- #1
schrodingerwitch
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Considering an stopped object in a horizontal plane, the frictional force between the object and the plane would be the product of the friction coefficient (static or kinetic if there was movement between the surfaces) by normal. Since the normal in this case would be given by N (vector) = - mg j (unit), we would have the frictional force given by F (vector) = - mgμ j (unit).
But we know that the frictional force must act against the direction of the object's movement, so its unit vector must have direction î (unitary).
Is this change in the unit vector simply a convention that comes from agreement with experimental physics or is there some kind of vector transformation that makes this vector j^ already become a vector î?
The books I researched were Halliday, Tipler, Moysés and Young and Freedman. In none of them did I see comments about it, so I think it might be trivial, but I wanted to clear that doubt. The only book that talked about it was Alonso and Finn - A University Course, but it was just a comment and I found it confusing.
But we know that the frictional force must act against the direction of the object's movement, so its unit vector must have direction î (unitary).
Is this change in the unit vector simply a convention that comes from agreement with experimental physics or is there some kind of vector transformation that makes this vector j^ already become a vector î?
The books I researched were Halliday, Tipler, Moysés and Young and Freedman. In none of them did I see comments about it, so I think it might be trivial, but I wanted to clear that doubt. The only book that talked about it was Alonso and Finn - A University Course, but it was just a comment and I found it confusing.