Chap28_PHY2049 - Chapter 28 – Sources of Magnetic Field -...

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Unformatted text preview: Chapter 28 – Sources of Magnetic Field - Magnetic Field of a Moving Charge - Magnetic Field of a Current Element - Magnetic Field of a Straight Current-Carrying Conductor - Force Between Parallel Conductors - Magnetic Field of a Circular Current Loop - Ampere’s Law - Applications of Ampere’s Law - Magnetic Materials 1. Magnetic Field of a Moving Charge - A charge creates a magnetic field only when the charge is moving. Source point: location of the moving charge. Field point: point P where we want to find the field. Magnetic field from a point charge moving with constant speed µ0 q v sin ϕ B= 4π r2 µ0 = 4π·10-7 Wb/A·m = N s2/C2 = N/A2 = T m/A (permeability of vacuum) c = (1/µ0ε0)1/2 speed of light Magnetic field of a point charge moving with constant velocity ˆ µ 0 qv × r B= 4π r 2 ˆ r = r / r = vector from source to field point Moving Charge: Magnetic Field Lines - The magnetic field lines are circles centered on the line of v and lying in planes perpendicular to that line. point right thumb in - Direction of field line: right hand rule for + charge direction of v. Your fingers curl around the charge in direction of magnetic field lines. 2. Magnetic Field of a Current Element - The total magnetic field caused by several moving charges is the vector sum of the fields caused by the individual charges. dQ = nqAdl (total moving charge in volume element dl A) Moving charges in current element are equivalent to dQ moving with drift velocity. µ 0 dQ vd sin ϕ µ 0 n q vd Adl sin ϕ µ 0 Idl sin ϕ dB = = = 2 4π r 4π r 4π r2 2 (I = n q vd A) Current Element: Vector Magnetic Field µ0 B= 4π ˆ Idl × r ∫ r2 Law of Biot and Savart Current Element: Magnetic Field Lines - Field vectors (dB) and magnetic field lines of a current element (dl) are like those generated by a + charge dQ moving in direction of vdrift. - Field lines are circles in planes ┴ to dl and centered on line of dl. 3. Magnetic Field of a Straight Current-Carrying Conductor µ0 B= 4π ˆ Idl × r ∫ r2 ˆ dl × r = dl ⋅1 ⋅ sin ϕ = dl ⋅ sin(π − ϕ ) = µ0 I B= 4π dl ⋅ x x2 + y2 a x ⋅ dy 2a µ0 I ∫a ( x 2 + y 2 )3 / 2 = 4π x x 2 + a 2 − If conductors length 2a >> x µ 0 I ( 2a ) µ 0 I B= = 4π ⋅ x ⋅ a 2π ⋅ x µ0 I B= 2π ⋅ r B direction: into the plane of the figure, perpendicular to x-y plane Field near a long, straight current-carrying conductor - Electric field lines radiate outward from + line charge distribution. They begin and end at electric charges. - Magnetic field lines encircle the current that acts as their source. They form closed loops and never have end points. -The total magnetic flux through any closed surface is zero there are no isolated magnetic charges (or magnetic monopoles) any magnetic field line that enters a closed surface must also emerge from that surface. 4. Force Between Parallel Conductors - Two conductors with current in same direction. Each conductor lies in B set-up by the other conductor. B generated by lower conductor at the position of upper conductor: B= µ0 I 2π ⋅ r F = I'L× B µ0 I F = I ' LB = I ' L 2π ⋅ r F µ0 I ⋅ I ' = L 2π ⋅ r Two long parallel current-carrying conductors Force on upper conductor is downward. - Parallel conductors carrying currents in same direction attract each other. If I has contrary direction they repel each other. Magnetic Forces and Defining the Ampere - One Ampere is the unvarying current that, if present in each of the two parallel conductors of infinite length and one meter apart in empty space, causes each conductor to experience a force of exactly 2 x 10-7 N per meter of length. 