<p>We derive a generalized Euler equation, <i>ϵ</i> + <i>p</i> = <i>sT</i> + <i>μq</i> + <InlineEquation ID="IEq1"> <EquationSource Format="MATHML"><math display="inline"> <mi>y</mi> <mfrac> <mrow> <mi>∂</mi> <mi>p</mi> </mrow> <mrow> <mi>∂</mi> <mi>y</mi> </mrow> </mfrac> </math></EquationSource> <EquationSource Format="TEX">\( y\frac{\partial p}{\partial y} \)</EquationSource> </InlineEquation>, using the effective field theory formulation of perfect fluids. This generalization was achieved by introducing a new variable <i>y</i> into the effective action, which encodes a geometrical scale of the spacetime where the fluid is on. Notably, the generalized Euler equation is independent of the AdS/CFT correspondence. However, when applied to a holographic perfect fluid, this equation naturally recovers the Smarr formula for AdS black holes, thus situating the physical interpretation of the Smarr formula within the framework of well-established physics. Finally, our findings raise important questions regarding the validity of treating the cosmological constant Λ as a thermodynamic variable, as proposed in certain frameworks within the literature.</p>

错误:搜索内容不能为空,请输入英文关键词
错误:关键词超出字数限制,请精简
高级检索

Generalized Euler equation from effective action: implications for the smarr formula in AdS black holes

  • Robinson Mancilla

摘要

We derive a generalized Euler equation, ϵ + p = sT + μq + y p y \( y\frac{\partial p}{\partial y} \) , using the effective field theory formulation of perfect fluids. This generalization was achieved by introducing a new variable y into the effective action, which encodes a geometrical scale of the spacetime where the fluid is on. Notably, the generalized Euler equation is independent of the AdS/CFT correspondence. However, when applied to a holographic perfect fluid, this equation naturally recovers the Smarr formula for AdS black holes, thus situating the physical interpretation of the Smarr formula within the framework of well-established physics. Finally, our findings raise important questions regarding the validity of treating the cosmological constant Λ as a thermodynamic variable, as proposed in certain frameworks within the literature.