* Your assessment is very important for improving the workof artificial intelligence, which forms the content of this project
Download PHYS 221 Recitation
Electrical resistance and conductance wikipedia , lookup
Insulator (electricity) wikipedia , lookup
Friction-plate electromagnetic couplings wikipedia , lookup
Magnetic field wikipedia , lookup
Magnetic monopole wikipedia , lookup
History of electromagnetic theory wikipedia , lookup
History of electrochemistry wikipedia , lookup
Multiferroics wikipedia , lookup
Electric machine wikipedia , lookup
Maxwell's equations wikipedia , lookup
Electrostatics wikipedia , lookup
Superconducting magnet wikipedia , lookup
Magnetoreception wikipedia , lookup
Force between magnets wikipedia , lookup
High voltage wikipedia , lookup
Electric current wikipedia , lookup
Electrical injury wikipedia , lookup
Magnetochemistry wikipedia , lookup
Alternating current wikipedia , lookup
Magnetic core wikipedia , lookup
Hall effect wikipedia , lookup
Electromagnetism wikipedia , lookup
Superconductivity wikipedia , lookup
Magnetohydrodynamics wikipedia , lookup
Electricity wikipedia , lookup
Scanning SQUID microscope wikipedia , lookup
Electromagnetic field wikipedia , lookup
Eddy current wikipedia , lookup
Lorentz force wikipedia , lookup
PHYS 221 Recitation Kevin Ralphs Week 6 Overview • • • • • • HW Questions Electromotive Force (EMF) Motional EMF Farraday’s Law Lenz’s Law Inductance HW Questions Ask Away… Electromotive Force (EMF) • What does it tell me? – The change in potential energy per unit charge an object has when moved along a path Δ𝑃𝐸 ℰ≡ 𝑞 – It can also refer to the voltage measured across two terminals • Why do I care? – So far we have considered conservative electric fields which have scalar potentials – For non-conservative fields, the change in potential energy becomes path dependent and EMF is accounting for that Electromotive Force (EMF) • Why do I care? – If a particle is free to move around in space, this is not all that helpful, but when they are constrained to move on a specified path (like an electronic circuit), it becomes well-defined. Note: 1. This is not a force, it has units of volts 2. This is not a potential, the path taken matters very much Motional EMF • When a conductor moves through a magnetic field, it acquires an EMF (this is more along the lines of the two terminal definition) • This happens because a Lorentz force from the magnetic field shuffles charges to opposite ends of the conductor • This sets up a voltage like a parallel plate capacitor bringing the charges into an equilibrium Motional EMF Faraday’s Law • Two earlier approximation schemes – Electrostatics • Stationary charges • Conducting charges at equilibrium 𝐸 ⋅ ∆𝑙 = 0 𝐿𝑜𝑜𝑝 – Magnetostatics • Steady Currents Faraday’s Law • In electrodynamics we allow non-steady currents • This causes time varying magnetic fields bringing Faraday’s law into effect 𝐿𝑜𝑜𝑝 ∆Φ𝐵 𝐸 ⋅ ∆𝑙 = − =Ɛ ∆𝑡 𝜕𝐵 𝛻 × 𝐸=− 𝜕𝑡 Faraday’s Law • What does it tell me? – A changing magnetic field creates a non-conservative electric field – Anything that affects that flux integral induces an EMF in a loop • Why should I care? – Without this law, you could not see, there would be no cell phones or radio: electromagnetic waves exist because of this – Inductors and transformers exploit this phenomenon Lenz’s Law • What does it tell me? – When the flux through a loop changes, a current is produced that fights this change • Why should I care? – This principle is how you determine the direction of an induced current Lenz’s Law • If you are having problems with this, you are not alone – People spend thousands of hours researching this (no kidding) • The idea is to find the direction of the induced magnetic field and use the right hand rule to find the current • To find the direction of the induced field – Note the direction of the original field through the loop – Determine whether this field is getting stronger or weaker – The direction of the induced field will maintain the status quo Inductance • What does it tell me? – The flux through a loop depends linearly on the currents through conductors in the vicinity (including itself) Φ𝑀 = 𝐿𝐼 + 𝑀𝑖 𝐼𝑖 – This is a direct consequence of the principle of superposition and magnetic fields being proportional to the currents that create them Inductance • Why should I care? – This is the sister component to the capacitor making it one of the most fundamental electronic components Capacitor Inductor Depends on geometry and material between the plates Depends on geometry and material in intervening space Proportionality between charge and voltage Proportionality between flux and current Stores energy in an electric field Stores energy in a magnetic field Causes current to lag voltage Causes current to lead voltage 𝑄 𝐶 Current starts at maximum and drops to zero 𝑑𝐼 𝑑𝑡 Current starts at zero and increases to maximum 𝑉= 𝑉=𝐿