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Understanding Magnetism & Electromagnetism: Maxwell's Equations & Transforming Fields, Slides of Physics

An in-depth exploration of magnetism, focusing on maxwell's equations and the consequences of special relativity, including length contraction and time dilation. The document also covers the lorentz force law, transforming electromagnetic fields, and faraday's law. Students will learn how to calculate magnetic fields in different frames of reference and understand the relationship between electric and magnetic fields.

Typology: Slides

2012/2013

Uploaded on 07/26/2013

sankrant
sankrant 🇮🇳

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Download Understanding Magnetism & Electromagnetism: Maxwell's Equations & Transforming Fields and more Slides Physics in PDF only on Docsity! wee - Maxwell’s Equations General Physics 2 Magnetism 1 3 Docsity.com Postulates of Special Relativity •  The laws of physics are the same for all inertial observers. •  The speed of light is the same for all observers. General Physics 2 Magnetism 2 Docsity.com General Physics 2 Magnetism 5 Lorentz Force Law •  The equation describes fht force exerted by an electromagnetic field on a particle with charge q in a frame where the particle moves with velocity, v. •  Applies only to particles €  F em = q  E +  v c ×  B bar       Docsity.com General Physics 2 Magnetism 6 How Fields Transform •  Given E and B in an inertial reference frame, we can calculate E and B in a moving frame •  Frame is moving at a speed v in the + x-direction •  β = v/c, and γ= (1 – v2/c2)-1/2 €  ′ E x  ′ E y  ′ E z           =  E x γ Ey −βBbar,z( ) γ Ez + βBbar,y( )           and  ′ B bar,x  ′ B bar,y  ′ B bar,z           = Bbar,x γ Bbar,y + βBbar,z( ) γ Bbar,z −βEy( )           Docsity.com General Physics 2 Magnetism 7 Transforming Fields - example •  Example 13.1 •  Calculate the magnetic field in the particle’s frame •  B is in the –y direction •  E is in the postive z direction •  β = v/c, and γ= (1 – v2/c2)-1/2 €  ′ E x  ′ E y  ′ E z           =  E x γ Ey −βBbar,z( ) γ Ez + βBbar,y( )           and  ′ B bar,x  ′ B bar,y  ′ B bar,z           = Bbar,x γ Bbar,y + βEz( ) γ Bbar,z −βEy( )           Docsity.com General Physics 2 Magnetism 10 Maxwell’s Equations •  Field inside spherical charge distribution € curl  B bar( ) − 1c d  E dt = 1 ε0  J c € curl  E ( ) + 1c d  B bar dt = 0 € div  E ( ) = ρ ε0 € div  B bar( ) = 0 Docsity.com Group Problems •  Review Two Minute Problems •  Whiteboard T2, T3, and T7 •  E13B.1 •  E13S.2 General Physics 2 Magnetism 11 Docsity.com
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