Is it valid to split the derivative in deriving the equation for e_s(T)?

KingBigness
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Homework Statement



From
\frac{de_{s}}{dT} = \frac{L_{v}e_{s}}{R_{v}T^{2}}

derive

e_{s}(T) = 6.11 e^{\frac{L}{RV}(\frac{1}{T}-\frac{1}{273})}

Homework Equations


The Attempt at a Solution



The way my lecturer derived it was he 'split' the derivative and took them to their respective sides and integrated.

So he got

\frac{de_{s}}{e_{s}} = \frac{LdT}{R_{v}T^{2}}

However I was under the impression that you can't 'split' a derivative like that. Is this just a shortcut some physicists take to make the maths more simple? If it is what is the correct way of deriving this?
 
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Curious3141 said:
http://en.wikipedia.org/wiki/Separation_of_variables

It's not just "physicist's shorthand", it's a well-worn technique called Separation of Variables. Some might balk at the notation, but it's generally accepted and makes life easier.

How accepted is it? I am doing a double degree in pure mathematics and physics. If I was to do this in my pure maths classes would I be stoned?
 
KingBigness said:
How accepted is it? I am doing a double degree in pure mathematics and physics. If I was to do this in my pure maths classes would I be stoned?

I've taken calculus 1 and I've seen it before? :s
 
iRaid said:
I've taken calculus 1 and I've seen it before? :s

Sorry I wasn't very clear. I have seen it before and done it countless times I just always have a memory of a teacher saying don't tell a pure mathematician about it.
 
KingBigness said:

Homework Statement



From
\displaystyle \frac{de_{s}}{dT} = \frac{L_{v}e_{s}}{R_{v}T^{2}}

derive

\displaystyle e_{s}(T) = 6.11 e^{\frac{L}{RV}(\frac{1}{T}-\frac{1}{273})}

Homework Equations



The Attempt at a Solution



The way my lecturer derived it was he 'split' the derivative and took them to their respective sides and integrated.

So he got

\displaystyle \frac{de_{s}}{e_{s}} = \frac{LdT}{R_{v}T^{2}}

However, I was under the impression that you can't 'split' a derivative like that. Is this just a shortcut some physicists take to make the maths more simple? If it is what is the correct way of deriving this?
In my experience, physicists & engineers are notorious for treating Leibniz's notation for the derivative as if it were a fraction.

A more rigorous handling of this derivative equation might be as follows:
Treating es as a function of T we have

\displaystyle \frac{d}{dT}(e_{s}) = \frac{L_{v}e_{s}}{R_{v}T^{2}}

Rewriting this equation gives us

\displaystyle \frac{1}{e_{s}}\frac{d}{dT}(e_{s}) = \frac{L}{R_{v}T^{2}}

Integrating w.r.t. T gives

\displaystyle \int {\frac{1}{e_{s}}\frac{d}{dT}(e_{s})}dT = \int{\frac{L}{R_{v}T^{2}}}dT

We can rewrite the integral on the left hand side.

\displaystyle \int {\frac{1}{e_{s}}\frac{d}{dT}(e_{s})}dT = \int {\frac{1}{e_{s}}}\,de_{s}​

Alternatively, if \displaystyle \frac{d}{dT}(e_{s}) = \frac{L_{v}e_{s}}{R_{v}T^{2}}\,,
then the differential of es is given by \displaystyle d\,e_{s} = \frac{L_{v}e_{s}}{R_{v}T^{2}}\,dT
 
SammyS said:
In my experience, physicists & engineers are notorious for treating Leibniz's notation for the derivative as if it were a fraction.

A more rigorous handling of this derivative equation might be as follows:
Treating es as a function of T we have

\displaystyle \frac{d}{dT}(e_{s}) = \frac{L_{v}e_{s}}{R_{v}T^{2}}

Rewriting this equation gives us

\displaystyle \frac{1}{e_{s}}\frac{d}{dT}(e_{s}) = \frac{L}{R_{v}T^{2}}

Integrating w.r.t. T gives

\displaystyle \int {\frac{1}{e_{s}}\frac{d}{dT}(e_{s})}dT = \int{\frac{L}{R_{v}T^{2}}}dT

We can rewrite the integral on the left hand side.

\displaystyle \int {\frac{1}{e_{s}}\frac{d}{dT}(e_{s})}dT = \int {\frac{1}{e_{s}}}\,de_{s}​

Alternatively, if \displaystyle \frac{d}{dT}(e_{s}) = \frac{L_{v}e_{s}}{R_{v}T^{2}}\,,
then the differential of es is given by \displaystyle d\,e_{s} = \frac{L_{v}e_{s}}{R_{v}T^{2}}\,dT

exactly what I wanted. thank you
 
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