23. ročník, úloha II . P telekinesis !!! chybí statistiky
Transkript
23. ročník, úloha II . P telekinesis !!! chybí statistiky
Fyzikální korespondenční seminář UK MFF http://fykos.mff.cuni.cz 23 . II . P 23. ročník, úloha II . P . . . telekinesis !!! chybí statistiky !!! Where does a permanent magnet take the power to lift stuff? We know that the magnetic force does no work. Lorenz equation, F = q(v × B), says that the magnetic force is perpen dicular to the velocity of a moving charge and therefore only changes its direction. In fact, the formula for the magnetic force does not imply zero work. Such a conclusion would be valid for a single charged particle without any other external forces. However, if there are some constraint forces (for example, consider an electron bound to the surface of a positively charged body by the electrostatic force) the magnetic force can act against those forces, pushing the particle to a configuration with a higher potential energy. If this is the case, the magnetic force must perform some work. It is also noteworthy that the magnetic field must be inhomogeneous to attract a magnetized body. (Any magnetic field created by a magnetic dipole is always inhomogeneous except for the centre of a dipole.) The total force of the magnetic force acting on a magnetic dipole is given by the following formula F = grad(m · B) where m denotes magnetic dipole moment. In case of a small loop, we have m = IS where I stands for the electric current in the loop and S is the area of the loop (oriented to its normal). A homogeneous magnetic field would only cause Larmor precession of a body but the total force would be zero. Marek Nečada [email protected] Fyzikální korespondenční seminář je organizován studenty UK MFF. Je zastřešen Oddělením pro vnější vztahy a propagaci UK MFF a podporován Ústavem teoretické fyziky UK MFF, jeho zaměstnanci a Jednotou českých matematiků a fyziků. -1-