Jan 23, 2008 - the analagous solution in four-dimensional General Relativity. .... galaxy clusters (for an excellent review of magnetic fields in the early universe, see [27]). It has been .... J1 = J2 Myers-Perry is a homogeneously squashed S3.
Goals of this lab ... In this lab you will actually sum up the contributions of B - d]
over such a path around a .... Software (as appropriate) in the Physics folder:.
and then review we current knowledge about magnetic fields in the Galactic disk, the ... Disk field: local structure in the solar vicinity (3 kpc)? .... Our Galaxy.
This thesis deals with the computation of magnetic and magnetostrictive forces, as well as with the magnetoelastic coupling in rotating electrical machines.
Aug 3, 2012 - We model the 3D magnetic field generated by the magnets and derive the ... throughputs in single molecule experimentation based on e.g..
arXiv:cond-mat/0002371v1 [cond-mat.mtrl-sci] 24 Feb 2000. The local magnetic moments and hyperfine magnetic fields in disordered metal-metalloid alloys.
May 14, 2007 - Alexander A Schekochihin1 and Steven C Cowley2. 1 DAMTP ...... Goldstein ML, Roberts DA (1999) Magnetohydrodynamic turbulence in the.
physics 112N. 7 magnetic fields ! a vector at each point in space ! compasses line
up along these vectors ! will produce a force on any moving charge (more later) ...
magnetic fields and forces
physics 112N
bar magnet & iron filings
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bar magnets
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the Earth’s magnetic field
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‘electro’-magnetism ! is there a connection between electricity and magnetism ?
! place a compass near a current carrying wire
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‘electro’-magnetism ! is there a connection between electricity and magnetism ? ! a loop carrying a large current
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magnetic fields ! a vector at each point in space ! compasses line up along these vectors ! will produce a force on any moving charge (more later)
physics 112N
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magnetic fields ! a vector at each point in space ! compasses line up along these vectors ! will produce a force on any moving charge (more later)
physics 112N
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magnetic fields
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magnetic fields ! a vector at each point in space ! compasses line up along these vectors ! will produce a force on any moving charge (more later)
physics 112N
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magnetic fields
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magnetic fields
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magnetic field superposition ! just as the total electric field at any point is the vector sum of the fields from all charges nearby, ! so the total magnetic field is the vector sum of the fields from all magnetic sources nearby. ! Consider two solenoids producing nearly uniform fields:
physics 112N
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magnetic field superposition
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magnetic forces ! magnetic fields produce a force on charged particles that are moving through them ! experiments show that the strength of the force is proportional to · the charge · the speed of the particle · the magnitude of the magnetic field
! experiments also show the direction the force acts in · perpendicular to the velocity · perpendicular to the magnetic field
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magnetic forces - the right-hand rule
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magnetic forces - the right-hand rule
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proton beam through a magnetic field A beam of protons moves through a uniform magnetic field with magnitude 2.0 T, directed along the positive z-axis. The protons have a velocity of magnitude 3.0x105 m/s in the xz-plane at an angle of 30o to the positive z-axis. Find the magnitude and direction of force on the proton.
physics 112N
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motion of charged particles in a magnetic field consider a positive charge moving in a plane perpendicular to a uniform magnetic field force is always perpendicular to the velocity and is of constant magnitude
constant acceleration perpendicular to the velocity circular motion
radius of the circle determined by
physics 112N
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protons in a magnetic field A beam of protons traveling at 1.20 km/s enters a uniform magnetic field traveling perpendicular to the field. The beam exits the magnetic field in a direction perpendicular to its original direction. The beam travels a distance of 1.18 cm in the field. What is the magnitude of the magnetic field ?
physics 112N
proton path
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force on a current carrying conductor ! what happens if we put a wire carrying current into a magnetic field? ! it contains moving charges, so we’d guess it feels a force we can work out a formula for the force: force on each charge in time Δt, a charge Q = I Δt flows in in time Δt, a charge moves so the total charge in the rod is
the total force on the rod is
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force on a current carrying conductor ! if the magnetic field is not perpendicular to the wire, then the formula is modified ! only the perpendicular component of the B-field contributes to the force
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force and torque on a current loop ! what happens if we put a closed current loop into a magnetic field? e.g. consider a rectangular current carrying loop of wire in a uniform field
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force and torque on a current loop ! what happens if we put a closed current loop into a magnetic field? e.g. consider a rectangular current carrying loop of wire in a uniform field
z
x
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force and torque on a current loop ! what happens if we put a closed current loop into a magnetic field? e.g. consider a rectangular current carrying loop of wire in a uniform field
z
x
loop feels a torque
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force and torque on a current loop ! what happens if we put a closed current loop into a magnetic field? e.g. consider a rectangular current carrying loop of wire in a uniform field
z
x
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force and torque on a current loop ! what happens if we put a closed current loop into a magnetic field? e.g. consider a rectangular current carrying loop of wire in a uniform field
z
x
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force and torque on a current loop ! what happens if we put a closed current loop into a magnetic field? e.g. consider a rectangular current carrying loop of wire in a uniform field
N.B. the animation isn’t showing the actual motion caused by the torque, just the variation of force with angle physics 112N
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solenoid in a uniform field ! the torque on the solenoid tends to line it up along the field ! same thing that a bar magnet does
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magnetic field from a long straight wire We now know what happens to moving charges and current carrying wires in magnetic fields ! but how do we generate a magnetic field? ! turns out we can generate magnetic fields using electrical currents ! simplest example is a long, straight current-carrying wire
magnitude of field a perpendicular distance r from a wire carrying current I
permeability of vacuum μ0 = 4!"10-7 Tm/A (magnetic analogue of ε0)
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magnetic field from a long straight wire
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solenoid field strength inside the coil
n = turns per unit length
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typical field strengths typical field strength from a wire 1 cm away from a wire carrying 10 A, B ~ 10-4 T ~ 1 Gauss typical field strength in a solenoid 200 turns in 10cm length carrying 10 A B ~ 10-2 T ~ 10 Gauss a strong fridge magnet
close to the pole, B ~ 10-1 T ~ 100 Gauss
Earth’s magnetic field B ~ 5!10-5 T ~ 0.5 Gauss electromagnet with an iron core B ~ 1 T ~ 104 Gauss superconducting electromagnets (e.g. in the LHC) B ~ 10 T ~ 105 Gauss physics 112N