Total Differentials: Taking the Total Differential of Reduced Mass

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The discussion focuses on understanding the total differential in the context of the reduced mass equation, specifically μ⁻¹ = m₁⁻¹ + m₂⁻². The user is confused about taking the total differential of μ⁻¹ and how it relates to maintaining a constant reduced mass, leading to the condition ∂μ = 0. They express familiarity with total differentials in the context of defined functions but seek clarity on applying this to the reduced mass equation. The user also correctly identifies that the exponent indicates the reciprocal relationship, which is relevant for differentiating. Overall, the conversation centers on applying mathematical principles to a specific physical context.
eprparadox
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Hello!

I'm reading Mary Boa's "mathematical methods in the physical sciences" and I'm on a section about total differentials.

So a total differential is for f(x, y) we know to be:

df = \frac{\partial f}{\partial x}{dx} + \frac{\partial f}{\partial y}{dy}


Now, I've attached a problem I'm confused about. It involves taking the total differential of the reduced mass equation:

\mu^{-1} = m_1^{-1} + m_2^{-2}

In her example, she says to take the total differential of the equation and sets the left side equal to zero. I understand why it's zero (because we want the reduced mass to be unchanged so we want \partial \mu = 0).

But essentially, I don't know what it means to just take the differential of \mu^{-1} because I'm accustomed to having some defined function f(x, y) or something and if I take it's differential, I just get df.

Thanks!
 

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I assume the exponent means a^{-1}=1/a. Then d(1/a)=d(a^{-1})=-a^{-1-1}da. This is just d(a^n)=na^{n-1}da.
 

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