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Eventually transatlantic signals! From Last Time… • Electromagnetic waves Capacitor banks Induction coils • Charges, current and forces: Coulomb’s law. Spark gap • Accelerating charges produce an electromagnetic wave • The idea of the electric field. Today… Electric fields, magnetic fields, and their unification Mon. Feb 20, 2006 Gulgielmo Marconi’s transatlantic transmitter Phy107 Lecture 14 1 Mon. Feb 20, 2006 Electromagnetic Waves Phy107 Lecture 14 2 The idea of electric fields y z x • EM wave made up of oscillating electric and magnetic fields. • But what is an electric field? • Electric and magnetic fields are perpendicular to propagation direction • Electric field is a way to describe the force on a charged particle due to other charges around it. • Can travel in empty space • Force = charge × electric field f = v/λ • The direction of the force is the direction of the electric field. • A Transverse wave. v = c = 3 x 108 m/s (186,000 miles/second!) Mon. Feb 20, 2006 Phy107 Lecture 14 3 Mon. Feb 20, 2006 Question Phy107 Lecture 14 4 The electric field Force on this charge… • Direction of force between two particles of the same charge (use next slide). Q2 + + F=k + Q1Q2 r2 Q1 …due to this charge ! Force = (Charge) " (Electric field) + + ! Mon. Feb 20, 2006 Phy107 Lecture 14 5 Mon. Feb 20, 2006 Phy107 Lecture 14 6 1 Visualizing the electric field Why bother? • Faraday invented the idea of field lines following the force to visualize the electric field. • Why invent fields - why not just use forces? Local electric field is same direction as field lines. Force is parallel or antiparallel to field lines. Charged particle will move along these field lines. • Think of the EM wave. A spark is an accelerating current flow, producing the wave. • The wave continues to propagate even when the spark is gone. • No charges anywhere, but time-varying fields propagate as a wave. Field lines emanate from positive charge and terminate on negative charge. Mon. Feb 20, 2006 Phy107 Lecture 14 7 Electric field: summary Mon. Feb 20, 2006 Phy107 Lecture 14 8 But wait… there’s more • Energy can be stored in the field. • Presence of electric field means that there will be a force on a charged particle. • Energy density proportional to • This force ( and electric field) can arise from electric charges (via Coulomb’s law) (Electric field)2 (Magnetic field)2 • Electromagnetic forces aren’t felt instantaneously, the propagate at speed of electromagnetic wave (speed of light) • Is a way to determine forces on a charged particle without thinking about the charges that give rise to the forces. • Object transfers momentum to the field, which later transfers it to another object. Mon. Feb 20, 2006 Phy107 Lecture 14 9 Mon. Feb 20, 2006 Phy107 Lecture 14 10 Magnetism: Permanent magnets Magnetic forces • Clearly magnets interact with each other Opposites attract • North Pole and South Pole • Sometimes attracting, sometimes repelling N • This is the elementary magnetic particle N • Visualized as a bar with positive pole (North) at one end and negative pole (South) at other. • Called magnetic dipole (North pole and South pole) S • These ‘magnetic charges’ cannot be broken apart — always appear in N-S pairs. • Poles interact with each other similar to charges. • But the magnetic particles are sort of a ‘composite’ positive and negative ‘magnetic charge’. S Mon. Feb 20, 2006 S N S S N N Phy107 Lecture 14 11 Mon. Feb 20, 2006 Likes repel Phy107 Lecture 14 12 2 Magnetic field Field lines of a magnet • Similar in spirit to electric field • Used to determine the ‘orientational’ force on a magnetic dipole: – Magnetic field exerts a force on a dipole that aligns it with magnetic field lines. – Uniform magnetic field only rotates dipole: doesn’t cause it to move. • Static magnetic field arises from permanent magnets (or currents). • Field lines indicate direction of field • Density indicates strength of field • Similar to electrostatic force, but force is felt by magnetic dipole • But, as electric field, can exist in an EM wave even without magnetic dipoles. Mon. Feb 20, 2006 Phy107 Lecture 14 13 Mon. Feb 20, 2006 Surprise! The Earth is a magnet! Earth is a magnetic dipole. Phy107 Lecture 14 14 Electric current produces magnetic field • Current (flow of electric charges ) in wire produces magnetic field. • That magnetic field aligns compass needle North magnetic pole ~ at south geographic pole Current A compass is a magnetic dipole Magnetic field Compass needle aligns with local Earth field Mon. Feb 20, 2006 Phy107 Lecture 14 15 Magnetic field from a current Mon. Feb 20, 2006 Phy107 Lecture 14 16 Forces between currents • Which of these pairs of currents will attract each other? A. A B. A & C C. B Iron filings align with magnetic field lines Mon. Feb 20, 2006 A Magnetic field loops around the current. Phy107 Lecture 14 17 Mon. Feb 20, 2006 B Phy107 Lecture 14 C 18 3 Magnetic field from a current loop Solenoid electromagnet • One loop: field still loops around the wire. • Sequence of current loops can produce strong magnetic fields. • This is an electromagnet • Many loops: same effect Mon. Feb 20, 2006 Phy107 Lecture 14 Mon. Feb 20, 2006 19 Phy107 Lecture 14 Magnetic Field Ranges Superconducting Magnets Field Size • Solenoid as in conventional electromagnet. • But once current is injected, power supply turned off, current and magnetic field stays forever… …as long as T < Tc Example Phy107 Lecture 14 0.2 T 0.01 T 33 T 0.0001 T 2T 21 0.00003 T 3x10-10 T Mon. Feb 20, 2006 Phy107 Lecture 14 22 Large scale applications • Magnetic Resonance Imaging typically done at 1.5 T • Superconducting magnet to provides static magnetic field • Spatial resolution of positions of tracer atomic nuclei. Phy107 Lecture 14 Example 60 T Magnets for MRI Mon. Feb 20, 2006 Field Size 0.4 T 850 T 0.5 T Mon. Feb 20, 2006 20 Superconducting magnet Plasma confinement torus Proposed ITER fusion test reactor 23 Mon. Feb 20, 2006 Phy107 Lecture 14 24 4 Faraday’s law of induction Time-varying magnetic field • Up to this point, electric and magnetic fields constant in time Faraday’s law: – time-varying magnetic field produces electric field • Constant electric current produces constant magnetic field. – Strength of electric field proportional to how fast magnetic field changes. • Constant magnetic field produces… nothing in particular! In this experiment: • Magnetic field is largest close to the bar magnet, drops off farther away. • But changing the magnetic field in time produces… an electric field! • Moving magnet toward coil causes magnetic field through coil to increase with time, producing electric field • This effect is called induction. Mon. Feb 20, 2006 Phy107 Lecture 14 • Since coil is conducting, this electric field produces a current in the wire of the coil and through the meter. 25 Mon. Feb 20, 2006 One step further: Lenz’s law • This induced current produces a magnetic field, which interacts with the bar magnet just as another bar magnet would. • Lenz’s law describes the direction of the induced field (or equivalently, the direction of the induced currents) – The induced current circulates in such a way as to generate a magnetic field that tends to cancel the change in the field. Phy107 Lecture 14 26 Time-varying electric field • Can also produce a time-varying magnetic field with a time-varying current in an electromagnet. • Faraday’s law: time-varying magnetic field produces electric field, electric field produces electric current (in a metal). • Just as before, the current is induced in such a way that the resulting magnetic dipole repels the changing flux that produced the current. – Causes repulsive force on original moving bar magnet. • This is the principle of an electromagnetic ‘gun’. Mon. Feb 20, 2006 Phy107 Lecture 14 27 Mon. Feb 20, 2006 Maxwell’s unification Phy107 Lecture 14 28 Electromagnetic Waves • Intimate connection between electricity and magnetism Current (up and down) creates electromagnetic wave consisting of oscillating electric and magnetic fields • Time-varying magnetic field induces an electric field (Faraday’s Law) • Time-varying electric field generates a r magnetic field r r 1 %B "#E =$ c %t r In vacuum: r r 1 %E "#B= c %t + This is the basis of Maxwell’s unification of electricity and magnetism into Electromagnetism - ! Mon. Feb 20, 2006 Phy107 Lecture 14 29 Mon. Feb 20, 2006 Phy107 Lecture 14 30 5 Electromagnetic Waves y z x • A Transverse wave. • Electric and magnetic fields are perpendicular to propagation direction • Can travel in empty space f = v/λ v = c = 3 x 108 m/s (186,000 miles/second!) Mon. Feb 20, 2006 Phy107 Lecture 14 31 6