5. Magnetic Field of a Circular Current Loop ˆ µ 0 Idl × r µ Idl B= B= 0 2 4π ∫ r 2 4π r µ0 I dl dB = 4π (x 2 + a 2 ) dBx = dB cos θ = µ0 I dl a 4π (x 2 + a 2 ) (x 2 + a 2 )1/ 2 µ0 I dl x dB y = dB sin θ = 4π (x 2 + a 2 ) (x 2 + a 2 )1/ 2 - Rotational symmetry about x axis no B component perpendicular to x. For dl on opposite sides of loop, dBx are equal in magnitude and in same direction, dBy have same magnitude but opposite direction (cancel). Bx = ∫ Bx = µ0 I µI µI adl a a =0 dl = 0 (2πa ) 2 2 3/ 2 2 2 3/ 2 ∫ 2 2 3/ 2 4π (x + a ) 4π (x + a ) 4π (x + a ) µ0 Ia 2 ( 2 x2 + a ) 2 3/ 2 (on the axis of a circular loop) Magnetic Field on the Axis of Coil µ 0 NIa 2 Bx = ( 2 2 x +a Bx = µ 0 NI ) 2 3/ 2 (on the axis of N circular loops) (at the center, x=0, of N circular loops) 2a µ = N ⋅ I ⋅ A = N ⋅ I ⋅ (πa 2 ) Bx = µ0 µ 2π ( x 2 + a 2 ) 3 / 2 (on the axis of any number of circular loops) 6. Ampere’s Law - Law that allows us to obtain the magnetic fields caused by highly symmetric current distributions. ∫ B ⋅ dl = ∫ B dl = µ I // 0 Ampere’s Law for a Long Straight Conductor µ0 I B= 2πr µ0 I ∫ B ⋅ dl =B ∫ dl = 2π ⋅ r (2π ⋅ r ) = µ0 I - Direction of current: right hand rule curl fingers of right hand around the integration path , the thumb indicates positive current direction. For an integration path that does not enclose the conductor: µ0 I B// = B1 = 2π ⋅ r1 − µ0 I B// = − B2 = 2π ⋅ r2 (circular arc ab) (circular arc cd ) B and dl antiparallel arc = (angle) x (radius) = θ r b c d a c d ∫ B ⋅ dl = ∫ B dl =B ∫ dl + (0)∫ dl + (− B )∫ dl +(0)∫ dl = // 1 2 a b µ0 I µ0 I = (r1θ ) + 0 − (r2θ ) + 0 = 0 2π ⋅ r1 2π ⋅ r2 B ⋅ dl = B ⋅ dl ⋅ cos ϕ = B ⋅ r ⋅ dθ µ0 I µ0 I ∫ B ⋅ dl = ∫ 2π ⋅ r (rdθ ) = 2π ∫ dθ =µ0 I - This result does not depend on the shape of the path or on position of the wire inside it. - If the path does not enclose the wire ∫ dθ = 0 around integration path. Ampere’s Law: General Statement - The total magnetic field at any point in the path is the vector sum of all fields produced by the individual conductors. ∫ B ⋅ dl =µ 0 I -If the integration path does not enclose a wire ∫ B ⋅ dl ∫ B ⋅ dl =µ 0 I encl ∫ B ⋅ dl =0 =0 does not mean that B = 0 everywhere along the path, only that Iencl = 0. ∫ B ⋅ dl 7. Applications of Ampere’s Law Ex. 28.8 =0 Ex. 28.9 Ex. 28.10 8. Magnetic Materials - Atoms contain moving electrons, e- form microscopy current loops that produce magnetic fields (randomly oriented, no net Bint). In some materials, external Bext causes these loops to orient with field, adding to the Bext magnetized material. - An electron moving with speed v in a circular orbit of radius r has an angular momentum L and oppositely directed orbital magnetic dipole moment µ. It also has a spin angular momentum and oppositely directed spin magnetic dipole moment. e e ev I= = = T 2π ⋅ r / v 2π ⋅ r ev evr 2µ 2 µ = I⋅A= (π ⋅ r ) = → v= 2π ⋅ r 2 e⋅r Model of electron in an atom Angular momentum of e-: L=r×p 2 µ 2 µm L = r ⋅ p = r ⋅ mv = r ⋅ m = e⋅r e µ= e L 2m - Atomic angular momentum is quantized: L ~ h/2π (its component along a direction is always an integer multiple of this value). (h = Planck constant = 6.626 x 10-34 J s) - Associated with the quantization of L is an uncertainty in direction of L and of µ (since they are related). e eh eh µB = L= = 9.274 ⋅10 − 24 Am 2 or J / T Bohr Magneton = 2m 2m 2π 4π ⋅ m - Electrons have intrinsic angular momentum (Spin) that is not related to orbital motion, but can be seen as spinning on an axis. The angular momentum has an associated magnetic moment with magnitude ≈ µB. Magnetic Materials - When magnetic materials are present, the magnetization of the material causes an