Prerequisite concepts
One can view $\frac{df}{dx}$ as approximately given by a fraction where $df$ is a small change in $f$ and $dx$ is a small change in $x$.
One of Zandieh's process-object layers for derivatives is that derivatives are functions. This means that the value of a derivative depends on where in the domain of the function one is looking. The derivative of a function is itself a function, with the same domain as the original function. Both the (derivative) function and the value of the derivative at a point are commonly referred to as "the derivative."
When taking a derivative of a multivariable function, it is possible to consider a simpler situation in which some of the variables are considered to be constant.
Derivatives of multivariable functions can be found by holding one or more variables constant (subject to physical limitations).
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One typical notation used for derivatives is Leibniz notation ($e.g.,$ $df/dx$). Physicists often think of the $df$ and $dx$ as distinct quantities (``differentials'') that can be measured, calculated, and manipulated independent of one another. In particular, a differential can be thought of as the (small) change in a quantity when a small change is made to a physical system. A differential can also be thought of as the difference between the values of a quantity between two different (nearby) physical states. This line of thinking is also valuable for thinking about integration in physical situations.
FIXME: Does the difference between zapping with d and taking the total differential need to be articulated?
FIXME: What? One can do algebra with differentials and reinterpret them as partial derivatives. Can treat like a variable
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Chain Rules
FIXME: NOT CORRECT DESCRIPTION: In this activity, students experimentally determine various derivatives using the partial derivate machine, a mechanical analogue for thermodynamic systems. Students explore the ratio, limit, and function aspects of multi-variable derivatives, with an emphasis on holding different variables constant. This activity is also an excellent exercise in representational fluency, as students must coordinate experiments and tables of data with (new) symbolic notations.
Representations used
Concepts taught
While it may be possible to conceptualize a particular derivative, such as $\left(\frac{\partial U}{\partial S}\right)_{V},$ Where $U$ is internal energy, $S$ is entropy, and $V$ is volume, that does not mean that the particular derivative can be directly measured. In the above example, the entropy $S$ is not measurable.
Because total differentials are linear, one can find the total differential and then solve algebraically to obtain partial derivatives that might not be obtainable though differentiation.
In other words,[\left(\frac{\partial y}{\partial z}\right)_z = \frac1{\left(\frac{\partial x}{\partial y}\right)_z}] Note that this equality is only true if the same variables are being held fixed on each side of the equality. This therefore relies on the thermodynamics notation that specifies what quantities are being held fixed for a partial derivative.