_{+})\)is nondecreasing in j and

$$\begin{aligned} x(\zeta,r)\leq{}& y(\zeta,r)+ \int _{\zeta _{0}}^{\zeta } \int _{r_{0}}^{r}l( \zeta,r,o,\varrho ) \biggl[x(o, \varrho ) \\ &{}+ \int _{\zeta _{0}}^{o} \int _{r_{0}}^{\varrho } \bigl(u(n,k)x\bigl(\sigma (n),k \bigr)+z(n,k)x^{ \xi }(n,k)-c(n,k)x^{\psi }(n,k) \bigr)\Delta k \Delta n \biggr]\Delta \varrho \Delta o \\ &{}+ \int _{\zeta _{0}}^{S}m(\zeta,o,r)x(o,r)\Delta o,\quad (\zeta,r) \in \varUpsilon, \end{aligned}$$


$$ \int _{\zeta _{0}}^{S}m(S,o,r)e_{V_{3}\oplus W_{3}}(o,\zeta _{0}) \Delta o< 1. $$


$$ x(\zeta,r)\leq \frac{y(S,r)}{1-\int _{\zeta _{0}}^{S}m(S,o,r)e_{V_{3}\oplus W_{3}}(o,\zeta _{0})\Delta o}e_{V_{3} \oplus W_{3}}(\zeta,\zeta _{0}), $$


$$\begin{aligned} & \varTheta _{3}(\zeta,r)= \int _{r_{0}}^{r}u(\zeta,\varrho )\Delta \varrho, \end{aligned}$$
$$\begin{aligned} &W_{3}(\zeta,r)= \int _{r_{0}}^{r}l\bigl(\sigma (\zeta ),r,\zeta,\varrho \bigr) \Delta \varrho + \int _{\zeta _{0}}^{\zeta } \int _{r_{0}}^{r}l^{\Delta _{2} \Delta _{1}}(\zeta,r,o,\varrho ) \Delta \varrho \Delta o \\ &\phantom{W_{3}(\zeta,r)=}{}+ \int _{r_{0}}^{r}H( \zeta,\varrho )\Delta \varrho, \end{aligned}$$
$$\begin{aligned} & V_{3}(\zeta,r)= \frac{\varTheta _{3}(\zeta,r)}{1-\mu (\zeta,r) \varTheta _{3}(\zeta,r)}. \end{aligned}$$


From (32) and Lemma 2.2, we have

$$\begin{aligned} x(\zeta,r)\leq {}&y(\zeta,r)+ \int _{\zeta _{0}}^{\zeta } \int _{r_{0}}^{r}l( \zeta,r,o,\varrho ) \biggl[x(o, \varrho ) \\ &{}+ \int _{\zeta _{0}}^{o} \int _{r_{0}}^{\varrho } \bigl(u(n,k)x\bigl(\sigma (n),k \bigr)+H(n,k)x(n,k) \bigr)\Delta k \Delta n \biggr]\Delta \varrho \Delta o \\ &{}+ \int _{\zeta _{0}}^{S}m(\zeta,o,r)x(o,r)\Delta o. \end{aligned}$$

Clearly, \(x(\zeta,r)\) is nonnegative. Also \(\int _{\zeta _{0}}^{S}m(\zeta,o,r)x(o,r)\Delta o\) is a nondecreasing function because \(m(\zeta,o,\varrho )\) is a nondecreasing function for \((\zeta,r)\in \varUpsilon \), By delta-differentiating (38), we get