additional contribution to B. Paramagnetism - In an atom, most of the orbital and spin magnetic moments add to zero. However, in case cases the atom has magnetic moment µB. If such atom is placed on B, the field will exert a torque: τ = µ×B this torque aligns the magnetic moment with magnetic field (position of minimum potential energy). In that position, the current loops add to the externally applied B. - B produced by a current loop is proportional to loop’s magnetic dipole moment µ additional B produced by electron current loops proportional to µtotal per unit volume of material (V) = Magnetization. Magnetization: M= µtotal Units: (A m2)/m3 = A/m V - Additional magnetic field due to M of material is: µ0 M - When a magnetized material surrounds a current-carrying conductor, the total B is: B = B0 + µ 0 M B0 = field caused by the current conductor behavior typical of a paramagnetic material. - The magnetic field at any point in a paramagnetic material is greater by the factor Km (relative permeability of the material) than it will be if the material were replaced by vacuum. - All equations from this chapter can be adapted to the situation in which the current-carrying conductor is embedded in a paramagnetic material by replacing µ0 Km µ0. Permeability: µ = K m µ0 Careful ! We have used the same symbol “µ” to represent two different physical quantities, the magnetic dipole moment (a vector), and the permeability (an scalar). Paramagnetism Magnetic Susceptibility: (χm small but >0) χm = Km −1 Km and χm are dimensionless. - The tendency of atomic magnetic moments to align themselves parallel to B is opposed by random thermal motion χm decreases with increasing T. B M =C T Curie’s Law C = constant T = temperature - An object with magnetic dipoles is attracted to magnet poles. Weak attraction in paramagnetic materials due to thermal randomization of magnetic moments. At low T, M increases stronger attractive forces. Diamagnetism - Total magnetic moment of all atomic current loops = 0 in absence of B. - These materials can still show magnetic effects when external Bext alters e- motion in atoms induced magnetic moment. The additional induced B has opposite direction to Bext (see Chap. 29). - An induced current always tends to cancel the field change that caused it. - Susceptibility χ < 0 and small. - Relative permeability Km slightly less than 1. Ferromagnetism (FM) - Strong interactions between atomic magnetic moments cause them to align parallel to each other in regions (magnetic domains) even when no Bext is present. Ex: Fe, Co. - If no Bext oriented. domain magnetizations are randomly domain M tend to align parallel to field, - If Bext domain boundaries shift, domains with M parallel to B grow. - Km >> 1 - Ferromagnets are strongly magnetized by Bext and attracted to magnet. -Saturation magnetization: M reached when all magnetic moments from FM are aligned // Bext. Once Msat is reached, increasing Bext will not change M. - For many FM materials, the relation between M and Bext = B0 is different when you increase or decrease B0 hysteresis loop. - In permanent magnets, after Msat is reached and B0 is reduced to zero, some M remains (remnant magnetization). To reduce M to zero requires B to change direction. Ferromagnetism Ferromagnetism - Magnetizing and de-magnetizing a material that has hysteresis involves dissipation of energy materials’ temperature increases. ...
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This note was uploaded on 07/30/2011 for the course PHY 2049 taught by Professor Saha during the Spring '08 term at University of Central Florida.

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