Trägheitsmoment einer Scheibe bzw. eines Zylinders
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
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Exercise:
Bestimme das Trägheitsmoment einer homogenen Scheibe mit der Masse m und dem Radius R bezüglich ihrer Symmetrieachse.
Solution:
Das Trägheitsmoment einer Scheibe mit der Dicke D und der homogenen Dichte rho ist: I r^ mboxdm && mboxdm rho mboxdV r^ rho mboxdV && mboxdVrmboxdrmboxdphimboxdztext Zylinderkoordinaten rho r^ rmboxdrmboxdphimboxdz && textIntegrationsgrenzen festlegen rho _^R r^mboxdr _^pimboxdphi _^Dmboxdz && textegrieren rho leftfrac r^right_^R pi D rho frac R^ pi D && textsortieren frac rho D pi R^ R^ && A pi R^ text Kreisfläche frac rho AD R^ && m rho V rho AD frac mR^ Der Wechsel von kartesischen Koordinaten nach Zylinderkoordinaten mboxdxmboxdymboxdzrightarrow rmboxdrmboxdphimboxdz ist eigentlich eine glqq Substitutiongrqq von drei Variablen. Dafür muss die Jacobi-Matrix dieser Transformation ausgerechnet werden; ihre Determinante ist r was das r in rmboxdrmboxdphimboxdz erklärt. Die Koordinatentransformation sieht wie folgt aus: x rcosphi &f_rphi z y rsinphi &f_rphi z z z & f_rphi z Die Jacobi-Matrix dieser Koordinatentransformation ist: J fracpartial f_ipartial x'_j fracpartialxyzpartialrphiz pmatrix fracpartial xpartial r & fracpartial xpartial phi & fracpartial xpartial z fracpartial ypartial r & fracpartial ypartial phi & fracpartial ypartial z fracpartial zpartial r & fracpartial zpartial phi & fracpartial zpartial z pmatrix pmatrix cosphi & -rsinphi & sinphi & rcosphi & & & pmatrix Die Determinante dieser Matrix kann einfach ausgerechnet werden: Sie ist r. Daher: mboxdxmboxdymboxdzrightarrow rmboxdrmboxdphimboxdz.
Bestimme das Trägheitsmoment einer homogenen Scheibe mit der Masse m und dem Radius R bezüglich ihrer Symmetrieachse.
Solution:
Das Trägheitsmoment einer Scheibe mit der Dicke D und der homogenen Dichte rho ist: I r^ mboxdm && mboxdm rho mboxdV r^ rho mboxdV && mboxdVrmboxdrmboxdphimboxdztext Zylinderkoordinaten rho r^ rmboxdrmboxdphimboxdz && textIntegrationsgrenzen festlegen rho _^R r^mboxdr _^pimboxdphi _^Dmboxdz && textegrieren rho leftfrac r^right_^R pi D rho frac R^ pi D && textsortieren frac rho D pi R^ R^ && A pi R^ text Kreisfläche frac rho AD R^ && m rho V rho AD frac mR^ Der Wechsel von kartesischen Koordinaten nach Zylinderkoordinaten mboxdxmboxdymboxdzrightarrow rmboxdrmboxdphimboxdz ist eigentlich eine glqq Substitutiongrqq von drei Variablen. Dafür muss die Jacobi-Matrix dieser Transformation ausgerechnet werden; ihre Determinante ist r was das r in rmboxdrmboxdphimboxdz erklärt. Die Koordinatentransformation sieht wie folgt aus: x rcosphi &f_rphi z y rsinphi &f_rphi z z z & f_rphi z Die Jacobi-Matrix dieser Koordinatentransformation ist: J fracpartial f_ipartial x'_j fracpartialxyzpartialrphiz pmatrix fracpartial xpartial r & fracpartial xpartial phi & fracpartial xpartial z fracpartial ypartial r & fracpartial ypartial phi & fracpartial ypartial z fracpartial zpartial r & fracpartial zpartial phi & fracpartial zpartial z pmatrix pmatrix cosphi & -rsinphi & sinphi & rcosphi & & & pmatrix Die Determinante dieser Matrix kann einfach ausgerechnet werden: Sie ist r. Daher: mboxdxmboxdymboxdzrightarrow rmboxdrmboxdphimboxdz.
