<p>Consider a fixed angle <InlineEquation ID="IEq1"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="22_2025_750_Article_IEq1.gif" Format="GIF" Height="19" Rendition="HTML" Resolution="72" Type="Linedraw" Width="71" /> </InlineMediaObject> <EquationSource Format="TEX">\(\alpha \in (0,\pi )\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>α</mi> <mo>∈</mo> <mo stretchy="false">(</mo> <mn>0</mn> <mo>,</mo> <mi>π</mi> <mo stretchy="false">)</mo> </mrow> </math></EquationSource> </InlineEquation> and a disc <i>B</i>. All the chords <InlineEquation ID="IEq2"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="22_2025_750_Article_IEq2.gif" Format="GIF" Height="19" Rendition="HTML" Resolution="72" Type="Linedraw" Width="46" /> </InlineMediaObject> <EquationSource Format="TEX">\([z_1,z_2]\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mo stretchy="false">[</mo> <msub> <mi>z</mi> <mn>1</mn> </msub> <mo>,</mo> <msub> <mi>z</mi> <mn>2</mn> </msub> <mo stretchy="false">]</mo> </mrow> </math></EquationSource> </InlineEquation> of <i>B</i> such that the tangent lines of <i>B</i> at <InlineEquation ID="IEq3"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="22_2025_750_Article_IEq3.gif" Format="GIF" Height="12" Rendition="HTML" Resolution="72" Type="Linedraw" Width="15" /> </InlineMediaObject> <EquationSource Format="TEX">\(z_1\)</EquationSource> <EquationSource Format="MATHML"><math> <msub> <mi>z</mi> <mn>1</mn> </msub> </math></EquationSource> </InlineEquation> and <InlineEquation ID="IEq4"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="22_2025_750_Article_IEq4.gif" Format="GIF" Height="12" Rendition="HTML" Resolution="72" Type="Linedraw" Width="15" /> </InlineMediaObject> <EquationSource Format="TEX">\(z_2\)</EquationSource> <EquationSource Format="MATHML"><math> <msub> <mi>z</mi> <mn>2</mn> </msub> </math></EquationSource> </InlineEquation> intersect at an angle <InlineEquation ID="IEq5"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="22_2025_750_Article_IEq5.gif" Format="GIF" Height="10" Rendition="HTML" Resolution="72" Type="Linedraw" Width="14" /> </InlineMediaObject> <EquationSource Format="TEX">\(\alpha \)</EquationSource> <EquationSource Format="MATHML"><math> <mi>α</mi> </math></EquationSource> </InlineEquation> (<InlineEquation ID="IEq6"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="22_2025_750_Article_IEq5.gif" Format="GIF" Height="10" Rendition="HTML" Resolution="72" Type="Linedraw" Width="14" /> </InlineMediaObject> <EquationSource Format="TEX">\(\alpha \)</EquationSource> <EquationSource Format="MATHML"><math> <mi>α</mi> </math></EquationSource> </InlineEquation>-chords), have the same length. It is known that under certain circumstances, a convex body with <InlineEquation ID="IEq7"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="22_2025_750_Article_IEq5.gif" Format="GIF" Height="10" Rendition="HTML" Resolution="72" Type="Linedraw" Width="14" /> </InlineMediaObject> <EquationSource Format="TEX">\(\alpha \)</EquationSource> <EquationSource Format="MATHML"><math> <mi>α</mi> </math></EquationSource> </InlineEquation>-chords of constant length is a disc. It is also known that a convex body, whose isoptic chords have constant length for angles <InlineEquation ID="IEq8"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="22_2025_750_Article_IEq5.gif" Format="GIF" Height="10" Rendition="HTML" Resolution="72" Type="Linedraw" Width="14" /> </InlineMediaObject> <EquationSource Format="TEX">\(\alpha \)</EquationSource> <EquationSource Format="MATHML"><math> <mi>α</mi> </math></EquationSource> </InlineEquation> and <InlineEquation ID="IEq9"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="22_2025_750_Article_IEq9.gif" Format="GIF" Height="13" Rendition="HTML" Resolution="72" Type="Linedraw" Width="46" /> </InlineMediaObject> <EquationSource Format="TEX">\(\pi -\alpha \)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>π</mi> <mo>-</mo> <mi>α</mi> </mrow> </math></EquationSource> </InlineEquation> must be a disc, when <InlineEquation ID="IEq10"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="22_2025_750_Article_IEq10.gif" Format="GIF" Height="20" Rendition="HTML" Resolution="72" Type="Linedraw" Width="11" /> </InlineMediaObject> <EquationSource Format="TEX">\(\frac{\alpha }{\pi }\)</EquationSource> <EquationSource Format="MATHML"><math> <mfrac> <mi>α</mi> <mi>π</mi> </mfrac> </math></EquationSource> </InlineEquation> is an irrational number or <InlineEquation ID="IEq11"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="22_2025_750_Article_IEq11.gif" Format="GIF" Height="22" Rendition="HTML" Resolution="72" Type="Linedraw" Width="75" /> </InlineMediaObject> <EquationSource Format="TEX">\(\alpha =\frac{p}{2r+1}\pi \)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>α</mi> <mo>=</mo> <mfrac> <mi>p</mi> <mrow> <mn>2</mn> <mi>r</mi> <mo>+</mo> <mn>1</mn> </mrow> </mfrac> <mi>π</mi> </mrow> </math></EquationSource> </InlineEquation>, where <i>p</i> and <i>r</i> are natural numbers. In this article we present a proof for the general case of this last statement. The set of points under which a convex body <i>K</i> is seen at an angle <InlineEquation ID="IEq12"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="22_2025_750_Article_IEq5.gif" Format="GIF" Height="10" Rendition="HTML" Resolution="72" Type="Linedraw" Width="14" /> </InlineMediaObject> <EquationSource Format="TEX">\(\alpha \)</EquationSource> <EquationSource Format="MATHML"><math> <mi>α</mi> </math></EquationSource> </InlineEquation> is known as the isoptic of angle <InlineEquation ID="IEq13"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="22_2025_750_Article_IEq5.gif" Format="GIF" Height="10" Rendition="HTML" Resolution="72" Type="Linedraw" Width="14" /> </InlineMediaObject> <EquationSource Format="TEX">\(\alpha \)</EquationSource> <EquationSource Format="MATHML"><math> <mi>α</mi> </math></EquationSource> </InlineEquation> for <i>K</i>. The pair of isoptics of angles <InlineEquation ID="IEq14"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="22_2025_750_Article_IEq5.gif" Format="GIF" Height="10" Rendition="HTML" Resolution="72" Type="Linedraw" Width="14" /> </InlineMediaObject> <EquationSource Format="TEX">\(\alpha \)</EquationSource> <EquationSource Format="MATHML"><math> <mi>α</mi> </math></EquationSource> </InlineEquation> and <InlineEquation ID="IEq15"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="22_2025_750_Article_IEq9.gif" Format="GIF" Height="13" Rendition="HTML" Resolution="72" Type="Linedraw" Width="46" /> </InlineMediaObject> <EquationSource Format="TEX">\(\pi -\alpha \)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>π</mi> <mo>-</mo> <mi>α</mi> </mrow> </math></EquationSource> </InlineEquation> is called a bisoptic for <i>K</i>. We also give some characterizations of the disc and figures of constant widht in terms of properties of their bisoptics.</p>

