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activities:guides:vfvring 2011/12/05 16:43 | activities:guides:vfvring 2019/06/03 13:18 current | ||
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* Power series expansion | * Power series expansion | ||

* Symmetry | * Symmetry | ||

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//Estimated Time: 40 min; Wrap-up: 10 min// | //Estimated Time: 40 min; Wrap-up: 10 min// | ||

- | - Students should be assigned to work in groups of three and given the following instructions using the visual of a hula hoop or other large ring: "This is a ring with total charge $Q$ and radius $R$. Find the electrical potential due to this ring in all space." Students do their work collectively with markers on a poster-sized sheet of whiteboard at their tables. \texttt{Link to worked solution resulting in an elliptic integral}. | + | - Students should be assigned to work in groups of three and given the following instructions using the visual of a hula hoop or other large ring: "This is a ring with total charge $Q$ and radius $R$. Find the electrical potential due to this ring in all space." Students do their work collectively with markers on a poster-sized sheet of whiteboard at their tables. |

- | - Students determine the power series expansion to represent the electrostatic potential due to the charged ring along a particular axis. Link to worked solutions for power series expansions. | + | - Students determine the power series expansion to represent the electrostatic potential due to the charged ring along a particular axis. |

*Note: students should not be told about part II until they have completed part I. | *Note: students should not be told about part II until they have completed part I. | ||

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==== Prerequisite Knowledge ==== | ==== Prerequisite Knowledge ==== | ||

- | This activity is may be used as the second in a sequence, following the electrostatic potential - discrete charges activity, or may be used on its own. Students will need understanding of: | + | This activity is may be used as the second in the [[whitepapers:sequences:emsequence:start|Ring Sequence]], following the <html><a href="http://www.physics.oregonstate.edu/portfolioswiki/doku.php?id=activities:main&file=vfvpoints">Electrostatic potential due to two points</a></html> activity, or may be used on its own. Students will need understanding of: |

- | * Spherical and cylindrical coordinates. You may want to consider using the activity, <html> <a href= "http://www.physics.oregonstate.edu/portfolioswiki/doku.php?id=activities:main&file=drvector">dr in curvilinear coordinates</a> </html>, in which students use geometric arguments to derive the form of $d\Vec r$ in these curvilinear coordinate systems. | + | * Spherical and cylindrical coordinates. You may want to consider using the <html> <a href= "http://www.physics.oregonstate.edu/portfolioswiki/doku.php?id=activities:main&file=vfdrvectorcurvi">Vector Differential</a> </html> activity, in which students use geometric arguments to derive the form of $d\Vec r$ in these curvilinear coordinate systems. |

- | * Integration as chopping and adding. | + | * Integration as chopping and adding |

- | * Linear charge density | + | * Linear charge density (see <html> <a href= "http://www.physics.oregonstate.edu/portfolioswiki/doku.php?id=activities:main&file=vfchargedensity">Acting Out Charge Densities</a> </html> activity) |

==== Props/Equipment ==== | ==== Props/Equipment ==== | ||

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* [[:Props:start#Voltmeter|Voltmeter]] | * [[:Props:start#Voltmeter|Voltmeter]] | ||

* [[:Props:start#Coordinate Axes|Coordinate Axes]] | * [[:Props:start#Coordinate Axes|Coordinate Axes]] | ||

- | * A handout for each student | + | |

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==== Activity: Introduction ==== | ==== Activity: Introduction ==== | ||

Students should be assigned to work in groups of three and given the following instructions using the visual of a hula hoop or other large ring: ``This is a ring with total charge Q and radius R. Find the electrical potential due to this ring in all space.'' | Students should be assigned to work in groups of three and given the following instructions using the visual of a hula hoop or other large ring: ``This is a ring with total charge Q and radius R. Find the electrical potential due to this ring in all space.'' | ||

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- | Students do their work collectively with markers on a poster-sized sheet of whiteboard at their tables. | ||

==== Activity: Student Conversations ==== | ==== Activity: Student Conversations ==== | ||

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* Putting the whole thing together requires three dimensional geometric understanding. One of the big advantages to doing this problem in class as opposed to homework is that the instructor can interact with student making 3-dimesional arguments. Either a hoop or a ring drawn on the table can be used to ask students about the potential at points in space that are outside the plane of the ring. | * Putting the whole thing together requires three dimensional geometric understanding. One of the big advantages to doing this problem in class as opposed to homework is that the instructor can interact with student making 3-dimesional arguments. Either a hoop or a ring drawn on the table can be used to ask students about the potential at points in space that are outside the plane of the ring. | ||

