Exercise 4.   Let the rays  [Graphics:Images/SourceSinkModHome_gr_203.gif]  and  [Graphics:Images/SourceSinkModHome_gr_204.gif] and the segment  [Graphics:Images/SourceSinkModHome_gr_205.gif]  

form the walls of a containing vessel for a fluid flow in the semi-infinite strip  [Graphics:Images/SourceSinkModHome_gr_206.gif]  that is produced by

two sources of equal strength located at the points  [Graphics:Images/SourceSinkModHome_gr_207.gif]  and  [Graphics:Images/SourceSinkModHome_gr_208.gif].  

Find the complex potential for the flow shown in Figure 11.102.           Figure 11.102.

Hint.  Use the fact that   [Graphics:Images/SourceSinkModHome_gr_209.gif].

Solution 4.

See text and/or instructor's solution manual.

Answer.   Look carefully at the result in Example 11.32.  Recall that the mapping   [Graphics:../Images/SourceSinkModHome_gr_210.gif]   is periodic with period  [Graphics:../Images/SourceSinkModHome_gr_211.gif]  and that   [Graphics:../Images/SourceSinkModHome_gr_212.gif].   

Furthermore,  [Graphics:../Images/SourceSinkModHome_gr_213.gif].    Hence  [Graphics:../Images/SourceSinkModHome_gr_214.gif]  

will produce streamlines where there are an infinite number of unit sources located at the points  [Graphics:../Images/SourceSinkModHome_gr_215.gif].   Here you need to visualize that

the graph in Figure 11.96 is translated infinitely many times by  [Graphics:../Images/SourceSinkModHome_gr_216.gif].  

 

                    [Graphics:../Images/SourceSinkModHome_gr_217.gif]

  

                    [Graphics:../Images/SourceSinkModHome_gr_218.gif]

        The rays  [Graphics:../Images/SourceSinkModHome_gr_219.gif]  and  [Graphics:../Images/SourceSinkModHome_gr_220.gif] and the segment  [Graphics:../Images/SourceSinkModHome_gr_221.gif]  are all portions of streamlines of   

                    [Graphics:../Images/SourceSinkModHome_gr_222.gif]  

and form the walls of a containing vessel for a fluid flow in the semi-infinite strip  [Graphics:../Images/SourceSinkModHome_gr_223.gif].

Therefore, the desired complex potential is   

                    [Graphics:../Images/SourceSinkModHome_gr_224.gif].

Solution.   In Exercise 3 we saw that  [Graphics:../Images/SourceSinkModHome_gr_225.gif]  is the complex potential for a source at  [Graphics:../Images/SourceSinkModHome_gr_226.gif].  

The function  [Graphics:../Images/SourceSinkModHome_gr_227.gif]  maps  [Graphics:../Images/SourceSinkModHome_gr_228.gif]  onto  [Graphics:../Images/SourceSinkModHome_gr_229.gif].  The composition  [Graphics:../Images/SourceSinkModHome_gr_230.gif]  is a complex potential in the

infinite strip   [Graphics:../Images/SourceSinkModHome_gr_231.gif],  where a single source located at the point  [Graphics:../Images/SourceSinkModHome_gr_232.gif] and the lines  [Graphics:../Images/SourceSinkModHome_gr_233.gif]  and  [Graphics:../Images/SourceSinkModHome_gr_234.gif]  form the walls of the containing vessel.  

The trigonometric identity  [Graphics:../Images/SourceSinkModHome_gr_235.gif]  can be used to see that a symmetric flow is produced in the infinite strip   [Graphics:../Images/SourceSinkModHome_gr_236.gif].  

        Also, the rays  [Graphics:../Images/SourceSinkModHome_gr_237.gif]  and  [Graphics:../Images/SourceSinkModHome_gr_238.gif] and the segment  [Graphics:../Images/SourceSinkModHome_gr_239.gif]  

are all portions of streamlines of   

                    [Graphics:../Images/SourceSinkModHome_gr_240.gif]  

and form the walls of a containing vessel for a fluid flow in the semi-infinite strip  [Graphics:../Images/SourceSinkModHome_gr_241.gif].

        Therefore  the desired complex potential is

                    [Graphics:../Images/SourceSinkModHome_gr_242.gif].  

 

We are done.   

 

Aside.  We can let Mathematica double check our work.

