Vector Calculus: Level curves and insulated boundaries

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SUMMARY

This discussion focuses on the relationship between isobars, which are lines of constant temperature, and insulated boundaries in vector calculus. The key conclusion is that isobars are indeed perpendicular to any part of an insulated boundary, as demonstrated by the condition \nabla{u}\cdot\underline{n} = 0, where \underline{n} is the outward normal vector. The reasoning involves analyzing the gradient \nabla{u} and its relationship to tangent lines at points on the boundary, confirming that the gradient lies in the tangent hyperplane, thus establishing the perpendicularity of isobars to the boundary. Additionally, it clarifies that isobars represent constant pressure rather than temperature.

PREREQUISITES
  • Understanding of vector calculus concepts, specifically gradients and normal vectors.
  • Familiarity with the concept of isobars in thermodynamics.
  • Knowledge of the mathematical notation used in multivariable calculus.
  • Basic principles of boundary conditions in heat transfer problems.
NEXT STEPS
  • Study the implications of the gradient vector in thermodynamic systems.
  • Learn about the mathematical properties of isobars in fluid dynamics.
  • Explore the concept of insulated boundaries in heat transfer and its mathematical representation.
  • Investigate the relationship between pressure and temperature in thermodynamic processes.
USEFUL FOR

Students and professionals in physics, engineering, and mathematics who are studying thermodynamics, vector calculus, or heat transfer principles will benefit from this discussion.

end3r7
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Need help checking if my reasoning is sound for this.

Homework Statement


Isobars are lines of constant temperature. Show that isobars are perpendicular to any part of the boundary that is insulated.


Homework Equations


u(t,\underline{X}) is the temperature at time t and spatial location \underline{X}

Let V be the region of the interest, then the at the points in the boundary of V, we have \nabla{u}\cdot\underline{n} = 0 (insulation), where \underline{n} is the outward normal at that point.


The Attempt at a Solution


Consider, for a fixed time t = \alpha, the isobar u(\alpha,\underline{X}(s)) = C, where C is an arbitrary constant and s parametrizes a curve \partial{X}in n-dimensional space. Its derivative for a fixed time is \displaystyle \displaystyle \frac{du}{ds} = \nabla{u}\cdot\frac{d\underline{X}(s)}{ds} = 0. Therefore, the gradient \nabla{u} is perpendicular to the tangent line.

Next, consider a point X = X_{0} in an insulated boundary \nabla{u(t,X_{0})}\cdot\underline{n} = 0 \forall t, where \underline{n} is understood as the outward normal to the boundary at X = X_{0}, which means that the gradient \nabla{u} at that point lies in the tangent n-1 hyperplane.

This means that at X = X_{0}, the tangent of \partial{X} lies normal to the n-1 tangent hyperplane, and they are thus perpendicular.
 
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Actually isobars are curves of constant pressure not temperature. ("bar" is from "barometric"). I'm not sure if there is a special name for constant temperature.

If T(x,y,z) is the temperature at the point (x,y,z) then \nabla f\cdot\vec{v} is the rate of change of T in the direction of the unit vector \vec{v}. In particular, if \vec{v} is tangent to a curve of constant temperature then \nabla T\cdot\vec{v}= 0 because T does not change in that direction. Combine that with the condition on an insulated boundary.
 
Then, errr, isn't that what I wrote?
 

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