<?xml version="1.0" encoding="UTF-8"?><!DOCTYPE article  PUBLIC "-//NLM//DTD Journal Publishing DTD v3.0 20080202//EN" "http://dtd.nlm.nih.gov/publishing/3.0/journalpublishing3.dtd"><article xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink" dtd-version="3.0" xml:lang="en" article-type="research article"><front><journal-meta><journal-id journal-id-type="publisher-id">JAMP</journal-id><journal-title-group><journal-title>Journal of Applied Mathematics and Physics</journal-title></journal-title-group><issn pub-type="epub">2327-4352</issn><publisher><publisher-name>Scientific Research Publishing</publisher-name></publisher></journal-meta><article-meta><article-id pub-id-type="doi">10.4236/jamp.2017.512193</article-id><article-id pub-id-type="publisher-id">JAMP-81389</article-id><article-categories><subj-group subj-group-type="heading"><subject>Articles</subject></subj-group><subj-group subj-group-type="Discipline-v2"><subject>Physics&amp;Mathematics</subject></subj-group></article-categories><title-group><article-title>
 
 
  Dynamic Inequalities for Convex Functions Harmonized on Time Scales
 
</article-title></title-group><contrib-group><contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>Muhammad</surname><given-names>Jibril Shahab Sahir</given-names></name><xref ref-type="aff" rid="aff1"><sub>1</sub></xref><xref ref-type="corresp" rid="cor1"><sup>*</sup></xref></contrib></contrib-group><aff id="aff1"><label>1</label><addr-line>University of Sargodha, Sub-Campus Bhakkar, Bhakkar, Pakistan</addr-line></aff><author-notes><corresp id="cor1">* E-mail:<email>jibrielshahab@gmail.com</email></corresp></author-notes><pub-date pub-type="epub"><day>06</day><month>12</month><year>2017</year></pub-date><volume>05</volume><issue>12</issue><fpage>2360</fpage><lpage>2370</lpage><history><date date-type="received"><day>1,</day>	<month>November</month>	<year>2017</year></date><date date-type="rev-recd"><day>26,</day>	<month>December</month>	<year>2017</year>	</date><date date-type="accepted"><day>29,</day>	<month>December</month>	<year>2017</year></date></history><permissions><copyright-statement>&#169; Copyright  2014 by authors and Scientific Research Publishing Inc. </copyright-statement><copyright-year>2014</copyright-year><license><license-p>This work is licensed under the Creative Commons Attribution International License (CC BY). http://creativecommons.org/licenses/by/4.0/</license-p></license></permissions><abstract><p><html>
 <head></head>
 
  We present here some general fractional Schl?milch’s type an
  d Rogers-H?lder’s type dynamic inequalities for convex functions harmonized on time scales. First we present general fractional Schl?milch’s type dynamic inequalities and generalize it for convex functions of several variables by using Bernoulli’s inequality, generalized Jensen’s inequality and Fubini’s theorem on diamond-
  α 
  calculus. To conclude our main results, we present general fractional Rogers-H?lder’s type dynamic inequalities for convex functions by using general fractional Schl?milch’s type dynamic inequality on diamond-
  α 
  calculus for p<sub>i</sub>&gt;1 with <img src="Edit_13da77b1-ab27-448b-a8c0-152b39deb7af.bmp" alt="" />.
