Magnetfeldstärke im Massenspektrometer für Uran-Isotope
About points...
We associate a certain number of points with each exercise.
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.
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
Solution
Short
Video
\(\LaTeX\)
Need help? Yes, please!
The following quantities appear in the problem:
Masse \(m\) / elektrische Ladung \(q, Q\) / Magnetische Flussdichte \(B\) / Kraft \(F\) / elektrische Spannung \(U\) / Energie \(E\) / Geschwindigkeit \(v\) / Radius \(r\) /
The following formulas must be used to solve the exercise:
\(E = qU \quad \) \(E_{\rm \scriptscriptstyle kin} = \dfrac12 mv^2 \quad \) \(F = qvB \quad \) \(F = m\dfrac{v^2}{r} \quad \)
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Exercise:
Mit einem Massenspektrometer sollen einfach negativ ionisierte Urankerne getrennt werden. Dazu werden sowohl isotopeU als auch isotopeU-Kerne mit vO in ein Massenspektrometer geschossen. Wie stark müsste das Magnetfeld im Massenspektrometer sein damit die Kerne räumlich um ddO getrennt würden d.h. die Kreisdurchmesser ihrer Flugbahnen sich um so viel unterschieden?
Solution:
NewQtydm.kg NewQtyvbe NewQtyq.C NewQtydm Aus den Überlegungen für Kreisbewegungen mfracv^rqvB folgt direkt dass r fracmvqB der Kreisradius der Bahn der Teilchen ist. Daraus kann man ableiten: Delta d Delta r fracDelta m vqB Somit gilt: SolQtyBdmX*vbX/qX/dXT B fracDelta m vq Delta d fracdm vbq d .eT
Mit einem Massenspektrometer sollen einfach negativ ionisierte Urankerne getrennt werden. Dazu werden sowohl isotopeU als auch isotopeU-Kerne mit vO in ein Massenspektrometer geschossen. Wie stark müsste das Magnetfeld im Massenspektrometer sein damit die Kerne räumlich um ddO getrennt würden d.h. die Kreisdurchmesser ihrer Flugbahnen sich um so viel unterschieden?
Solution:
NewQtydm.kg NewQtyvbe NewQtyq.C NewQtydm Aus den Überlegungen für Kreisbewegungen mfracv^rqvB folgt direkt dass r fracmvqB der Kreisradius der Bahn der Teilchen ist. Daraus kann man ableiten: Delta d Delta r fracDelta m vqB Somit gilt: SolQtyBdmX*vbX/qX/dXT B fracDelta m vq Delta d fracdm vbq d .eT
Meta Information
Exercise:
Mit einem Massenspektrometer sollen einfach negativ ionisierte Urankerne getrennt werden. Dazu werden sowohl isotopeU als auch isotopeU-Kerne mit vO in ein Massenspektrometer geschossen. Wie stark müsste das Magnetfeld im Massenspektrometer sein damit die Kerne räumlich um ddO getrennt würden d.h. die Kreisdurchmesser ihrer Flugbahnen sich um so viel unterschieden?
Solution:
NewQtydm.kg NewQtyvbe NewQtyq.C NewQtydm Aus den Überlegungen für Kreisbewegungen mfracv^rqvB folgt direkt dass r fracmvqB der Kreisradius der Bahn der Teilchen ist. Daraus kann man ableiten: Delta d Delta r fracDelta m vqB Somit gilt: SolQtyBdmX*vbX/qX/dXT B fracDelta m vq Delta d fracdm vbq d .eT
Mit einem Massenspektrometer sollen einfach negativ ionisierte Urankerne getrennt werden. Dazu werden sowohl isotopeU als auch isotopeU-Kerne mit vO in ein Massenspektrometer geschossen. Wie stark müsste das Magnetfeld im Massenspektrometer sein damit die Kerne räumlich um ddO getrennt würden d.h. die Kreisdurchmesser ihrer Flugbahnen sich um so viel unterschieden?
Solution:
NewQtydm.kg NewQtyvbe NewQtyq.C NewQtydm Aus den Überlegungen für Kreisbewegungen mfracv^rqvB folgt direkt dass r fracmvqB der Kreisradius der Bahn der Teilchen ist. Daraus kann man ableiten: Delta d Delta r fracDelta m vqB Somit gilt: SolQtyBdmX*vbX/qX/dXT B fracDelta m vq Delta d fracdm vbq d .eT
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Massenspektrometer by TeXercises
| Title | Matched on |
|---|---|
| Massenspektrometer um Kohlenstoff-Isotope zu trennen | tags |
| Massenspektrometer | tags |
| Massenspektrometer | tags |
| Kreisbahn | tags |
| Kreisbahn | tags |
Similar exercises (6)
| Title | Matched on |
|---|---|
| Massenspektrometer um Kohlenstoff-Isotope zu trennen | tags |
| Massenspektrometer | tags |
| Massenspektrometer | tags |
| Kreisbahn | tags |
| Kreisbahn | tags |
| Magnetfeld im Massenspektrometer für Uran | title |