$$\begin{aligned} x^{\Delta _{1}}(\zeta,r)={}& \int _{r_{0}}^{r}l\bigl(\sigma (\zeta ),r, \zeta,\varrho \bigr) \biggl[x(\zeta,\varrho )+ \int _{\zeta _{0}}^{\zeta } \int _{r_{0}}^{\varrho } \bigl(u(o,k)x\bigl(\sigma (o),k \bigr) \\ &{}+H(o,k)x(o,k) \Delta k \Delta o \bigr) \biggr]\Delta \varrho \\ &{}+ \int _{\zeta _{0}}^{\zeta } \int _{r_{0}}^{r}l^{\Delta _{2}\Delta _{1}}( \zeta,r,o,\varrho ) \biggl[x(o,\varrho ) \\ &{}+ \int _{\zeta _{0}}^{o} \int _{r_{0}}^{v} \bigl(u(n,k)x\bigl(\sigma (n),k \bigr)+H(n,k)x(n,k) \bigr)\Delta k \Delta n \biggr] \Delta \varrho \Delta o \\ \leq{}& \biggl[ \int _{r_{0}}^{r}l\bigl(\sigma (\zeta ),r,\zeta,\varrho \bigr) \Delta v+ \int _{\zeta _{0}}^{\zeta } \int _{r_{0}}^{r}l^{\Delta _{2} \Delta _{1}}(\zeta,r,o,\varrho ) \Delta \varrho \Delta o \biggr]A_{2}( \zeta,r), \end{aligned}$$

so that

$$ A_{2}(\zeta,r)=x(\zeta,r)+ \int _{\zeta _{0}}^{\zeta } \int _{r_{0}}^{r} \bigl(u(o,\varrho )x\bigl(\sigma (o), \varrho \bigr)+H(o,\varrho )x(o,\varrho ) \bigr)\Delta \varrho \Delta o $$


$$ x(\zeta,r)\leq A_{2}(\zeta,r). $$

From inequality (39), again by delta differentiating with respect to j and using (40) and (41), we get

$$\begin{aligned} A^{\Delta _{1}}_{2}(\zeta,r)&\leq W_{3}( \zeta,r)A_{2}(\zeta,r)+ \varTheta _{3}(\zeta,r)A_{2} \bigl(\sigma (\zeta ),r\bigr). \end{aligned}$$

Further, the above inequality, by utilizing Lemma 2.4, (37), and the fact that \(A_{2}(\zeta _{0},r)=y(\zeta,r)+\int _{\zeta _{0}}^{P}m(\zeta,o,r)x(o,r) \Delta o\), gives the bound

$$ A_{2}(\zeta,r)\leq \biggl(y(\zeta,r)+ \int _{\zeta _{0}}^{S}m(\zeta,o,r)x(o,r) \Delta o \biggr)e_{V_{3}\oplus W_{3}}(\zeta,\zeta _{0}), $$

where \(\varTheta _{3}\), \(W_{3}\), \(V_{3}\) are defined as in (35), (36), and (37), respectively. The monotonicity of y and m in the last inequality yields

$$\begin{aligned} A_{2}(\zeta,r)&\leq \biggl(y(S,r)+ \int _{\zeta _{0}}^{P}m(S,o,r)x(o,r) \Delta o \biggr)e_{V_{3}\oplus W_{3}}(\zeta,\zeta _{0}) \\ &=B_{1}(S,r)e_{V_{3}\oplus W_{3}}(\zeta,\zeta _{0}), \end{aligned}$$


$$ B_{1}(S,r)=y(S,r)+ \int _{\zeta _{0}}^{S}m(S,o,r)x(o,r)\Delta o. $$

From the definition of \(B_{1}(\zeta,r)\), (41) and (42), we obtain

$$ B_{1}(S,r)\leq \frac{y(S,r)}{1-\int _{\zeta _{0}}^{S}m(S,o,r)e_{V_{3}\oplus W_{3}}(o,\zeta _{0})\Delta o}, $$

so the required bound in (34) can be acquired by combining (41), (42), and (43). □

Remark 3.10

If we fix r and \(x(\zeta,r)=u(t), y(\zeta,r)=c\), \(c\geq 0\), \(l(\zeta,r,o,\varrho )=f(t), u(\zeta,r)=c(\zeta,r)=m(\zeta,r)=0\), \(z(\zeta,r)=\omega (t,s)\) in Theorem 3.9, where \(\omega (t,s)\geq 0 \), then we get the inequality obtained by Li et al. in [37]; see their Theorem 3.1.

