Dipole in Field of Charged Wire
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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.
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 dipole is placed in the field of a uniformly charged wire linear charge density lambda with its dipole moment vec p q vec d ed in the direction of the field lines. center includegraphicswidthtextwidth#image_path:dipoland-wir# center abcliste abc Show that for a distance r from the po charge Q with r gg d the force acting on the dipole can be written as F - fracpivarepsilon_ fraclambda pr^ abc Calculate the force on an HF hydrogen fluoride molecule at a distance rO from a wire with a linear charge density laO. The dipole moment of an HFL molecule is pO. Compare the result to the force acting on an electron at the same distance. abcliste
Solution:
abcliste abc The forces on the positive and negative charge of a dipole at distance r from a po charge Q are F_+ q E_Qr+d/ q fracpivarepsilon_ fraclambdar+d/ F_- -q E_Qr-d/ -q fracpivarepsilon_ fraclambdar-d/ where we ase a simple dipole with its negative charge facing the positively charged wire see figure. The net force is thus F q fracpivarepsilon_ lambda leftfracr+d/ - fracr-d/ right fracq lambdapivarepsilon_ fracr-d/ - r+d/r+d/ r-d/ fracq lambdapivarepsilon_ frac-dr^-d^/ &approx fracq lambdapivarepsilon_ frac-dr^ - fracpivarepsilon_ fracq d lambdar^ - fracpivarepsilon_ fraclambda pr^ In this situation the force pos towards the wire negative sign. abc The force acting on the molecule is F FF fracpitimesnceps timesfraclatimespr^ resultFS The force on an electron at the same distance from the wire would be F' FeF fracpitimesnceps times fraclatimesncer resultFeS The force on the dipole is much weaker than that on the electron. abcliste
A dipole is placed in the field of a uniformly charged wire linear charge density lambda with its dipole moment vec p q vec d ed in the direction of the field lines. center includegraphicswidthtextwidth#image_path:dipoland-wir# center abcliste abc Show that for a distance r from the po charge Q with r gg d the force acting on the dipole can be written as F - fracpivarepsilon_ fraclambda pr^ abc Calculate the force on an HF hydrogen fluoride molecule at a distance rO from a wire with a linear charge density laO. The dipole moment of an HFL molecule is pO. Compare the result to the force acting on an electron at the same distance. abcliste
Solution:
abcliste abc The forces on the positive and negative charge of a dipole at distance r from a po charge Q are F_+ q E_Qr+d/ q fracpivarepsilon_ fraclambdar+d/ F_- -q E_Qr-d/ -q fracpivarepsilon_ fraclambdar-d/ where we ase a simple dipole with its negative charge facing the positively charged wire see figure. The net force is thus F q fracpivarepsilon_ lambda leftfracr+d/ - fracr-d/ right fracq lambdapivarepsilon_ fracr-d/ - r+d/r+d/ r-d/ fracq lambdapivarepsilon_ frac-dr^-d^/ &approx fracq lambdapivarepsilon_ frac-dr^ - fracpivarepsilon_ fracq d lambdar^ - fracpivarepsilon_ fraclambda pr^ In this situation the force pos towards the wire negative sign. abc The force acting on the molecule is F FF fracpitimesnceps timesfraclatimespr^ resultFS The force on an electron at the same distance from the wire would be F' FeF fracpitimesnceps times fraclatimesncer resultFeS The force on the dipole is much weaker than that on the electron. abcliste
Meta Information
Exercise:
A dipole is placed in the field of a uniformly charged wire linear charge density lambda with its dipole moment vec p q vec d ed in the direction of the field lines. center includegraphicswidthtextwidth#image_path:dipoland-wir# center abcliste abc Show that for a distance r from the po charge Q with r gg d the force acting on the dipole can be written as F - fracpivarepsilon_ fraclambda pr^ abc Calculate the force on an HF hydrogen fluoride molecule at a distance rO from a wire with a linear charge density laO. The dipole moment of an HFL molecule is pO. Compare the result to the force acting on an electron at the same distance. abcliste
Solution:
abcliste abc The forces on the positive and negative charge of a dipole at distance r from a po charge Q are F_+ q E_Qr+d/ q fracpivarepsilon_ fraclambdar+d/ F_- -q E_Qr-d/ -q fracpivarepsilon_ fraclambdar-d/ where we ase a simple dipole with its negative charge facing the positively charged wire see figure. The net force is thus F q fracpivarepsilon_ lambda leftfracr+d/ - fracr-d/ right fracq lambdapivarepsilon_ fracr-d/ - r+d/r+d/ r-d/ fracq lambdapivarepsilon_ frac-dr^-d^/ &approx fracq lambdapivarepsilon_ frac-dr^ - fracpivarepsilon_ fracq d lambdar^ - fracpivarepsilon_ fraclambda pr^ In this situation the force pos towards the wire negative sign. abc The force acting on the molecule is F FF fracpitimesnceps timesfraclatimespr^ resultFS The force on an electron at the same distance from the wire would be F' FeF fracpitimesnceps times fraclatimesncer resultFeS The force on the dipole is much weaker than that on the electron. abcliste
A dipole is placed in the field of a uniformly charged wire linear charge density lambda with its dipole moment vec p q vec d ed in the direction of the field lines. center includegraphicswidthtextwidth#image_path:dipoland-wir# center abcliste abc Show that for a distance r from the po charge Q with r gg d the force acting on the dipole can be written as F - fracpivarepsilon_ fraclambda pr^ abc Calculate the force on an HF hydrogen fluoride molecule at a distance rO from a wire with a linear charge density laO. The dipole moment of an HFL molecule is pO. Compare the result to the force acting on an electron at the same distance. abcliste
Solution:
abcliste abc The forces on the positive and negative charge of a dipole at distance r from a po charge Q are F_+ q E_Qr+d/ q fracpivarepsilon_ fraclambdar+d/ F_- -q E_Qr-d/ -q fracpivarepsilon_ fraclambdar-d/ where we ase a simple dipole with its negative charge facing the positively charged wire see figure. The net force is thus F q fracpivarepsilon_ lambda leftfracr+d/ - fracr-d/ right fracq lambdapivarepsilon_ fracr-d/ - r+d/r+d/ r-d/ fracq lambdapivarepsilon_ frac-dr^-d^/ &approx fracq lambdapivarepsilon_ frac-dr^ - fracpivarepsilon_ fracq d lambdar^ - fracpivarepsilon_ fraclambda pr^ In this situation the force pos towards the wire negative sign. abc The force acting on the molecule is F FF fracpitimesnceps timesfraclatimespr^ resultFS The force on an electron at the same distance from the wire would be F' FeF fracpitimesnceps times fraclatimesncer resultFeS The force on the dipole is much weaker than that on the electron. abcliste
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