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Some results on bisoptic curves

  • V. A. Aguilar-Arteaga,
  • R. I. Ayala-Figueroa,
  • J. Jerónimo-Castro,
  • F. G. Jimenez-Lopez

摘要

Consider a fixed angle \(\alpha \in (0,\pi )\) α ( 0 , π ) and a disc B. All the chords \([z_1,z_2]\) [ z 1 , z 2 ] of B such that the tangent lines of B at \(z_1\) z 1 and \(z_2\) z 2 intersect at an angle \(\alpha \) α ( \(\alpha \) α -chords), have the same length. It is known that under certain circumstances, a convex body with \(\alpha \) α -chords of constant length is a disc. It is also known that a convex body, whose isoptic chords have constant length for angles \(\alpha \) α and \(\pi -\alpha \) π - α must be a disc, when \(\frac{\alpha }{\pi }\) α π is an irrational number or \(\alpha =\frac{p}{2r+1}\pi \) α = p 2 r + 1 π , where p and r are natural numbers. In this article we present a proof for the general case of this last statement. The set of points under which a convex body K is seen at an angle \(\alpha \) α is known as the isoptic of angle \(\alpha \) α for K. The pair of isoptics of angles \(\alpha \) α and \(\pi -\alpha \) π - α is called a bisoptic for K. We also give some characterizations of the disc and figures of constant widht in terms of properties of their bisoptics.