- | * This activity also gives students the opportunity to use curvilinear coordinates and then realize that they cannot successfully integrate without transforming them using rectangular basis vectors. Understanding that $|\Vec{r} - \Vec r'|$ cannot be integrated by simply using $r'$ in curvilinear coordinates is an important realization. Unlike linear coordinates where $x - x'$ always refers to components of vectors that point in the same direction, this is not the case for curvilinear coordinates where $\Vec r$ and $\Vec r'$ can be oriented in different directions at any angle. Solving this problem entirely in rectangular coordinates from the beginning is overly cumbersome, but the curvilinear coordinates that successfully simplify the problem can lead one to incorrectly think that using $|\Vec{r} - \Vec r'|$ in curvilinear coordinates can be successfully integrated. To see how this fits into the whole process, see the \texttt{link to worked solution resulting in an elliptic integral}. | + | * This activity also gives students the opportunity to use curvilinear coordinates and then realize that they cannot successfully integrate without transforming them using rectangular basis vectors. Understanding that $|\Vec{r} - \Vec r'|$ cannot be integrated by simply using $r'$ in curvilinear coordinates is an important realization. Unlike linear coordinates where $x - x'$ always refers to components of vectors that point in the same direction, this is not the case for curvilinear coordinates where $\Vec r$ and $\Vec r'$ can be oriented in different directions at any angle. Solving this problem entirely in rectangular coordinates from the beginning is overly cumbersome, but the curvilinear coordinates that successfully simplify the problem can lead one to incorrectly think that using $|\Vec{r} - \Vec r'|$ in curvilinear coordinates can be successfully integrated. |

* The final component is that students need to recognize an elliptic integral and what to do when they run into one. Most commonly students have never seen such `unsolvable' integrals in their calculus classes. In our case we had students do the power series expansion before the integral (see below). | * The final component is that students need to recognize an elliptic integral and what to do when they run into one. Most commonly students have never seen such `unsolvable' integrals in their calculus classes. In our case we had students do the power series expansion before the integral (see below). | ||

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- | * With the charged ring in the $x,y-$plane, students will make the power series expansion for either near or far from the plane on the $z$ axis or near or far from the $z$ axis in the $x,y-$plane. Once all students have made significant progress toward finding the integral from part I, and some students have successfully determined it, then the instructor can quickly have a whole class discussion emphasizing some of the points above, followed by telling students to now create a power series expansion. The instructor may choose to have the whole class do one particular case or have different groups do different cases. {{activities:content:solutions:vfvringsol.pdf|Link to worked solutions for power series expansions}}. | + | * With the charged ring in the $x,y-$plane, students will make the power series expansion for either near or far from the plane on the $z$ axis or near or far from the $z$ axis in the $x,y-$plane. Once all students have made significant progress toward finding the integral from part I, and some students have successfully determined it, then the instructor can quickly have a whole class discussion emphasizing some of the points above, followed by telling students to now create a power series expansion. The instructor may choose to have the whole class do one particular case or have different groups do different cases. |

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+ | * If you are doing this activity without having had students first create power series expansions for the electrostatic potential due to two charges, students will probably find this portion of the activity very challenging. If they have already done the <html><a href="http://www.physics.oregonstate.edu/portfolioswiki/doku.php?id=activities:main&file=vfvpoints">Electrostatic potential due to two points</a></html> activity, or similar activity, students will probably be successful with the $z$ axis case without a lot of assistance because it is very similar to the $y$ axis case for the two $+Q$ point charges. However, the $y$ axis presents a new challenges because the ``something small'' is two terms. It will probably not be obvious for students to let $\epsilon = {2R\over r}\cos\phi' + {R^2 \over r^2}$ (see Eq. 17 in the solutions) and suggestions should be given to avoid having them stuck for a long period of time. Once this has been done, students may also have trouble combining terms of the same order. For example the $\epsilon^2$ term results in a third and forth order term in the expansion and students may not realize that to get a valid third order expansion they need to calculate the $\epsilon^3$ term. | ||

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- | * If you are doing this activity without having had students first create power series expansions for the electrostatic potential due to two charges, students will probably find this portion of the activity very challenging. If they have already done the \texttt{Electrostatic Potential - Discrete Charges} activity, or similar activity, students will probably be successful with the $y$ axis case without a lot of assistance because it is very similar to the $y$ axis case for the two $+Q$ point charges. However, the $y$ axis presents a new challenges because the ``something small'' is two terms. It will probably not be obvious for students to let $\epsilon = {2R\over r}\cos\phi' + {R^2 \over r^2}$ (see Eq. 17 in the solutions) and suggestions should be given to avoid having them stuck for a long period of time. Once this has been done, students may also have trouble combining terms of the same order. For example the $\epsilon^2$ term results in a third and forth order term in the expansion and students may not realize that to get a valid third order expansion they need to calculate the $\epsilon^3$ term. | ||

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==== Activity: Wrap-up ==== | ==== Activity: Wrap-up ==== | ||

