Field of uniformly charged cylinder
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As with difficulty, there is no straight forward and generally accepted way.
But as a guideline, we tend to give as many points by default as there are mathematical steps to do in the exercise.
Again, very vague... But the number should kind of represent the "work" required.
When you click an exercise into a collection, this number will be taken as points for the exercise, kind of "by default".
But once the exercise is on the collection, you can edit the number of points for the exercise in the collection independently, without any effect on "points by default" as represented by the number here.
That being said... How many "default points" should you associate with an exercise upon creation?
As with difficulty, there is no straight forward and generally accepted way.
But as a guideline, we tend to give as many points by default as there are mathematical steps to do in the exercise.
Again, very vague... But the number should kind of represent the "work" required.
About difficulty...
We associate a certain difficulty with each exercise.
When you click an exercise into a collection, this number will be taken as difficulty for the exercise, kind of "by default".
But once the exercise is on the collection, you can edit its difficulty in the collection independently, without any effect on the "difficulty by default" here.
Why we use chess pieces? Well... we like chess, we like playing around with \(\LaTeX\)-fonts, we wanted symbols that need less space than six stars in a table-column... But in your layouts, you are of course free to indicate the difficulty of the exercise the way you want.
That being said... How "difficult" is an exercise? It depends on many factors, like what was being taught etc.
In physics exercises, we try to follow this pattern:
Level 1 - One formula (one you would find in a reference book) is enough to solve the exercise. Example exercise
Level 2 - Two formulas are needed, it's possible to compute an "in-between" solution, i.e. no algebraic equation needed. Example exercise
Level 3 - "Chain-computations" like on level 2, but 3+ calculations. Still, no equations, i.e. you are not forced to solve it in an algebraic manner. Example exercise
Level 4 - Exercise needs to be solved by algebraic equations, not possible to calculate numerical "in-between" results. Example exercise
Level 5 -
Level 6 -
When you click an exercise into a collection, this number will be taken as difficulty for the exercise, kind of "by default".
But once the exercise is on the collection, you can edit its difficulty in the collection independently, without any effect on the "difficulty by default" here.
Why we use chess pieces? Well... we like chess, we like playing around with \(\LaTeX\)-fonts, we wanted symbols that need less space than six stars in a table-column... But in your layouts, you are of course free to indicate the difficulty of the exercise the way you want.
That being said... How "difficult" is an exercise? It depends on many factors, like what was being taught etc.
In physics exercises, we try to follow this pattern:
Level 1 - One formula (one you would find in a reference book) is enough to solve the exercise. Example exercise
Level 2 - Two formulas are needed, it's possible to compute an "in-between" solution, i.e. no algebraic equation needed. Example exercise
Level 3 - "Chain-computations" like on level 2, but 3+ calculations. Still, no equations, i.e. you are not forced to solve it in an algebraic manner. Example exercise
Level 4 - Exercise needs to be solved by algebraic equations, not possible to calculate numerical "in-between" results. Example exercise
Level 5 -
Level 6 -
Question
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Exercise:
A long hollow cylinder is uniformly charged with linear charge density lambda. abcliste abc Using Gauss's law show that there is no electric field on the inside of the cylinder. abc Using Gauss's law show that the electric field on the outside of the cylinder is given by Er fracpivarepsilon_ fraclambdar where r is the distance from the central axis of the cylinder. abcliste
Solution:
abcliste abc If there is an electric field on the inside of the cylinder it has to respect the symmetry of the charge distribution i.e. the field lines are perpicular to the inner wall of the cylinder an po towards the centre or away from it and the magnitude of the field vectors is constant for a given distance from the centre. An appropriate closed surface Gaussian surface is therefore a cylinder with radius rR where R is the radius of the cylinder. The electric flux through this cylinder is then see inner green cylinder in figure center includegraphicswidthtextwidth#image_path:gauss-cylinder-# center Phi_E Er Ar Er pi r L where L is the length of the cylinder. The flux through the circular pieces is zero since the field lines are parallel. Using Gauss's law Phi_E fracsscQenclosedvarepsilon_ it follows that Er for rR abc For the field on the outside the cylindrical symmetry again implies a radial field. In order to find an expression for the electric field at distance r' R from the cylinder axis we choose a cylindrical surface with the corresponding radius. The electric flux is see a Phi_E Er' Ar Er' pi r' L Using Gauss's law it follows that Er' fracsscQenclosedpi r' L varepsilon_ fracpivarepsilon_ fraclambdar' quad square abcliste