 
</html></p></abstract><kwd-group><kwd>Delta</kwd><kwd> Nabla and Diamond-α Time Scales</kwd><kwd> Fractional Integral Inequalities</kwd></kwd-group></article-meta></front><body><sec id="s1"><title>1. Introduction</title><p>In the following, we present a result proved by Mitrinović and Pečarić as given in [<xref ref-type="bibr" rid="scirp.81389-ref1">1</xref>] and ( [<xref ref-type="bibr" rid="scirp.81389-ref2">2</xref>] , p. 235).</p><p>Theorem 1. Let g i ∈ G ( f i , k ) for ( i = 1 , 2 ) be a class, where f i ( x ) for ( i = 1 , 2 ) are continuous functions and f 2 ( x ) &gt; 0 implies g 2 ( x ) &gt; 0 for every x ∈ [ a , b ] and g i : [ a , b ] → ℝ are represented by</p><p>g i ( x ) : = ∫ a b     k ( x , y ) f i ( y ) d y , ∀ x ∈ [ a , b ] , i = 1 , 2 ,</p><p>where k ( x , y ) is nonnegative arbitrary kernel. Consider w ( x ) ≥ 0 for every x ∈ [ a , b ] . Let F : ℝ 0 + = [ 0 , ∞ ) → ℝ be a convex and increasing function, then the following inequality holds</p><p>∫ a b     w ( x ) F ( | g 1 ( x ) g 2 ( x ) | ) d x ≤ ∫ a b     F ( | f 1 ( y ) f 2 ( y ) | ) s ( y ) d y , (1)</p><p>where,</p><p>s ( y ) : = f 2 ( y ) ∫ a b w ( x ) k ( x , y ) g 2 ( x ) d x , ∀ y ∈ [ a , b ] , g 2 ( x ) ≠ 0.</p><p>Next we present a result on diamond-α calculus, as given in [<xref ref-type="bibr" rid="scirp.81389-ref3">3</xref>] .</p><p>Theorem 2. Let T 1 , T 2 be two time scales, and a , b ∈ T 1 ; c , d ∈ T 2 ; k ( x , y ) is a kernel function with x ∈ [ a , b ] T 1 , y ∈ [ c , d ] T 2 ; k is continuous function from [ a , b ] T 1 &#215; [ c , d ] T 2 into ℝ 0 + = [ 0 , ∞ ) . Consider</p><p>K ( x ) : = ∫ c d     k ( x , y ) ⋄ α y , ∀ x ∈ [ a , b ] T 1 .</p><p>We assume that K ( x ) &gt; 0 , ∀ x ∈ [ a , b ] T 1 . Consider f : [ c , d ] T 2 → ℝ continuous, and the ⋄ α -integral operator function</p><p>g ( x ) : = ∫ c d     k ( x , y ) f ( y ) ⋄ α y , ∀ x ∈ [ a , b ] T 1 .</p><p>Consider also the weight function w : [ a , b ] T 1 → ℝ 0 + , which is continuous.</p><p>Define further the function s ( y ) : = ∫ a b w ( x ) k ( x , y ) K ( x ) ⋄ α x , ∀ y ∈ [ c , d ] T 2 . Let I denote</p><p>any of ( 0, ∞ ) or [ 0, ∞ ) , and F : I → ℝ be a convex and increasing function. In particular, we assume that</p><p>| f | ( [ c , d ] T 2 ) ⊆ I .</p><p>Then</p><p>∫ a b   w ( x ) F ( | g ( x ) | K ( x ) ) ⋄ α x ≤ ∫ c d s ( y ) F ( | f ( y ) | ) ⋄ α y . (2)</p><p>We extend these results on time scale calculus. In this paper, it is assumed that all considerable integrals exist and are finite and T is a time scale, a , b ∈ T with a &lt; b and an interval [ a , b ] T means the intersection of a real interval with the given time scale.</p></sec><sec id="s2"><title>2. Preliminaries</title><p>We need here basic concepts of delta calculus. The results of delta calculus are adapted from [<xref ref-type="bibr" rid="scirp.81389-ref4">4</xref>] [<xref ref-type="bibr" rid="scirp.81389-ref5">5</xref>] [<xref ref-type="bibr" rid="scirp.81389-ref6">6</xref>] .