On Liouville type theorems for the steady Navier-Stokes equations in
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In this paper we prove three different Liouville type theorems for the steady Navier&ndash;Stokes equations in <span id="mmlsi1" class="mathmlsrc"><span class="formulatext stixSupport mathImg" data-mathURL="/science?_ob=MathURL&_method=retrieve&_eid=1-s2.0-S0022039616302194&_mathId=si1.gif&_user=111111111&_pii=S0022039616302194&_rdoc=1&_issn=00220396&md5=69a54831ff1daf12cb981ef6aa1f53f0" title="Click to view the MathML source">R<sup>3sup>span><span class="mathContainer hidden"><span class="mathCode">si1.gif" overflow="scroll">sup>struck">R3sup>span>span>span>. In the first theorem we improve logarithmically the well-known <span id="mmlsi2" class="mathmlsrc">source" class="mathImg" data-mathURL="/science?_ob=MathURL&_method=retrieve&_eid=1-s2.0-S0022039616302194&_mathId=si2.gif&_user=111111111&_pii=S0022039616302194&_rdoc=1&_issn=00220396&md5=62358d6aa384b8c236d18e186eb0d91a">ss="imgLazyJSB inlineImage" height="21" width="51" alt="View the MathML source" title="View the MathML source" src="/sd/grey_pxl.gif" data-inlimgeid="1-s2.0-S0022039616302194-si2.gif">script>style="vertical-align:bottom" width="51" alt="View the MathML source" title="View the MathML source" src="http://origin-ars.els-cdn.com/content/image/1-s2.0-S0022039616302194-si2.gif">script><span class="mathContainer hidden"><span class="mathCode">si2.gif" overflow="scroll">sup>L92sup>stretchy="false">(sup>struck">R3sup>stretchy="false">)span>span>span> result. In the second theorem we present a sufficient condition for the trivially of the solution (<span id="mmlsi28" class="mathmlsrc"><span class="formulatext stixSupport mathImg" data-mathURL="/science?_ob=MathURL&_method=retrieve&_eid=1-s2.0-S0022039616302194&_mathId=si28.gif&_user=111111111&_pii=S0022039616302194&_rdoc=1&_issn=00220396&md5=f91db8c2fe7631618ddb1d9e2aa1e1a5" title="Click to view the MathML source">v=0span><span class="mathContainer hidden"><span class="mathCode">si28.gif" overflow="scroll">v=0span>span>span>) in terms of the head pressure, <span id="mmlsi4" class="mathmlsrc">source" class="mathImg" data-mathURL="/science?_ob=MathURL&_method=retrieve&_eid=1-s2.0-S0022039616302194&_mathId=si4.gif&_user=111111111&_pii=S0022039616302194&_rdoc=1&_issn=00220396&md5=91b699a75f0e3e3c37ab4406ec9b2a5e">ss="imgLazyJSB inlineImage" height="22" width="96" alt="View the MathML source" title="View the MathML source" src="/sd/grey_pxl.gif" data-inlimgeid="1-s2.0-S0022039616302194-si4.gif">script>style="vertical-align:bottom" width="96" alt="View the MathML source" title="View the MathML source" src="http://origin-ars.els-cdn.com/content/image/1-s2.0-S0022039616302194-si4.gif">script><span class="mathContainer hidden"><span class="mathCode">si4.gif" overflow="scroll">Q=12stretchy="false">|vsup>stretchy="false">|2sup>+pspan>span>span>. The imposed integrability condition here has the same scaling property as the Dirichlet integral. In the last theorem we present Fubini type condition, which guarantee <span id="mmlsi28" class="mathmlsrc"><span class="formulatext stixSupport mathImg" data-mathURL="/science?_ob=MathURL&_method=retrieve&_eid=1-s2.0-S0022039616302194&_mathId=si28.gif&_user=111111111&_pii=S0022039616302194&_rdoc=1&_issn=00220396&md5=f91db8c2fe7631618ddb1d9e2aa1e1a5" title="Click to view the MathML source">v=0span><span class="mathContainer hidden"><span class="mathCode">si28.gif" overflow="scroll">v=0span>span>span>.

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