4 Applications

In this section we focus on some of the applications of Theorem 3.1 to research certain properties of differential equation solutions. Let us discuss the following dynamic integral equation on time scales:

$$\begin{aligned} x(\zeta,r)={}&y(\zeta,r)+ \int _{\zeta _{0}}^{\zeta } \int _{r_{0}}^{r}Y \bigl(o,\varrho,x(o,\varrho ) \bigr) \Delta \varrho \Delta o \\ &{}+t(\zeta,r) \int _{\zeta _{0}}^{\zeta } \int _{r_{0}}^{r}P \bigl(\zeta,r,o, \varrho,x(o,\varrho ),x\bigl(\sigma (o),\varrho \bigr) \bigr)\Delta \varrho \Delta o \\ &{}+ \int _{\zeta _{0}}^{\zeta }T \bigl(o,r,x(o,r) \bigr)\Delta o, \end{aligned}$$

where \(P\in C_{rd}(\varUpsilon ^{2}\times \mathbb{R}^{2},\mathbb{R})\) and \(Y, T\in C_{rd}(\varUpsilon \times \mathbb{R},\mathbb{R})\).

The ensuing example addresses the global existence on the solutions of (44).

Example 4.1

Suppose that

$$\begin{aligned} & \bigl\vert Y(\zeta,r,d) \bigr\vert \leq l(\zeta,r) \vert d \vert , \end{aligned}$$
$$\begin{aligned} &\bigl\vert P(\zeta,r,o,\varrho,d,h) \bigr\vert \leq \varPi ( \zeta,r,o,\varrho ) \bigl[u(o, \varrho ) \vert d \vert +z(o,\varrho ) \vert h \vert ^{\xi }-c(o,\varrho ) \vert h \vert ^{\psi } \bigr], \end{aligned}$$
$$\begin{aligned} &\bigl\vert T(\zeta,r,d) \bigr\vert \leq m(\zeta,r) \vert d \vert , \end{aligned}$$

for \((\zeta,r)\in \varUpsilon \), \(d,\varrho \in \mathbb{R}\), then \(x(\zeta,r)\) is a solution of (44) with

$$ \mu (\zeta,r)\varTheta (\zeta,r)< 1,\qquad \int _{\zeta _{0}}^{S}m(o,r)e_{V \oplus W}(o,\zeta _{0})\Delta o< 1, $$

and satisfies

$$\begin{aligned} \bigl\vert x(\zeta,r) \bigr\vert \leq{}& \bigl\vert y( \zeta,r) \bigr\vert + \frac{\int _{\zeta _{0}}^{S}m(o,r) [ \vert y(o,r) \vert +\int _{\zeta _{0}}^{o}e_{V\oplus W}(o,\sigma (\tau ))D(\tau,r)\Delta \tau ]\Delta a}{1-\int _{\zeta _{0}}^{S}m(o,r)e_{V\oplus W}(o,\zeta _{0})\Delta o}e_{V \oplus W}(\zeta,\zeta _{0}) \\ &{}+ \int _{\zeta _{0}}^{S}m(o,r)e_{V\oplus W}\bigl(\tau, \sigma (o)\bigr)\Delta o, \end{aligned}$$

where \(x, l, t, y, u, z, c, m, \varPi, \xi, \psi, \varTheta, W, V\) and D are as in Theorem 3.1.