</p><p>Time scale calculus was initiated by Stefan Hilger as given in [<xref ref-type="bibr" rid="scirp.81389-ref7">7</xref>] . A time scale is an arbitrary nonempty closed subset of the real numbers. It is denoted by T . For t ∈ T , forward jump operator σ : T → T is defined by</p><p>σ ( t ) : = inf { s ∈ T : s &gt; t } .</p><p>The mapping μ : T → ℝ 0 + = [ 0 , ∞ ) such that μ ( t ) : = σ ( t ) − t is called the forward graininess function. The backward jump operator ρ : T → T is defined by</p><p>ρ ( t ) : = sup { s ∈ T : s &lt; t } .</p><p>The mapping ν : T → ℝ 0 + = [ 0 , ∞ ) such that ν ( t ) : = t − ρ ( t ) is called the backward graininess function. If σ ( t ) &gt; t , we say that t is right-scattered, while if ρ ( t ) &lt; t , we say that t is left-scattered. Also, if t &lt; sup T and σ ( t ) = t , then t is called right-dense, and if t &gt; inf T and ρ ( t ) = t , then t is called left-dense. Points that are right-dense and left-dense at the same time are called dense. If T has a left-scattered maximum M, then T k = T − { M } . Otherwise T k = T .</p><p>For a function f : T → ℝ , the derivative f Δ is defined as follows. Let t ∈ T k , if there exists f Δ ( t ) ∈ ℝ such that for all ϵ &gt; 0 , there exists a neighborhood U of t, such that</p><p>| f ( σ ( t ) ) − f ( s ) − f Δ ( t ) ( σ ( t ) − s ) | ≤ ϵ | σ ( t ) − s | ,</p><p>for all s ∈ U , then f is said to be delta differentiable at t, and f Δ ( t ) is called the delta derivative of f at t.</p><p>A function f : T → ℝ is said to be right-dense continuous (rd-continuous), if it is continuous at each right-dense point and there exists a finite left limit in every left-dense point. The set of all rd-continuous functions is denoted by C r d ( T , ℝ ) .</p><p>The next definition is given in [<xref ref-type="bibr" rid="scirp.81389-ref4">4</xref>] [<xref ref-type="bibr" rid="scirp.81389-ref5">5</xref>] [<xref ref-type="bibr" rid="scirp.81389-ref6">6</xref>] .</p><p>Definition 1. A function F : T → ℝ is called a delta antiderivative of f : T → ℝ , provided that F Δ ( t ) = f ( t ) holds for all t ∈ T k , then the delta integral of f is defined by</p><p>∫ a b f ( t ) Δ t = F ( b ) − F ( a ) .</p><p>The following results of nabla calculus are taken from [<xref ref-type="bibr" rid="scirp.81389-ref4">4</xref>] [<xref ref-type="bibr" rid="scirp.81389-ref5">5</xref>] [<xref ref-type="bibr" rid="scirp.81389-ref6">6</xref>] [<xref ref-type="bibr" rid="scirp.81389-ref8">8</xref>] .</p><p>If T has a right-scattered minimum m, then T k = T − { m } . Otherwise T k = T . The function f : T → ℝ is called nabla differentiable at t ∈ T k , if there exists f ∇ ( t ) ∈ ℝ such that for any ϵ &gt; 0 , there exists a neighborhood V of t, such that</p><p>| f ( ρ ( t ) ) − f ( s ) − f ∇ ( t ) ( ρ ( t ) − s ) | ≤ ϵ | ρ ( t ) − s | ,</p><p>for all s ∈ V .</p><p>A function f : T → ℝ is left-dense continuous (ld-continuous), provided it is continuous at left-dense points in T and its right-sided limits exist (finite) at right-dense points in T . The set of all ld-continuous functions is denoted by C l d ( T , ℝ ) .