- | * Discuss which variables are variable and which variables are held constant - Students frequently think of anything represented by a letter as a `variable' and do not realize that for each particular situation certain variables remain constant during integration. For example students frequently do not see that the $R$ representing the radius of the ring is held constant during the integration over all space while the r representing the distance to the origin is varying. Understanding this is something trained physicists do naturally while students frequently don't even consider it. This is an important discussion that helps students understand this particular ring problem and also lays the groundwork for better understanding of integration in a variety of contexts. [[whitepapers:variables:start|Link to helping students understand what is variable are what is held constant]]. | + | * Discuss which quantities are variable and which variables are held constant - Students frequently think of anything represented by a letter as a `variable' and do not realize that for each particular situation certain quantities remain constant during integration. For example students frequently do not see that the $R$ representing the radius of the ring is held constant during the integration over all space while the r representing the distance to the origin is varying. Understanding this is something trained physicists do naturally while students frequently don't even consider it. This is an important discussion that helps students understand this particular ring problem and also lays the groundwork for better understanding of integration in a variety of contexts. For more information on this topic, see [[whitepapers:variables:start|Students understanding of variables and constants]]. |

- | * Maple representation of elliptic integral - After finding the elliptic integral and doing the power series expansion, students can see what electric potential `looks like' over all space by using {{activities:guides:vfringcontinuous.mws|this Maple worksheet}}. | + | |

+ | * Emphasize that while one may not be able to perform a particular integral, the power series expansion of that integrand can be integrated **term by term**. | ||

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==== Extensions ==== | ==== Extensions ==== | ||

It is very helpful to end this activity with a way to visualize the value of the potential everywhere in space. | It is very helpful to end this activity with a way to visualize the value of the potential everywhere in space. | ||

+ | * Maple/Mathematica representation of elliptic integral - After finding the elliptic integral and doing the power series expansion, students can see what electric potential `looks like' over all space by using a {{activities:guides:vfvring.mw|Maple}} or {{activities:guides:vfvring.nb|Mathematica}} worksheet. | ||

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+ | This activity is a part of the [[whitepapers:sequences:emsequence:start|Ring Sequence]], which uses a sequence of activities with similar geometries to help students learn how to solve a hard activity by breaking it up into several steps ([[publications:start#student_theses|A Master's Thesis]] about the Ring Sequence). The other activities in the sequence are: | ||

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+ | *Preceding Activity: | ||

+ | *[[courses:activities:vfact:vfvpoints|Electrostatic Potential Due to Two Point Charges]]: Students use what they learned about finding the distance between two points and apply what they know about power series approximations to find a general expression and asymptotic solution to the electrostatic potential due to two point charges. | ||

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+ | *Follow-up Activities: | ||

+ | *[[courses:activities:vfact:vfering|Electric Field Due to a Ring of Charge]]: In this small group activity, students use the definition of the electric field as $\vec{E}(\vec{r})=\frac{1}{4\pi\epsilon_0}\int_{ring}{\frac{\lambda(\vec{r'})(\vec{r}-\vec{r'})|d\vec{r'}|}{|\vec{r}-\vec{r'}|^3}} $ in order to work out the electric field due to a ring of charge. | ||

+ | *[[courses:activities:vfact:vfaring|Magnetic Vector Potential Due to a Spinning Ring of Charge]]: This small group activity is the magnetic analogy to [[courses:activities:vfact:vfvring|Electrostatic Potential Due to a Ring of Charge]] where students solve for the magnetic vector potential due to a spinning ring of charge. The set up for this problem is more complex because students now must think about current densities and the inherent vector nature of the magnetic vector potential. | ||

+ | *[[courses:activities:vfact:vfbring|Magnetic Field Due to a Spinning Ring of Charge]]: Building from their experience with the previous exercises, students in this small group activity use techniques from the previous activities to obtain an expression for the magnetic field due to a spinning ring of charge. | ||

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+ | This activity is part of the sequence of activities addressing [[whitepapers:sequences:scalarfieldseq|Representations of Scalar Fields]] in the context of electrostatic potentials. | ||

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+ | *Preceding Activities: | ||

+ | *[[swbq:emsw:vfswpointpot|Electrostatic Potential due to a Point Charge]]: This small whiteboard question asks students to recall the electrostatic potential due to a point charge which results in discussions likely to include notation of the distance from the origin to a point charge. | ||

+ | *[[courses:activities:vfact:vfdrawquadrupole|Drawing Equipotential Surfaces]]: This small group activity has students construct a contour plot of the electrostatic potential, level curves of equipotential, in the plane of four point charges. | ||

+ | *[[courses:activities:vfact:vfvisv|Visualizing Electrostatic Potentials]]: Students begin by brainstorming ways in which to represent three-dimensional scalar fields in two-dimensions and then use a Mathematica notebook to explore various representations for a distribution of point charges. | ||