Proving the reciprocal relation between partial derivatives

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SUMMARY

The discussion centers on proving the reciprocal relationship between partial derivatives when three variables \(x\), \(y\), and \(z\) are constrained by a function \(F(x,y,z) = \text{constant}\). The correct approach involves using the implicit function theorem, which states that if \(F_x(x,y,z) \neq 0\), then \(x\) can be expressed in terms of \(y\) and \(z\). By applying the chain rule, the relationship \(\frac{\partial x}{\partial y} = -\frac{F_y}{F_x}\) is derived, confirming the reciprocity of partial derivatives. Additionally, the identity \(\frac{\partial x}{\partial y} \frac{\partial y}{\partial z} \frac{\partial z}{\partial x} = -1\) is established under the condition that all partial derivatives are non-zero.

PREREQUISITES
  • Understanding of partial derivatives and their notation
  • Familiarity with the implicit function theorem
  • Knowledge of the chain rule in calculus
  • Basic concepts of multivariable functions
NEXT STEPS
  • Study the implicit function theorem in detail
  • Learn about the chain rule and its applications in multivariable calculus
  • Explore examples of reciprocal relationships in partial derivatives
  • Investigate conditions under which partial derivatives are defined and non-zero
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Mathematicians, students of calculus, and anyone studying multivariable functions and their derivatives will benefit from this discussion.

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If three variables [itex]x,y[/itex] and [itex]z[/itex] are related via some condition that can be expressed as $$F(x,y,z)=constant$$ then the partial derivatives of the functions are reciprocal, e.g. $$\frac{\partial x}{\partial y}=\frac{1}{\frac{\partial y}{\partial x}}$$ Is the correct way to prove this the following.

As [itex]x,y[/itex] and [itex]z[/itex] are related by [itex]F(x,y,z)=constant[/itex], at most only two of the variables can be independent (as the third can be expressed in terms of the other two). Consider the differentials $$dx=\frac{\partial x}{\partial y}dy+\frac{\partial x}{\partial z}dz$$ $$dy=\frac{\partial y}{\partial x}dx+\frac{\partial y}{\partial z}dz$$
Substituting the second expression into the first gives $$dx=\frac{\partial x}{\partial y}\left(\frac{\partial y}{\partial x}dx+\frac{\partial y}{\partial z}dz\right)+\frac{\partial x}{\partial z}dz \\ \Rightarrow\;\;\left(1-\frac{\partial x}{\partial y}\frac{\partial y}{\partial x}\right)dx=\left(\frac{\partial x}{\partial y}\frac{\partial y}{\partial z}+\frac{\partial x}{\partial z}\right)dz$$

Now, we choose [itex]x[/itex] and [itex]z[/itex] to be the independent variables, and as such, for this equality to be true [itex]\forall\; x,z[/itex] it must be that the terms in the brackets vanish identically. We see then, from the left-hand side of the equality, that $$\left(1-\frac{\partial x}{\partial y}\frac{\partial y}{\partial x}\right)=0\;\;\Rightarrow\;\;\frac{\partial x}{\partial y}=\frac{1}{\frac{\partial y}{\partial x}}$$ and from the right-hand side $$\left(\frac{\partial x}{\partial y}\frac{\partial y}{\partial z}+\frac{\partial x}{\partial z}\right)=0\;\;\Rightarrow\;\;\frac{\partial x}{\partial y}\frac{\partial y}{\partial z}=-\frac{\partial x}{\partial z}$$ and hence together this gives the relation $$\frac{\partial x}{\partial y}\frac{\partial y}{\partial z}\frac{\partial z}{\partial x}=-1.$$
 
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You should just use implicit function theorem here. You calculations are too complicated, and I do not see an easy way to justify them. In particular the phrase "at most only two of the variables can be independent" is too vague.

To be rigorous one should work in terms of functions and not variables.

The implicit function theorem gives you that if at some point ##F_x(x,y,z)\ne 0## then in a neighborhood of this point ##x## can be expressed in terms of ##y## and ##z##. Writing $$F(x(y,z),y,z)=C$$ and taking partial with respect to ##y## you get using chain rule that
$$F_x \frac{\partial x}{\partial y} + F_y =0,$$ so $$\frac{\partial x}{\partial y} = - F_y/F_x$$ Similarly $$\frac{\partial y}{\partial x} = - F_x/F_y,$$ and you get reciprocity. Your last identity also can be easily obtained this way (it holds when all 3 partials ##F_x##, ##F_y## and ##F_z## are non-zero).
 
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