</p><p>The next definition is given in [<xref ref-type="bibr" rid="scirp.81389-ref4">4</xref>] [<xref ref-type="bibr" rid="scirp.81389-ref5">5</xref>] [<xref ref-type="bibr" rid="scirp.81389-ref6">6</xref>] [<xref ref-type="bibr" rid="scirp.81389-ref8">8</xref>] .</p><p>Definition 2. A function G : T → ℝ is called a nabla antiderivative of g : T → ℝ , provided that G ∇ ( t ) = g ( t ) holds for all t ∈ T k , then the nabla integral of g is defined by</p><p>∫ a b g ( t ) ∇ t = G ( b ) − G ( a ) .</p><p>Now we present short introduction of diamond-α derivative as given in [<xref ref-type="bibr" rid="scirp.81389-ref4">4</xref>] [<xref ref-type="bibr" rid="scirp.81389-ref9">9</xref>] .</p><p>Let T be a time scale and f ( t ) be differentiable on T in the Δ and ∇ senses. For t ∈ T k k , where T k k = T k ∩ T k , diamond-α dynamic derivative f ⋄ α ( t ) is defined by</p><p>f ⋄ α ( t ) = α f Δ ( t ) + ( 1 − α ) f ∇ ( t ) , 0 ≤ α ≤ 1.</p><p>Thus f is diamond-α differentiable if and only if f is Δ and ∇ differentiable.</p><p>The diamond-α derivative reduces to the standard Δ -derivative for α = 1 , or the standard ∇ -derivative for α = 0 . It represents a weighted dynamic derivative for α ∈ ( 0,1 ) .</p><p>Theorem 3. [<xref ref-type="bibr" rid="scirp.81389-ref9">9</xref>] : Let f , g : T → ℝ be diamond-α differentiable at t ∈ T . Then</p><p>1) f &#177; g : T → ℝ is diamond-α differentiable at t ∈ T , with</p><p>( f &#177; g ) ⋄ α ( t ) = f ⋄ α ( t ) &#177; g ⋄ α ( t ) .</p><p>2) f g : T → ℝ is diamond-α differentiable at t ∈ T , with</p><p>( f g ) ⋄ α ( t ) = f ⋄ α ( t ) g ( t ) + α f σ ( t ) g Δ ( t )     + ( 1 − α ) f ρ ( t ) g ∇ ( t ) .</p><p>3) For g ( t ) g σ ( t ) g ρ ( t ) ≠ 0 , f g : T → ℝ is diamond-α differentiable at</p><p>t ∈ T , with</p><p>( f g ) ⋄ α ( t ) = f ⋄ α ( t ) g σ ( t ) g ρ ( t ) − α f σ ( t ) g ρ ( t ) g Δ ( t ) − ( 1 − α ) f ρ ( t ) g σ ( t ) g ∇ ( t ) g ( t ) g σ ( t ) g ρ ( t ) .</p><p>Theorem 4. [<xref ref-type="bibr" rid="scirp.81389-ref9">9</xref>] : Let a , t ∈ T and h : T → ℝ . Then the diamond-α integral from a to t of h is defined by</p><p>∫ a t h ( s ) ⋄ α s = α ∫ a t h ( s ) Δ s + ( 1 − α ) ∫ a t h ( s ) ∇ s , 0 ≤ α ≤ 1,</p><p>provided that there exist delta and nabla integrals of h on T .</p><p>Theorem 5. [<xref ref-type="bibr" rid="scirp.81389-ref9">9</xref>] : Let a , b , t ∈ T , c ∈ ℝ . Assume that f ( s ) and g ( s ) are ⋄ α -integrable functions on [ a , b ] T , then</p><p>1) ∫ a t [ f ( s ) &#177; g ( s ) ] ⋄ α s = ∫ a t f ( s ) ⋄ α s &#177; ∫ a t g ( s ) ⋄ α s ;</p><p>2) ∫ a t c f ( s ) ⋄ α s = c ∫ a t f ( s ) ⋄ α s ;</p><p>3) ∫ a t f ( s ) ⋄ α s = − ∫ t a f ( s ) ⋄ α s ;</p><p>4) ∫ a t f ( s ) ⋄ α s = ∫ a b f ( s ) ⋄ α s + ∫ b t f ( s ) ⋄ α s ;</p><p>5) ∫ a a f ( s ) ⋄ α s = 0 .</p><p>We need the following results.</p><p>Theorem 6. [<xref ref-type="bibr" rid="scirp.81389-ref4">4</xref>] : Let a , b ∈ T and c , d ∈ ℝ . Suppose that g ∈ C ( [ a , b ] T , ( c , d ) ) and h ∈ C ( [ a , b ] T , ℝ ) with ∫ a b | h ( s ) | ⋄ α s &gt; 0 . If F ∈ C ( ( c , d ) , ℝ ) is convex, then generalized Jensen’s inequality is</p><p>F ( ∫ a b | h ( s ) | g ( s ) ⋄ α s ∫ a b | h ( s ) | ⋄ α s ) ≤ ∫ a b | h ( s ) | F ( g ( s ) ) ⋄ α s ∫ a b | h ( s ) | ⋄ α s . (3)</p><p>If F is strictly convex, then the inequality ≤ can be replaced by &lt; .