 

The velocity potential  [Graphics:../Images/SourceSinkModHome_gr_243.gif]  is   

[Graphics:../Images/SourceSinkModHome_gr_245.gif]

[Graphics:../Images/SourceSinkModHome_gr_246.gif]

The stream function   [Graphics:../Images/SourceSinkModHome_gr_247.gif]  is   

[Graphics:../Images/SourceSinkModHome_gr_249.gif]

[Graphics:../Images/SourceSinkModHome_gr_250.gif]

[Graphics:../Images/SourceSinkModHome_gr_251.gif]

[Graphics:../Images/SourceSinkModHome_gr_252.gif]


We are really done.   

 

        We can let Mathematica graph some of the streamlines and velocity potentials.

 

                    [Graphics:../Images/SourceSinkModHome_gr_253.gif]

                    Some streamlines   [Graphics:../Images/SourceSinkModHome_gr_254.gif]  for a fluid flow in the semi-infinite strip  [Graphics:../Images/SourceSinkModHome_gr_255.gif]  

                    that is produced by two sources of equal strength located at the points  [Graphics:../Images/SourceSinkModHome_gr_256.gif]  and  [Graphics:../Images/SourceSinkModHome_gr_257.gif].  



                    [Graphics:../Images/SourceSinkModHome_gr_259.gif]

                    Some velocity potentials   [Graphics:../Images/SourceSinkModHome_gr_260.gif]  for a fluid flow in the semi-infinite strip  [Graphics:../Images/SourceSinkModHome_gr_261.gif]  

                    that is produced by two sources of equal strength located at the points  [Graphics:../Images/SourceSinkModHome_gr_262.gif]  and  [Graphics:../Images/SourceSinkModHome_gr_263.gif].  

 

                    [Graphics:../Images/SourceSinkModHome_gr_264.gif]

                    Streamlines and velocity potentials for a fluid flow in the semi-infinite strip  [Graphics:../Images/SourceSinkModHome_gr_265.gif]  

                    that is produced by two sources of equal strength located at the points  [Graphics:../Images/SourceSinkModHome_gr_266.gif]  and  [Graphics:../Images/SourceSinkModHome_gr_267.gif].  

 

We are really really done.   

 

        Solving for the inverse of    [Graphics:../Images/SourceSinkModHome_gr_268.gif]    we get  

                    [Graphics:../Images/SourceSinkModHome_gr_269.gif].

We can use Mathematica to check our work and graph the conformal mapping   [Graphics:../Images/SourceSinkModHome_gr_270.gif].

 

[Graphics:../Images/SourceSinkModHome_gr_271.gif]

[Graphics:../Images/SourceSinkModHome_gr_272.gif]

[Graphics:../Images/SourceSinkModHome_gr_273.gif]

          [Graphics:../Images/SourceSinkModHome_gr_274.gif]          [Graphics:../Images/SourceSinkModHome_gr_275.gif]

                      The conformal mapping   [Graphics:../Images/SourceSinkModHome_gr_276.gif].  

 

We are really really done.   

 

        We can let Mathematica draw some other graphs of the streamlines and velocity potentials.

 

                    [Graphics:../Images/SourceSinkModHome_gr_277.gif]

         A density plot of some velocity potentials  [Graphics:../Images/SourceSinkModHome_gr_278.gif] for a fluid flow in the semi-infinite strip [Graphics:../Images/SourceSinkModHome_gr_279.gif]  

         that is produced by two sources of equal strength located at the points  [Graphics:../Images/SourceSinkModHome_gr_280.gif]  and  [Graphics:../Images/SourceSinkModHome_gr_281.gif].  

 

                    [Graphics:../Images/SourceSinkModHome_gr_282.gif]

          Some streamlines   [Graphics:../Images/SourceSinkModHome_gr_283.gif]  for a fluid flow in the semi-infinite strip  [Graphics:../Images/SourceSinkModHome_gr_284.gif]  

          that is produced by two sources of equal strength located at the points  [Graphics:../Images/SourceSinkModHome_gr_285.gif]  and  [Graphics:../Images/SourceSinkModHome_gr_286.gif].  

 

                    [Graphics:../Images/SourceSinkModHome_gr_287.gif]

          Some velocity potentials  [Graphics:../Images/SourceSinkModHome_gr_288.gif]  for a fluid flow in the semi-infinite strip [Graphics:../Images/SourceSinkModHome_gr_289.gif]  

         that is produced by two sources of equal strength located at the points  [Graphics:../Images/SourceSinkModHome_gr_290.gif]  and  [Graphics:../Images/SourceSinkModHome_gr_291.gif].  

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

This solution is complements of the authors.

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

(c) 2008 John H. Mathews, Russell W. Howell