[PDF] 4. Calculating ds in a different coordinate system Cylindrical polar





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Polar Coordinates

Polar Coordinates. In a rectangular coordinate system we were plotting points based on an ordered pair of (x



4. Calculating ds in a different coordinate system Cylindrical polar

(c) Starting from ds2 = dx2 + dy2 + dz2 show that ds2 = d?2 + ?2d?2 + dz2. (d) Having warmed up with that calculation repeat with spherical polar coordinates 



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Feb 4 2018 Stresses and Strains in Cylindrical Coordinates ... A similar calculation can be carried out for forces in the tangential direction {? ...





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Integrals in cylindrical spherical coordinates (Sect. 15.7) Cylindrical

Remark: Cylindrical coordinates are just polar coordinates on the The calculation is simple the region is a simple section of a sphere.

4.Calculatingdsinadi↵erentcoordinates ystem

Cylindricalpolarcoordinatesaredefine dby

x=⇢cos y=⇢sin z=z (a)Confirmthatdx=d⇢cos⇢sind. (b)Calculateasimilarexpress ion fordy. (c)Startingfromds 2 =dx 2 +dy 2 +dz 2 showthatds 2 =d⇢ 2 2 d 2 +dz 2 (d)Havingwarmedupwit hthatcalculation,r epeatwi thsphericalp olarcoordinat eswhichare definedby x=rsin✓cos y=rsin✓sin z=rcos✓ andshow thatds 2 =dr 2 +r 2 d 2 +r 2 sin 2 d 2 Hint:Thespheric alresultis easiertogetstartingfromthe cylindricalresul tandus ing ⇢=rsin✓.

4.Solution:Calculatingdsinadi↵erentcoordinatesy stem

(a)Thisisasimpl eapplic ati onoftheproductruledx=d⇢cos⇢sind. (b)dy=d⇢sin+⇢cosd. (c)Now dx 2 +dy 2 =(d⇢cos⇢sind) 2 +(d⇢sin+⇢cosd) 2

Thecrosst ermscancelso

dx 2 +dy 2 =d⇢ 2 (cos 2 +sin 2 2 d 2 (sin 2 +cos 2 )=d⇢ 2 2 d 2

Addingdz

2 givesthedesi redresult . (d)Startwithds 2 =d⇢ 2 2 d 2 +dz 2 .Now ⇢ 2 =r 2 sin 2 ✓andthe productru leappliedtod⇢ gives d ⇢=drsin✓+rcos✓d✓ andalso dz=drcos✓rsin✓d✓

Thussubstit utingintods

2 fromabovegi ves ds 2 =(drsin✓+rcos✓d✓) 2 +r 2 sin 2 d 2 +(drcos✓rsin✓d✓) 2

Onceagainthecr oss-ter mscancelle aving

ds 2 =dr 2 (sin 2 ✓+cos 2 ✓)+r 2 (cos 2 ✓+sin 2 ✓)d✓ 2 +r 2 sin 2 d 2 whichsimplifiesto thedesiredresultds 2 =dr 2 +r 2 d 2 +r 2 sin 2 d 2 4

5.GeodesicsontheSphere

Theequati onofasphereinspheri calp olarc oordinatesisparticul arlysim ple:itisr=a,where aisacons tant . (a)Startingwithdsinsphe ricalpolarcoordinates,writed ownthesim plifiedformofdswhen r=aisacons tant . (b)Usethis expressionfordstowri tedownanintegralth atrepresents the distancebetween twopoints connectedbyapatht hatliesonthesurfaceofaspher e.Wri tet heintegrali n theformwhe reisafun cti onof✓. (c)Writedownafirst integralforthi sin tegrand. (d)Showthat 0 =sin 1 [↵cot✓] satisfiesthefirstintegral ,where 0 and↵aretwo independe ntconstants. (e)Theequati onofaplanethroughtheorigi ni sAx+By+Cz=0.R ewr itethisequationin sphericalpolarcoordinates.Re arrangetheeq uationtomakeitlooklikethesolutionabo ve andfind ↵and 0 interm sofA,BandC. (f)Thusgiveasim plegeometri cde scriptionandmethodof findinggeodesicsonasphe re.

5.Solution:GeodesicsontheS phere

(a)Ifr=aisacons tant then ds 2 =a 2 d 2 +a 2 sin 2 d 2 (b)Theintegr alis I= Z ds=a Z B A q 1+sin 2 0 2 d

ThusF(✓,,

0 p 1+sin 2 0 2 (c)Since@F/@=0 afir sti ntegralis sinquotesdbs_dbs12.pdfusesText_18
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