</p><p>Theorem 7. [<xref ref-type="bibr" rid="scirp.81389-ref3">3</xref>] [<xref ref-type="bibr" rid="scirp.81389-ref10">10</xref>] : Let a , b ∈ T . Let f i ∈ C ( [ a , b ] T , ℝ ) , i = 1 , ⋯ , n are ⋄ α -</p><p>integrable functions and p i &gt; 1 such that ∑ i = 1 n 1 p i = 1 . Then</p><p>∫ a b ∏ i = 1 n | f i ( t ) | ⋄ α t ≤ ∏ i = 1 n ( ∫ a b | f i ( t ) | p i ⋄ α t ) 1 p i , (4)</p><p>which is generalized Rogers-H&#246;lder’s Inequality.</p><p>Definition 3. [<xref ref-type="bibr" rid="scirp.81389-ref11">11</xref>] : A function f : T → ℝ is called convex on I T = I ∩ T , where I is an interval of ℝ (open or closed), if</p><p>f ( λ t + ( 1 − λ ) s ) ≤ λ f ( t ) + ( 1 − λ ) f ( s ) , (5)</p><p>for all t , s ∈ I T and all λ ∈ [ 0,1 ] such that λ t + ( 1 − λ ) s ∈ I T .</p><p>The function f is strictly convex on I T if (5) is strict for distinct t , s ∈ I T and λ ∈ ( 0,1 ) .</p><p>The function f is concave (respectively, strictly concave) on I T , if − f is convex (respectively, strictly convex).</p></sec><sec id="s3"><title>3. Main Results</title><p>First we present ⋄ α -integral general fractional Schl&#246;milch’s type inequalities on time scales, which is an extension of Schl&#246;milch’s inequality given in [<xref ref-type="bibr" rid="scirp.81389-ref12">12</xref>] .</p><p>Theorem 8. Let [ a , b ] T 1 and [ c , d ] T 2 be two time scales;</p><p>k ( x , y ) : [ a , b ] T 1 &#215; [ c , d ] T 2 → ℝ 0 + is continuous kernel function with x ∈ [ a , b ] T 1 and y ∈ [ c , d ] T 2 . Let ⋄ α -integral operator functions g i : [ a , b ] T 1 → ℝ belonging to a class G ( f i , k ) for ( i = 1 , 2 ) are represented by</p><p>g i ( x ) : = ∫ c d k ( x , y ) f i ( y ) ⋄ α y ,</p><p>where f i : [ c , d ] T 2 → ℝ are continuous functions. Continuous weight function is defined by w : [ a , b ] T 1 → ℝ 0 + with ∫ a b w ( x ) ⋄ α x = 1 . Define</p><p>s ( y ) : = f 2 ( y ) ∫ a b w ( x ) k ( x , y ) g 2 ( x ) ⋄ α x and ∀ y ∈ [ c , d ] T 2 , where f 2 ( y ) &gt; 0 implies</p><p>g 2 ( x ) &gt; 0 . Let F : ℝ 0 + = [ 0, ∞ ) → ℝ 0 + be a convex and increasing function.</p><p>If η 2 ≥ η 1 ≥ 1 , then the following inequality holds</p><p>( ∫ a b w ( x ) F ( | g 1 ( x ) g 2 ( x ) | ) η 1 ⋄ α x ) 1 η 1 ≤ ( ∫ c d F ( | f 1 ( y ) f 2 ( y ) | ) η 2 s ( y ) ⋄ α y ) 1 η 2 . (6)</p><p>Proof. In order to prove this Theorem, we need Bernoulli’s inequality, that is, if x &gt; 0 , then</p><p>p x + 1 − p ≤ x p , if   p ≥ 1.</p><p>Since η 2 ≥ η 1 ≥ 1 , we have η 2 η 1 ≥ 1 . Thus, by Bernoulli’s inequality, we have</p><p>∫ a b w ( x ) ( F ( | g 1 ( x ) g 2 ( x ) | ) ∫ a b w ( x ) F ( | g 1 ( x ) g 2 ( x ) | ) ⋄ α x ) η 2 η 1 ⋄ α x ≥ ∫ a b w ( x ) ( η 2 η 1 F ( | g 1 ( x ) g 2 ( x ) | ) ∫ a b w ( x ) F ( | g 1 ( x ) g 2 ( x ) | ) ⋄ α x + 1 − η 2 η 1 ) ⋄ α x = 1 ,</p><p>that is,</p><p>∫ a b w ( x ) F ( | g 1 ( x ) g 2 ( x ) | ) η 2 η 1 ⋄ α x ≥ ( ∫ a b w ( x ) F ( | g 1 ( x ) g 2 ( x ) | ) ⋄ α x ) η 2 η 1 .