Meta Information
Exercise:
Bestimme das Trägheitsmoment einer homogenen Scheibe mit der Masse m und dem Radius R bezüglich ihrer Symmetrieachse.
Solution:
Das Trägheitsmoment einer Scheibe mit der Dicke D und der homogenen Dichte rho ist: I r^ mboxdm && mboxdm rho mboxdV r^ rho mboxdV && mboxdVrmboxdrmboxdphimboxdztext Zylinderkoordinaten rho r^ rmboxdrmboxdphimboxdz && textIntegrationsgrenzen festlegen rho _^R r^mboxdr _^pimboxdphi _^Dmboxdz && textegrieren rho leftfrac r^right_^R pi D rho frac R^ pi D && textsortieren frac rho D pi R^ R^ && A pi R^ text Kreisfläche frac rho AD R^ && m rho V rho AD frac mR^ Der Wechsel von kartesischen Koordinaten nach Zylinderkoordinaten mboxdxmboxdymboxdzrightarrow rmboxdrmboxdphimboxdz ist eigentlich eine glqq Substitutiongrqq von drei Variablen. Dafür muss die Jacobi-Matrix dieser Transformation ausgerechnet werden; ihre Determinante ist r was das r in rmboxdrmboxdphimboxdz erklärt. Die Koordinatentransformation sieht wie folgt aus: x rcosphi &f_rphi z y rsinphi &f_rphi z z z & f_rphi z Die Jacobi-Matrix dieser Koordinatentransformation ist: J fracpartial f_ipartial x'_j fracpartialxyzpartialrphiz pmatrix fracpartial xpartial r & fracpartial xpartial phi & fracpartial xpartial z fracpartial ypartial r & fracpartial ypartial phi & fracpartial ypartial z fracpartial zpartial r & fracpartial zpartial phi & fracpartial zpartial z pmatrix pmatrix cosphi & -rsinphi & sinphi & rcosphi & & & pmatrix Die Determinante dieser Matrix kann einfach ausgerechnet werden: Sie ist r. Daher: mboxdxmboxdymboxdzrightarrow rmboxdrmboxdphimboxdz.
Bestimme das Trägheitsmoment einer homogenen Scheibe mit der Masse m und dem Radius R bezüglich ihrer Symmetrieachse.
Solution:
Das Trägheitsmoment einer Scheibe mit der Dicke D und der homogenen Dichte rho ist: I r^ mboxdm && mboxdm rho mboxdV r^ rho mboxdV && mboxdVrmboxdrmboxdphimboxdztext Zylinderkoordinaten rho r^ rmboxdrmboxdphimboxdz && textIntegrationsgrenzen festlegen rho _^R r^mboxdr _^pimboxdphi _^Dmboxdz && textegrieren rho leftfrac r^right_^R pi D rho frac R^ pi D && textsortieren frac rho D pi R^ R^ && A pi R^ text Kreisfläche frac rho AD R^ && m rho V rho AD frac mR^ Der Wechsel von kartesischen Koordinaten nach Zylinderkoordinaten mboxdxmboxdymboxdzrightarrow rmboxdrmboxdphimboxdz ist eigentlich eine glqq Substitutiongrqq von drei Variablen. Dafür muss die Jacobi-Matrix dieser Transformation ausgerechnet werden; ihre Determinante ist r was das r in rmboxdrmboxdphimboxdz erklärt. Die Koordinatentransformation sieht wie folgt aus: x rcosphi &f_rphi z y rsinphi &f_rphi z z z & f_rphi z Die Jacobi-Matrix dieser Koordinatentransformation ist: J fracpartial f_ipartial x'_j fracpartialxyzpartialrphiz pmatrix fracpartial xpartial r & fracpartial xpartial phi & fracpartial xpartial z fracpartial ypartial r & fracpartial ypartial phi & fracpartial ypartial z fracpartial zpartial r & fracpartial zpartial phi & fracpartial zpartial z pmatrix pmatrix cosphi & -rsinphi & sinphi & rcosphi & & & pmatrix Die Determinante dieser Matrix kann einfach ausgerechnet werden: Sie ist r. Daher: mboxdxmboxdymboxdzrightarrow rmboxdrmboxdphimboxdz.
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