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Unformatted text preview: Chapter 36 The BiotSavart Law 318 36 The BiotSavart Law The BiotSavart Law provides us with a way to find the magnetic field at an empty point in space, let’s call it point P , due to current in wire. The idea behind the BiotSavart Law is that each infinitesimal element of the currentcarrying wire makes an infinitesimal contribution to the magnetic field at the empty point in space. Once you find each contribution, all you have to do is add them all up. Of course, there are an infinite number of contributions to the magnetic field at point P and each one is a vector, so, we are talking about an infinite sum of vectors. This business should seem familiar to you. You did this kind of thing when you were calculating the electric field back in Chapter 30 The Electric Field Due to a Continuous Distribution of Charge on a Line . The idea is similar, but here, of course, we are talking about magnetism. The BiotSavart Law gives the infinitesimal contribution to the magnetic field at point P due to an infinitesimal element of the currentcarrying wire. The following diagram helps to illustrate just what the BiotSavart Law tells us. The BiotSavart Law states that: 3 o 4 r I r l h h h × = d B d π μ (361) The BiotSavart Law represents a powerful straightforward method of calculating the magnetic field due to a current distribution. I r P d l dB Chapter 36 The BiotSavart Law 319 Example 361 Calculate the magnetic field due to a long straight wire carrying a current I along the z axis in the positive z direction. Treat the wire as extending to infinity in both directions....
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This note was uploaded on 02/29/2012 for the course PHYS 227 taught by Professor Rabe during the Fall '08 term at Rutgers.
 Fall '08
 RABE
 Physics, Current

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