</p><p>Let F be replaced by F η 1 and taking power 1 η 2 &gt; 0 , we get</p><p>( ∫ a b w ( x ) F ( | g 1 ( x ) g 2 ( x ) | ) η 1 ⋄ α x ) 1 η 1 ≤ ( ∫ a b w ( x ) F ( | g 1 ( x ) g 2 ( x ) | ) η 2 ⋄ α x ) 1 η 2 = ( ∫ a b w ( x ) F ( | ∫ c d k ( x , y ) f 1 ( y ) ⋄ α y g 2 ( x ) | ) η 2 ⋄ α x ) 1 η 2 = ( ∫ a b w ( x ) F ( | 1 g 2 ( x ) ∫ c d k ( x , y ) f 2 ( y ) f 1 ( y ) f 2 ( y ) ⋄ α y | ) η 2 ⋄ α x ) 1 η 2</p><p>≤ ( ∫ a b w ( x ) ( 1 g 2 ( x ) ∫ c d k ( x , y ) f 2 ( y ) F ( | f 1 ( y ) f 2 ( y ) | ) η 2 ⋄ α y ) ⋄ α x ) 1 η 2 = ( ∫ c d F ( | f 1 ( y ) f 2 ( y ) | ) η 2 ( f 2 ( y ) ∫ a b w ( x ) k ( x , y ) g 2 ( x ) ⋄ α x ) ⋄ α y ) 1 η 2 = ( ∫ c d F ( | f 1 ( y ) f 2 ( y ) | ) η 2 s ( y ) ⋄ α y ) 1 η 2 ,</p><p>where we used the generalized Jensen’s inequality and Fubini’s theorem.</p><p>This proves the claim. □</p><p>Remark. If we set η 1 = η 2 = 1 and F : [ 0, ∞ ) → ℝ be a convex and increasing function, then (6) takes the form</p><p>∫ a b w ( x ) F ( | g 1 ( x ) g 2 ( x ) | ) ⋄ α x ≤ ∫ c d F ( | f 1 ( y ) f 2 ( y ) | ) s ( y ) ⋄ α y . (7)</p><p>If [ a , b ] T 1 = [ c , d ] T 2 , where T 1 = T 2 = ℝ , then (7) takes the form of (1).</p><p>Corollary 1. If η 1 = η 2 = 1 , F : [ 0, ∞ ) → ℝ be a convex and increasing function and α = 1 , then delta version form of (6) is</p><p>∫ a b w ( x ) F ( | g 1 ( x ) g 2 ( x ) | ) Δ x ≤ ∫ c d F ( | f 1 ( y ) f 2 ( y ) | ) s ( y ) Δ y . (8)</p><p>If η 1 = η 2 = 1 , F : [ 0, ∞ ) → ℝ be a convex and increasing function and α = 0 , then nabla version form of (6) is</p><p>∫ a b w ( x ) F ( | g 1 ( x ) g 2 ( x ) | ) ∇ x ≤ ∫ c d F ( | f 1 ( y ) f 2 ( y ) | ) s ( y ) ∇ y . (9)</p><p>Remark. Now we take that F is not necessarily increasing and is taken from</p><p>( 0, ∞ ) into ℝ 0 + and f 1 ( y ) f 2 ( y ) has fixed and strict sign, then according to</p><p>Theorem 8, we get</p><p>( ∫ a b w ( x ) F ( | g 1 ( x ) g 2 ( x ) | ) η 1 ⋄ α x ) 1 η 1 ≤ ( ∫ c d F ( | f 1 ( y ) f 2 ( y ) | ) η 2 s ( y ) ⋄ α y ) 1 η 2 .</p><p>Corollary 2. If we apply for F ( x ) = x p , p &gt; 1 , then (6) takes the form</p><p>( ∫ a b w ( x ) ( | g 1 ( x ) g 2 ( x ) | ) p η 1 ⋄ α x ) 1 η 1 ≤ ( ∫ c d ( | f 1 ( y ) f 2 ( y ) | ) p η 2 s ( y ) ⋄ α y ) 1 η 2 . (10)</p><p>Corollary 3. If we apply for F ( x ) = e x , x ≥ 0 , then (6) takes the form</p><p>( ∫ a b w ( x ) e η 1 ( | g 1 ( x ) g 2 ( x ) | ) ⋄ α x ) 1 η 1 ≤ ( ∫ c d     e η 2 ( | f 1 ( y ) f 2 ( y ) | ) s ( y ) ⋄ α y ) 1 η 2 . (11)</p><p>Corollary 4. If η 1 = η 2 = 1 , F : ( 0, ∞ ) → ℝ be a convex and not necessarily</p><p>increasing function, f 1 ( y ) f 2 ( y ) has fixed and strict sign and we apply for</p><p>F ( x ) = − ln x , x &gt; 0 , then (6) takes the form</p><p>∫ a b w ( x ) ln ( | g 1 ( x ) g 2 ( x ) | ) ⋄ α x ≥ ∫ c d ln ( | f 1 ( y ) f 2 ( y ) | ) s ( y ) ⋄ α y . (12)</p><p>Remark. If we set f 2 ( y ) = 1 , g 1 ( x ) = g ( x ) , f 1 ( y ) = f ( y ) , η 1 = η 2 = 1 and F : [ 0, ∞ ) → ℝ be a convex and increasing function, then</p><p>g 2 ( x ) = ∫ c d k ( x , y ) ⋄ α y = K ( x ) , ∀ x ∈ [ a , b ] T 1 .</p><p>We assume that K ( x ) &gt; 0 , and define</p><p>s ( y ) : = ∫ a b w ( x ) k ( x , y ) K ( x ) ⋄ α x , ∀ y ∈ [ c , d ] T 2 .