When do total differentials cancel with partial derivatives

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Total differentials can cancel with partial derivatives under specific conditions, particularly when applying the multivariable chain rule. This cancellation is often seen in general relativity derivations, but clarity on its applicability in inertial coordinates is necessary. The discussion emphasizes that derivatives, whether ordinary or partial, should not be treated as fractions, and the chain rule does not involve cancellation in a traditional sense. The conversation highlights the importance of understanding the underlying principles rather than relying on mnemonic devices. Overall, a deeper comprehension of the chain rule and the nature of derivatives is essential for accurate application in mathematical contexts.
sunrah
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I've just done a derivation and had to use the following

u_{b}u^{c}\partial_{c}\rho = u_{b}\frac{dx^{c}}{d\tau}\frac{\partial\rho}{\partial x^{c}} = u_{b}\frac{d\rho}{d\tau}

We've done this cancellation a lot during my GR course, but I'm not clear exactly when/why this is possible.

EDIT: is this only true in inertial coordinates?
 
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Are you familiar with the multivariable chain rule
\frac{d f (x,y)}{dt} = \frac{\partial f}{\partial x}\frac{dx}{dt} + \frac{\partial f}{\partial y}\frac{dy}{dt}?
The 'cancellation' you performed there is simply a simplification using the chain rule (remember that you are using the Einstein summation convention).
 
Fightfish said:
Are you familiar with the multivariable chain rule
\frac{d f (x,y)}{dt} = \frac{\partial f}{\partial x}\frac{dx}{dt} + \frac{\partial f}{\partial y}\frac{dy}{dt}?
The 'cancellation' you performed there is simply a simplification using the chain rule (remember that you are using the Einstein summation convention).

Thanks, i did notice that of course after posting o:)
 
And, while it may be a useful "mnemonic", the derivative, ordinary or partial, is NOT a fraction and the "chain rule" does NOT involve "cancelling".
 
In an inertial frame of reference (IFR), there are two fixed points, A and B, which share an entangled state $$ \frac{1}{\sqrt{2}}(|0>_A|1>_B+|1>_A|0>_B) $$ At point A, a measurement is made. The state then collapses to $$ |a>_A|b>_B, \{a,b\}=\{0,1\} $$ We assume that A has the state ##|a>_A## and B has ##|b>_B## simultaneously, i.e., when their synchronized clocks both read time T However, in other inertial frames, due to the relativity of simultaneity, the moment when B has ##|b>_B##...

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