Equation (44) by utilizing (45)–(47) can be restated as

$$\begin{aligned} \bigl\vert x(\zeta,r) \bigr\vert \leq{}& \biggl\vert y(\zeta,r)+ \int _{\zeta _{0}}^{S} \int _{r_{0)}}^{r}Y \bigl(o,\varrho,x(o,\varrho ) \bigr) \Delta \varrho \Delta o \\ &{}+t(\zeta,r) \int _{\zeta _{0}}^{p} \int _{r_{0}}^{r}P \bigl(\zeta,r,o, \varrho,x(o,\varrho ),x\bigl(\sigma (o),\varrho \bigr) \bigr)\Delta v \Delta o \\ &{}+ \int _{\zeta _{0}}^{\zeta }T \bigl(o,r,x(o,r) \bigr)\Delta o \biggr\vert \\ \leq{}& \bigl\vert y(\zeta,r) \bigr\vert + \int _{\zeta _{0}}^{\zeta } \int _{r_{0}}^{r} \bigl\vert Y \bigl(o,\varrho,x(o, \varrho ) \bigr) \bigr\vert \Delta \varrho \Delta o \\ &{}+t(\zeta,r) \int _{\zeta _{0}}^{\zeta } \int _{r_{0}}^{r} \bigl\vert P \bigl( \zeta,r,o, \varrho,x(o,\varrho ),x\bigl(\sigma (o),\varrho \bigr) \bigr) \bigr\vert \Delta \varrho \Delta o \\ &{}+ \int _{\zeta _{0}}^{\zeta } \bigl\vert T \bigl(o,r,x(o,r) \bigr) \bigr\vert \Delta o \\ \leq{}& \bigl\vert y(\zeta,r) \bigr\vert + \int _{\zeta _{0}}^{\zeta } \int _{r_{0}}^{r}l(o, \varrho ) \bigl\vert x(o,\varrho ) \bigr\vert \Delta \varrho \Delta o \\ &{}+t(\zeta,r) \int _{\zeta _{0}}^{\zeta } \int _{r_{0}}^{r}\varPi (\zeta,r,o, \varrho ) \bigl[u(o, \varrho ) \bigl\vert x(o,\varrho ) \bigr\vert +z(o,\varrho ) \bigl\vert x \bigl(\sigma (o), \varrho \bigr) \bigr\vert ^{\xi } \\ &{}-c(o,\varrho ) \bigl\vert x\bigl(\sigma (o),\varrho \bigr) \bigr\vert ^{\psi } \bigr] \Delta \varrho \Delta o \\ &{}+ \int _{\zeta _{0}}^{S}m(o,r) \bigl\vert x(o,r) \bigr\vert \Delta o. \end{aligned}$$

We attain (48) by applying the same procedure as in the proof of Theorem 3.1 to (49). □

Example 4.2

Let us consider the following hypotheses:

$$\begin{aligned} & \bigl\vert Y(\zeta,r,d_{1})-Y(\zeta,r,d_{2}) \bigr\vert \leq l(\zeta,r) \vert d_{1}-d_{2} \vert , \end{aligned}$$
$$\begin{aligned} &\bigl\vert P(\zeta,r,o,\varrho,d_{1},h_{1})-P( \zeta,r,o,\varrho,d_{2},h_{2}) \bigr\vert \leq \varPi ( \zeta,r,o,\varrho ) \bigl[u(o,\varrho ) \vert d_{1}-d_{2} \vert \\ &\phantom{\bigl\vert P(\zeta,r,o,\varrho,d_{1},h_{1})-P( \zeta,r,o,\varrho,d_{2},h_{2}) \bigr\vert \leq}{}+z(o,\varrho ) \vert h_{1}-h_{2} \vert ^{\xi }-c(o,\varrho ) \vert h_{1}-h_{2} \vert ^{\psi } \bigr], \end{aligned}$$
$$\begin{aligned} &\bigl\vert T(\zeta,r,d_{1})-T(\zeta,r,d_{2}) \bigr\vert \leq m(\zeta,r) \vert d_{1}-d_{2} \vert , \end{aligned}$$

then the dynamic integral equation (44) has a unique solution.