</p><p>Then (6) takes the form of (2), as proved in [<xref ref-type="bibr" rid="scirp.81389-ref3">3</xref>] .</p><p>Corollary 5. If we take T 1 = q ℕ 0 , q &gt; 1 , where ℕ 0 is the set of nonnegative integers and T 2 = ℝ .</p><p>Then</p><p>∫ q m q n f ( x ) ⋄ α x = ( q − 1 ) ∑ i = m n − 1     q i [ α f ( q i ) + ( 1 − α ) f ( q i + 1 ) ] ,</p><p>for [ a , b ] T 1 = [ q m , q n ] q ℕ 0 , m &lt; n , where m , n ∈ ℕ 0 .</p><p>And</p><p>∫ c d f ( y ) ⋄ α y = ∫ c d f ( y ) d y .</p><p>When η 1 = η 2 = 1 and F : [ 0, ∞ ) → ℝ be a convex and increasing function, then (6) can be written as</p><p>( q − 1 ) ∑ i = m n − 1     q i [ α w ( q i ) F ( | g 1 ( q i ) g 2 ( q i ) | ) + ( 1 − α ) w ( q i + 1 ) F ( | g 1 ( q i + 1 ) g 2 ( q i + 1 ) | ) ] ≤ ∫ c d F ( | f 1 ( y ) f 2 ( y ) | ) s ( y ) d y .</p><p>We can generalize Theorem 8 for convex functions of several variables on time scales in the upcoming theorem.</p><p>Theorem 9. Let [ a , b ] T 1 and [ c , d ] T 2 be two time scales;</p><p>k ( x , y ) : [ a , b ] T 1 &#215; [ c , d ] T 2 → ℝ 0 + is continuous kernel function with x ∈ [ a , b ] T 1 and y ∈ [ c , d ] T 2 . Let ⋄ α -integral operator functions g i : [ a , b ] T 1 → ℝ belonging to a class G ( f i , k ) for ( i = 1 , 2 , 3 ) are represented by</p><p>g i ( x ) : = ∫ c d k ( x , y ) f i ( y ) ⋄ α y ,</p><p>where f i : [ c , d ] T 2 → ℝ are continuous functions. Continuous weight function is defined by w : [ a , b ] T 1 → ℝ 0 + with ∫ a b w ( x ) ⋄ α x = 1 . Define</p><p>s ( y ) : = f 2 ( y ) ∫ a b w ( x ) k ( x , y ) g 2 ( x ) ⋄ α x and ∀ y ∈ [ c , d ] T 2 , where f 2 ( y ) &gt; 0 implies</p><p>g 2 ( x ) &gt; 0 . Let F : ℝ 0 + &#215; ℝ 0 + = [ 0, ∞ ) &#215; [ 0, ∞ ) → ℝ 0 + be a convex and increasing function.</p><p>If η 2 ≥ η 1 ≥ 1 , then the following inequality holds</p><p>( ∫ a b w ( x ) F ( | g 1 ( x ) g 2 ( x ) | , | g 3 ( x ) g 2 ( x ) | ) η 1 ⋄ α x ) 1 η 1 ≤ ( ∫ c d F ( | f 1 ( y ) f 2 ( y ) | , | f 3 ( y ) f 2 ( y ) | ) η 2 s ( y ) ⋄ α y ) 1 η 2 . (13)</p><p>Proof. Proof is similar to Theorem 8. □</p><p>Remark. If we set η 1 = η 2 = 1 , F : [ 0, ∞ ) &#215; [ 0, ∞ ) → ℝ be a convex and increasing function and [ a , b ] T 1 = [ c , d ] T 2 , where T 1 = T 2 = ℝ , then (13) reduces to</p><p>∫ a b w ( x ) F ( | g 1 ( x ) g 2 ( x ) | , | g 3 ( x ) g 2 ( x ) | ) d x ≤ ∫ a b F ( | f 1 ( y ) f 2 ( y ) | , | f 3 ( y ) f 2 ( y ) | ) s ( y ) d y ,</p><p>as given in ( [<xref ref-type="bibr" rid="scirp.81389-ref2">2</xref>] , p. 236).</p><p>Now we present ⋄ α -integral general fractional Rogers-Holder’s type inequalities.</p><p>Upcoming result is an application of general fractional Schl&#246;milch’s type dynamic inequality.