Calculating Line Elements in Cylindrical and Spherical Coordinates ...

Calculating Line Elements in Cylindrical and Spherical Coordinates ... Calculating Line Elements in Cylindrical and Spherical Coordinates ...

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Calculating Line Elements inCylindrical and Spherical Coordinatesby Corinne Manogue and Katherine Meyerc○1997 Corinne A. ManogueRectangular Coordinates:The arbitrary infinitesimal displacement vector in Cartesian coordinates is:d⃗r = dx î + dy ĵ + dz ˆkGiven the cube shown below, find d⃗r on each of the three paths, leading froma to b.zPath 1: d⃗r =Path 2: d⃗r =Path 3: d⃗r =path 1abpath 3yxpath 2The expression above for d⃗r is valid for any path in rectangular coordinates.Find the appropriate expression for d⃗r for the path which goes directly froma to c as drawn below.Path 4: d⃗r =zapath 4cyxHowever, Cartesian coordinates would be a poor choice to describe a path ona cylindrically or spherically shaped surface. Next we will find an appropriateexpression in these cases.

<strong>Calculat<strong>in</strong>g</strong> <strong>L<strong>in</strong>e</strong> <strong>Elements</strong> <strong>in</strong>Cyl<strong>in</strong>drical <strong>and</strong> <strong>Spherical</strong> Coord<strong>in</strong>atesby Cor<strong>in</strong>ne Manogue <strong>and</strong> Kather<strong>in</strong>e Meyerc○1997 Cor<strong>in</strong>ne A. ManogueRectangular Coord<strong>in</strong>ates:The arbitrary <strong>in</strong>f<strong>in</strong>itesimal displacement vector <strong>in</strong> Cartesian coord<strong>in</strong>ates is:d⃗r = dx î + dy ĵ + dz ˆkGiven the cube shown below, f<strong>in</strong>d d⃗r on each of the three paths, lead<strong>in</strong>g froma to b.zPath 1: d⃗r =Path 2: d⃗r =Path 3: d⃗r =path 1abpath 3yxpath 2The expression above for d⃗r is valid for any path <strong>in</strong> rectangular coord<strong>in</strong>ates.F<strong>in</strong>d the appropriate expression for d⃗r for the path which goes directly froma to c as drawn below.Path 4: d⃗r =zapath 4cyxHowever, Cartesian coord<strong>in</strong>ates would be a poor choice to describe a path ona cyl<strong>in</strong>drically or spherically shaped surface. Next we will f<strong>in</strong>d an appropriateexpression <strong>in</strong> these cases.


Cyl<strong>in</strong>drical Coord<strong>in</strong>ates:SEE DIAGRAM ON NEXT PAGEYou will now derive the general form for d⃗r <strong>in</strong> cyl<strong>in</strong>drical coord<strong>in</strong>ates bydeterm<strong>in</strong><strong>in</strong>g d⃗r along the specific paths below.Note that an <strong>in</strong>f<strong>in</strong>itesmial element of length <strong>in</strong> the ˆr direction is simply dr,just as an <strong>in</strong>f<strong>in</strong>itesimal element of length <strong>in</strong> the î direction is dx. But, an<strong>in</strong>f<strong>in</strong>itesimal element of length <strong>in</strong> the ˆφ direction is not just dφ, s<strong>in</strong>ce thiswould be an angle <strong>and</strong> does not even have the units of length.Geometrically determ<strong>in</strong>e the length of the three paths lead<strong>in</strong>g from a to b<strong>and</strong> write these lengths <strong>in</strong> the correspond<strong>in</strong>g boxes on the diagram.Now, remember<strong>in</strong>g that d⃗r has both magnitude <strong>and</strong> direction, write downbelow the <strong>in</strong>f<strong>in</strong>tesimal displacement vector d⃗r along the three paths from ato b. Notice that, along any of these three paths, only one coord<strong>in</strong>ate r, φ, orz is chang<strong>in</strong>g at a time. (i.e. along path 1, dr ≠ 0, but dφ = 0 <strong>and</strong> dz = 0).Path 1: d⃗r =Path 2: d⃗r =Path 3: d⃗r =If all three coord<strong>in</strong>ates are allowed to change simultaneously, by an <strong>in</strong>f<strong>in</strong>itesimalamount, we could write this d⃗r for any path as:d⃗r=This is the general l<strong>in</strong>e element <strong>in</strong> cyl<strong>in</strong>drical coord<strong>in</strong>ates.


zpath 3length=(r+dr, φ+ d φ,z+dz)=ba= (r, φ,z)path 1length=path 2length=yxφdφ<strong>L<strong>in</strong>e</strong> <strong>Elements</strong> <strong>in</strong> Cyl<strong>in</strong>drical Coord<strong>in</strong>ates


zθlength=path 1(r, θ, φ)=apath 2path 3length=dθlength=b=(r+dr, θ+d θ, φ +d φ)xφdφ<strong>L<strong>in</strong>e</strong> <strong>Elements</strong> <strong>in</strong> <strong>Spherical</strong> Coord<strong>in</strong>ates<strong>Spherical</strong> Coord<strong>in</strong>ates:You will now derive the general form for d⃗r <strong>in</strong> spherical coord<strong>in</strong>ates by determ<strong>in</strong><strong>in</strong>gd⃗r along the specific paths below. As <strong>in</strong> the cyl<strong>in</strong>drical case, notethat an <strong>in</strong>f<strong>in</strong>itesmial element of length <strong>in</strong> the ˆθ or ˆφ direction is not justdθ or dφ. You will need to be more careful. Geometrically determ<strong>in</strong>e thelength of the three paths lead<strong>in</strong>g from a to b <strong>and</strong> write these lengths <strong>in</strong> thecorrespond<strong>in</strong>g boxes on the diagram. Now, remember<strong>in</strong>g that d⃗r has bothmagnitude <strong>and</strong> direction, write down below the <strong>in</strong>f<strong>in</strong>tesimal displacementvector d⃗r along the three paths from a to b. Notice that, along any of thesethree paths, only one coord<strong>in</strong>ate r, θ, or φ is chang<strong>in</strong>g at a time. (i.e. alongpath 1, dr ≠ 0, but dθ = 0 <strong>and</strong> dφ = 0).Path 1: d⃗r =Path 2: d⃗r =Path 3: d⃗r =y(Be careful, this is the tricky one.)If all 3 coord<strong>in</strong>ates are allowed to change simultaneously, by an <strong>in</strong>f<strong>in</strong>itesimalamount, we could write this d⃗r for any path as:d⃗r=This is the general l<strong>in</strong>e element <strong>in</strong> spherical coord<strong>in</strong>ates.

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