If \(x_{1}(\zeta,r)\) and \(x_{2}(\zeta,r)\) are solutions of (44), then

$$\begin{aligned} x_{1}(\zeta,r)-x_{2}(\zeta,r) ={}& \int _{\zeta _{0}}^{\zeta } \int _{r_{0}}^{r} \bigl[Y \bigl(o,\varrho,x_{1}(o, \varrho ) \bigr)-Y \bigl(o,\varrho,x_{2}(o, \varrho ) \bigr) \bigr] \Delta v \Delta o \\ &{}+t(\zeta,r) \int _{\zeta _{0}}^{\zeta } \int _{r_{0}}^{r} \bigl[P \bigl( \zeta,r,o, \varrho,x_{1}(o,\varrho ),x_{1}\bigl(\sigma (o),\varrho \bigr) \bigr) \\ &{}-P \bigl(\zeta,r,o,\varrho,x_{2}(o,\varrho ),x_{2}\bigl(\sigma (o), \varrho \bigr) \bigr) \bigr]\Delta \varrho \Delta o \\ &{}+ \int _{\zeta _{0}}^{\zeta } \bigl[T \bigl(o,r,x_{1}(o,r) \bigr)-T \bigl(o,r,x_{1}(o,r) \bigr) \bigr]\Delta o. \end{aligned}$$

From (50)–(52) used to the previous equation, we get

$$\begin{aligned} &\bigl\vert x_{1}(\zeta,r)-x_{2}(\zeta,r) \bigr\vert \\ &\quad \leq \int _{\zeta _{0}}^{\zeta } \int _{r_{0}}^{r}l(o,\varrho ) \bigl\vert x_{1}(o,\varrho )-x_{2}(o,\varrho ) \bigr\vert \Delta \varrho \Delta o+t(\zeta,r) \int _{\zeta _{0}}^{\zeta } \int _{r_{0}}^{r} \varPi (\zeta,r,o,\varrho ) \\ &\qquad{}\times \bigl[u(o,\varrho ) \bigl\vert x_{1}(o,\varrho )-x_{2}(o,\varrho ) \bigr\vert +z(o, \varrho ) \bigl\vert x_{1}\bigl(\sigma (o),\varrho \bigr)-x_{2}\bigl(\sigma (o), \varrho \bigr) \bigr\vert ^{\xi } \\ &\qquad{}-c(o,\varrho ) \bigl\vert x_{1}\bigl(\sigma (o),\varrho \bigr)-x_{2}\bigl(\sigma (o),\varrho \bigr) \bigr\vert ^{ \psi } \bigr]\Delta \varrho \Delta o \\ &\qquad{}+ \int _{\zeta _{0}}^{S}m(o,r) \bigl\vert x_{1}(o,r)-x_{2}(o,r) \bigr\vert \Delta o, \end{aligned}$$

so applying a similar method as that in Theorem 3.1 with suitable changes to the function \(|x_{1}(p,r)-x_{2}(p,r)|\) in (53), we have

$$ \bigl\vert x_{1}(\zeta,r)-x_{2}(\zeta,r) \bigr\vert \leq 0,\quad (\zeta,r)\in \varUpsilon. $$

Hence \(x_{1}(\zeta,r)=x_{2}(\zeta,r)\). Thus the dynamic equation (44) has one positive solution. □

5 Conclusion

Like other recognized and proven inequalities in the literature, Theorems 3.1, 3.6, and 3.9 examined such dynamic integral inequalities with suggested remarks for two independent variables on time scales. In order to overcome the conceptual classifications of differential equations, one may also apply the introduced corollaries. Our results may be extended by using the basic methodology to solve the difficulty of achieving estimates on the specific bounds of unknown functions and therefore to expand and unify continuous inequalities. This investigation offers the foundation for further advancement of the idea of integral inequality for time scale calculus implementations, providing scope for maximizing efforts to reach a desirable outcome.


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The authors would like to thank the editor and the referees for their careful reading and for their helpful comments and suggestions that led to considerable improvements of the paper.

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This research was funded by the Deanship of Scientific Research at Princess Nourah bint Abdulrahman University through the Fast-track Research Funding Program.

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Khan, Z.A., Jarad, F., Khan, A. et al. Derivation of dynamical integral inequalities based on two-dimensional time scales theory. J Inequal Appl 2020, 209 (2020).

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