</p><p>Theorem 10. Let [ a , b ] T 1 and [ c , d ] T 2 be two time scales; k i ( x , y ) : [ a , b ] T 1 &#215; [ c , d ] T 2 → ℝ 0 + for i = 1 , ⋯ , n ∈ ℕ are continuous kernel functions with x ∈ [ a , b ] T 1 and y ∈ [ c , d ] T 2 . Let ⋄ α -integral operator functions f i , g i : [ a , b ] T 1 → ℝ for i = 1 , ⋯ , n ∈ ℕ are represented by</p><p>f i ( x ) : = ∫ c d k i ( x , y ) u i ( y ) ⋄ α y ,</p><p>and</p><p>g i ( x ) : = ∫ c d k i ( x , y ) v i ( y ) ⋄ α y ,</p><p>where u i , v i : [ c , d ] T 2 → ℝ are continuous functions for i = 1 , ⋯ , n ∈ ℕ . Continuous weight function is defined by w : [ a , b ] T 1 → ℝ 0 + with</p><p>∫ a b w ( x ) ⋄ α x = 1 . Define s i ( y ) : = v i ( y ) ∫ a b w ( x ) k i ( x , y ) g i ( x ) ⋄ α x , and ∀ y ∈ [ c , d ] T 2 for</p><p>i = 1 , ⋯ , n ∈ ℕ , where v i ( y ) &gt; 0 implies g i ( x ) &gt; 0 for i = 1 , ⋯ , n ∈ ℕ . Let F i : ℝ 0 + → ℝ 0 + for i = 1 , ⋯ , n ∈ ℕ are convex and increasing functions.</p><p>If p i &gt; 1 with ∑ i = 1 n 1 p i &lt; 1 . Then the following inequality holds</p><p>∫ a b w ( x ) ∏ i = 1 n F i ( | f i ( x ) g i ( x ) | ) ⋄ α x ≤ ∏ i = 1 n ( ∫ c d F i ( | u i ( y ) v i ( y ) | ) p i s i ( y ) ⋄ α y ) 1 p i . (14)</p><p>Proof. Let γ : = ∑ i = 1 n 1 p i &lt; 1 and ζ i : = γ p i &lt; p i for i = 1 , ⋯ , n . Then ∑ i = 1 n 1 ζ i = 1 ,</p><p>where ζ i &gt; 1 for i = 1 , ⋯ , n . We use here generalized Rogers-H&#246;lder’s inequality, Schl&#246;milch’s inequality, generalized Jensen’s inequality and Fubini’s theorem, as</p><p>∫ a b w ( x ) ∏ i = 1 n F i ( | f i ( x ) g i ( x ) | ) ⋄ α x = ∫ a b ∏ i = 1 n ( w ( x ) 1 ζ i F i ( | f i ( x ) g i ( x ) | ) ) ⋄ α x ≤ ∏ i = 1 n ( ∫ a b w ( x ) F i ( | f i ( x ) g i ( x ) | ) ζ i ⋄ α x ) 1 ζ i</p><p>≤ ∏ i = 1 n ( ∫ a b w ( x ) F i ( | f i ( x ) g i ( x ) | ) p i ⋄ α x ) 1 p i = ∏ i = 1 n ( ∫ a b w ( x ) F i ( | ∫ c d k i ( x , y ) u i ( y ) ⋄ α y g i ( x ) | ) p i ⋄ α x ) 1 p i</p><p>= ∏ i = 1 n ( ∫ a b w ( x ) F i ( | 1 g i ( x ) ∫ c d k i ( x , y ) v i ( y ) u i ( y ) v i ( y ) ⋄ α y | ) p i ⋄ α x ) 1 p i ≤ ∏ i = 1 n ( ∫ a b w ( x ) ( 1 g i ( x ) ∫ c d k i ( x , y ) v i ( y ) F i ( | u i ( y ) v i ( y ) | ) p i ⋄ α y ) ⋄ α x ) 1 p i = ∏ i = 1 n ( ∫ c d F i ( | u i ( y ) v i ( y ) | ) p i ( v i ( y ) ∫ a b w ( x ) k i ( x , y ) g i ( x ) ⋄ α x ) ⋄ α y ) 1 p i = ∏ i = 1 n ( ∫ c d F i ( | u i ( y ) v i ( y ) | ) p i s i ( y ) ⋄ α y ) 1 p i .</p><p>This proves the claim. □</p><p>Corollary 6. If we apply for F i ( x ) = x ξ i , x ≥ 0 , i = 1 , ⋯ , n and let ξ i ≥ 1 , i = 1 , ⋯ , n . Then (14) takes the form</p><p>∫ a b w ( x ) ∏ i = 1 n ( | f i ( x ) g i ( x ) | ) ξ i ⋄ α x ≤ ∏ i = 1 n ( ∫ c d ( | u i ( y ) v i ( y ) | ) ξ i p i s i ( y ) ⋄ α y ) 1 p i . (15)</p></sec><sec id="s4"><title>4. Conclusion and Future Work</title><p>The study of dynamic inequalities on time scales has a lot of scope. This research article is devoted to some general fractional Schl&#246;milch’s type and Rogers-H&#246;lder’s type dynamic inequalities for convex functions harmonized on diamond-α calculus and their delta and nabla versions are similar cases. Similarly, in future, we can present such inequalities by using Riemann-Liouville type fractional integrals and fractional derivatives on time scales. It will also be very interesting to present such inequalities on quantum calculus.</p></sec><sec id="s5"><title>Cite this paper</title><p>Sahir, M.J.S. 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