Question about the Derivation of the Stream-function for a Doublet

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Master1022
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This is a question about the derivation of the stream-function of a doublet using potential flow theory
Hi,

I just wanted to ask a question about the derivation of the stream function [itex]\psi[/itex] for a doublet. In the pictures below is a derivation (in this one the source is on the left and the sink is on the right). I understand everything in the left photo, however my questions are:

1) Why do we divide by the distance between two sources [itex]s[/itex] before taking the limit? I cannot really understand the reason provided. I understand that the sources will cancel out, but am unclear as to why that means that we need to counter that by including a [itex]\frac{1}{s}[/itex] term.

2) Why does the derivation come out differently if we swap the placements of the source and sink? Intuitively, I feel that I have made an algebraic error, but I fail to see it. If we place the source on the right and the sink on the left, then we will get:
[tex]\psi = \frac{m}{2 \pi} \theta_{source} - \frac{m}{2 \pi} \theta_{sink} = \frac{m}{2 \pi} \left( atan(\frac{y}{x-s}) - atan(\frac{y}{x+s}) \right)[/tex]. Now we will get the same expression as before (except we have +m instead of -m), except we will end up with a different sign at the end. Surely, the end result should be the same irrespective of the original geometry.

I would appreciate any help. Thanks in advance.

Screen Shot 2020-01-12 at 12.03.18 PM.png
Screen Shot 2020-01-12 at 12.03.24 PM.png
 
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Chestermiller said:
If you swap the locations, the fluid velocities (calculated from the derivatives of the stream function) are, as expected physically, in the opposite direction. So what's the problem?
Ah yes, that is true. Thank you.

Do you know the reason behind the division by [itex]\frac{1}{s}[/itex]?
 
Chestermiller said:
You are determining the limit as the two charges are very close together.
I understand the intuition, but why does that mean that we need a [itex]\frac{1}{s}[/itex] term