A long hollow cylinder is uniformly charged with linear charge density lambda. abcliste abc Using Gauss's law show that there is no electric field on the inside of the cylinder. abc Using Gauss's law show that the electric field on the outside of the cylinder is given by Er fracpivarepsilon_ fraclambdar where r is the distance from the central axis of the cylinder. abcliste
Solution:
abcliste abc If there is an electric field on the inside of the cylinder it has to respect the symmetry of the charge distribution i.e. the field lines are perpicular to the inner wall of the cylinder an po towards the centre or away from it and the magnitude of the field vectors is constant for a given distance from the centre. An appropriate closed surface Gaussian surface is therefore a cylinder with radius rR where R is the radius of the cylinder. The electric flux through this cylinder is then see inner green cylinder in figure center includegraphicswidthtextwidth#image_path:gauss-cylinder-# center Phi_E Er Ar Er pi r L where L is the length of the cylinder. The flux through the circular pieces is zero since the field lines are parallel. Using Gauss's law Phi_E fracsscQenclosedvarepsilon_ it follows that Er for rR abc For the field on the outside the cylindrical symmetry again implies a radial field. In order to find an expression for the electric field at distance r' R from the cylinder axis we choose a cylindrical surface with the corresponding radius. The electric flux is see a Phi_E Er' Ar Er' pi r' L Using Gauss's law it follows that Er' fracsscQenclosedpi r' L varepsilon_ fracpivarepsilon_ fraclambdar' quad square abcliste
Meta Information
Exercise:
A long hollow cylinder is uniformly charged with linear charge density lambda. abcliste abc Using Gauss's law show that there is no electric field on the inside of the cylinder. abc Using Gauss's law show that the electric field on the outside of the cylinder is given by Er fracpivarepsilon_ fraclambdar where r is the distance from the central axis of the cylinder. abcliste
Solution:
abcliste abc If there is an electric field on the inside of the cylinder it has to respect the symmetry of the charge distribution i.e. the field lines are perpicular to the inner wall of the cylinder an po towards the centre or away from it and the magnitude of the field vectors is constant for a given distance from the centre. An appropriate closed surface Gaussian surface is therefore a cylinder with radius rR where R is the radius of the cylinder. The electric flux through this cylinder is then see inner green cylinder in figure center includegraphicswidthtextwidth#image_path:gauss-cylinder-# center Phi_E Er Ar Er pi r L where L is the length of the cylinder. The flux through the circular pieces is zero since the field lines are parallel. Using Gauss's law Phi_E fracsscQenclosedvarepsilon_ it follows that Er for rR abc For the field on the outside the cylindrical symmetry again implies a radial field. In order to find an expression for the electric field at distance r' R from the cylinder axis we choose a cylindrical surface with the corresponding radius. The electric flux is see a Phi_E Er' Ar Er' pi r' L Using Gauss's law it follows that Er' fracsscQenclosedpi r' L varepsilon_ fracpivarepsilon_ fraclambdar' quad square abcliste
A long hollow cylinder is uniformly charged with linear charge density lambda. abcliste abc Using Gauss's law show that there is no electric field on the inside of the cylinder. abc Using Gauss's law show that the electric field on the outside of the cylinder is given by Er fracpivarepsilon_ fraclambdar where r is the distance from the central axis of the cylinder. abcliste
Solution:
abcliste abc If there is an electric field on the inside of the cylinder it has to respect the symmetry of the charge distribution i.e. the field lines are perpicular to the inner wall of the cylinder an po towards the centre or away from it and the magnitude of the field vectors is constant for a given distance from the centre. An appropriate closed surface Gaussian surface is therefore a cylinder with radius rR where R is the radius of the cylinder. The electric flux through this cylinder is then see inner green cylinder in figure center includegraphicswidthtextwidth#image_path:gauss-cylinder-# center Phi_E Er Ar Er pi r L where L is the length of the cylinder. The flux through the circular pieces is zero since the field lines are parallel. Using Gauss's law Phi_E fracsscQenclosedvarepsilon_ it follows that Er for rR abc For the field on the outside the cylindrical symmetry again implies a radial field. In order to find an expression for the electric field at distance r' R from the cylinder axis we choose a cylindrical surface with the corresponding radius. The electric flux is see a Phi_E Er' Ar Er' pi r' L Using Gauss's law it follows that Er' fracsscQenclosedpi r' L varepsilon_ fracpivarepsilon_ fraclambdar' quad square abcliste
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