<p>In this manuscript, we propose a simplified mathematical model based on the heat transfer laws to predict the temperature profiles of a liquid controlled by a simple thermostat. The model result in a set of linear ordinary differential equations ODEs with forcing which turn on and off at a priori unknown times <InlineEquation ID="IEq1"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="10665_2024_10416_Article_IEq1.gif" Format="GIF" Height="19" Rendition="HTML" Resolution="72" Type="Linedraw" Width="160" /> </InlineMediaObject> <EquationSource Format="TEX">\({\mathcal {T}}_M=\left\{ \zeta _0,\zeta _1,\ldots ,\zeta _M\right\} \)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <msub> <mi mathvariant="script">T</mi> <mi>M</mi> </msub> <mo>=</mo> <mfenced close="}" open="{"> <msub> <mi>ζ</mi> <mn>0</mn> </msub> <mo>,</mo> <msub> <mi>ζ</mi> <mn>1</mn> </msub> <mo>,</mo> <mo>…</mo> <mo>,</mo> <msub> <mi>ζ</mi> <mi>M</mi> </msub> </mfenced> </mrow> </math></EquationSource> </InlineEquation>. The <i>p</i>th switch-time <InlineEquation ID="IEq2"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="10665_2024_10416_Article_IEq2.gif" Format="GIF" Height="19" Rendition="HTML" Resolution="72" Type="Linedraw" Width="54" /> </InlineMediaObject> <EquationSource Format="TEX">\(\zeta _p\in {\mathcal {T}}_p\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <msub> <mi>ζ</mi> <mi>p</mi> </msub> <mo>∈</mo> <msub> <mi mathvariant="script">T</mi> <mi>p</mi> </msub> </mrow> </math></EquationSource> </InlineEquation> is calculated from the zeros of a function <InlineEquation ID="IEq3"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="10665_2024_10416_Article_IEq3.gif" Format="GIF" Height="20" Rendition="HTML" Resolution="72" Type="Linedraw" Width="186" /> </InlineMediaObject> <EquationSource Format="TEX">\({\mathcal {Q}}(\chi )={\mathcal {Q}}(\chi ;\zeta _1,\ldots ,\zeta _{p-1})\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi mathvariant="script">Q</mi> <mrow> <mo stretchy="false">(</mo> <mi>χ</mi> <mo stretchy="false">)</mo> </mrow> <mo>=</mo> <mi mathvariant="script">Q</mi> <mrow> <mo stretchy="false">(</mo> <mi>χ</mi> <mo>;</mo> <msub> <mi>ζ</mi> <mn>1</mn> </msub> <mo>,</mo> <mo>…</mo> <mo>,</mo> <msub> <mi>ζ</mi> <mrow> <mi>p</mi> <mo>-</mo> <mn>1</mn> </mrow> </msub> <mo stretchy="false">)</mo> </mrow> </mrow> </math></EquationSource> </InlineEquation> coming from analytical solutions of the system depending on the previous times <InlineEquation ID="IEq4"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="10665_2024_10416_Article_IEq4.gif" Format="GIF" Height="19" Rendition="HTML" Resolution="72" Type="Linedraw" Width="83" /> </InlineMediaObject> <EquationSource Format="TEX">\(\zeta _1,\ldots ,\zeta _{p-1}\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <msub> <mi>ζ</mi> <mn>1</mn> </msub> <mo>,</mo> <mo>…</mo> <mo>,</mo> <msub> <mi>ζ</mi> <mrow> <mi>p</mi> <mo>-</mo> <mn>1</mn> </mrow> </msub> </mrow> </math></EquationSource> </InlineEquation>. The mathematical problem can be solved by using standard techniques for solving ODEs once <InlineEquation ID="IEq5"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="10665_2024_10416_Article_IEq5.gif" Format="GIF" Height="16" Rendition="HTML" Resolution="72" Type="Linedraw" Width="24" /> </InlineMediaObject> <EquationSource Format="TEX">\({\mathcal {T}}_M\)</EquationSource> <EquationSource Format="MATHML"><math> <msub> <mi mathvariant="script">T</mi> <mi>M</mi> </msub> </math></EquationSource> </InlineEquation> is calculated by <i>M</i>-successive iterations of the conditional expression <InlineEquation ID="IEq6"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="10665_2024_10416_Article_IEq6.gif" Format="GIF" Height="20" Rendition="HTML" Resolution="72" Type="Linedraw" Width="105" /> </InlineMediaObject> <EquationSource Format="TEX">\({\mathcal {Q}}(\chi =\zeta _p)=0\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi mathvariant="script">Q</mi> <mo stretchy="false">(</mo> <mi>χ</mi> <mo>=</mo> <msub> <mi>ζ</mi> <mi>p</mi> </msub> <mo stretchy="false">)</mo> <mo>=</mo> <mn>0</mn> </mrow> </math></EquationSource> </InlineEquation> and the Newton–Raphson method. We provide analytical expressions for the temperature as a function of time and <InlineEquation ID="IEq7"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="10665_2024_10416_Article_IEq7.gif" Format="GIF" Height="16" Rendition="HTML" Resolution="72" Type="Linedraw" Width="24" /> </InlineMediaObject> <EquationSource Format="TEX">\({\mathcal {T}}_M\)</EquationSource> <EquationSource Format="MATHML"><math> <msub> <mi mathvariant="script">T</mi> <mi>M</mi> </msub> </math></EquationSource> </InlineEquation> considering direct (DC) and alternate (AC) feeding voltages. We solve the system using this numerical-analytical approach and compare it with the results of the 4th Runge–Kutta method finding a good agreement between both methods.</p>

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Simple thermodynamic model of thermostats for a liquid into a tank: an analytical approach

  • Robert Salazar,
  • Felipe Deaza,
  • José Zamudio,
  • Leonardo García

摘要

In this manuscript, we propose a simplified mathematical model based on the heat transfer laws to predict the temperature profiles of a liquid controlled by a simple thermostat. The model result in a set of linear ordinary differential equations ODEs with forcing which turn on and off at a priori unknown times \({\mathcal {T}}_M=\left\{ \zeta _0,\zeta _1,\ldots ,\zeta _M\right\} \) T M = ζ 0 , ζ 1 , , ζ M . The pth switch-time \(\zeta _p\in {\mathcal {T}}_p\) ζ p T p is calculated from the zeros of a function \({\mathcal {Q}}(\chi )={\mathcal {Q}}(\chi ;\zeta _1,\ldots ,\zeta _{p-1})\) Q ( χ ) = Q ( χ ; ζ 1 , , ζ p - 1 ) coming from analytical solutions of the system depending on the previous times \(\zeta _1,\ldots ,\zeta _{p-1}\) ζ 1 , , ζ p - 1 . The mathematical problem can be solved by using standard techniques for solving ODEs once \({\mathcal {T}}_M\) T M is calculated by M-successive iterations of the conditional expression \({\mathcal {Q}}(\chi =\zeta _p)=0\) Q ( χ = ζ p ) = 0 and the Newton–Raphson method. We provide analytical expressions for the temperature as a function of time and \({\mathcal {T}}_M\) T M considering direct (DC) and alternate (AC) feeding voltages. We solve the system using this numerical-analytical approach and compare it with the results of the 4th Runge–Kutta method finding a good agreement between both methods.