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Published byNickolas Grant Modified over 9 years ago
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p212c31: 1 Chapter31: Inductance Currents create magnetic fields Changing currents create changing magnetic fields Changing magnetic fields induce EMF’s Circuit elements interact magnetically!
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p212c31: 2 Mutual Inductance Magnetic Interaction between two circuits i1i1 B2B2
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p212c31: 3 Mutual Inductance: Units [M] = [ ]/[I]=(T m 2 )/(A) = Henry (H) Depends upon Geometry (Magnetic) material properties
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p212c31: 4 Example: Long Solenoid with Length l, area A and N 1 turns surrounded by a coil with N 2 turns. A
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p212c31: 5 Self Inductance Circuit elements of same circuit link magnetically B I
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p212c31: 6 Example: Solenoid from previous example
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p212c31: 7 Inductors Schematic symbol Induced EMF (Lenz’s Law) Switch closes, current increases Inductor opposes increase opposes battery. Steady current (i constant) no EMF. i
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p212c31: 8 Magnetic Field Energy Energy stored in an inductor I
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p212c31: 9 Energy stored in a magnetic field Uniform Magnetic field energy is distributed uniformly
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p212c31: 10 Example: How big an inductor would be required to store 150kWh of energy using a coil carrying 200 A? Example: What is the energy density associated with the design field strength produced by the magnets for the ill fated SSC?
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p212c31: 11 a b a b i i increasing a b i decreasing Potential differences across inductors in circuits V ab depends upon rate of change of current
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p212c31: 12 Homework: How do inductors combine in circuits? -in series? Hints: currents are the same, EMF’s add -in parallel? Hints: EMF’s are the same, currents add Look at derivation for resistors!
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p212c31: 13 The R-L Circuit i E L R
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p212c31: 14 i E /R t =
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p212c31: 15 i E L R
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p212c31: 16 i IoIo t =
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p212c31: 17 The L-C Circuit i L qq q
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p212c31: 18
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p212c31: 19 Q t q QQ i t
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p212c31: 20 The L-R-C Circuit i L qq q C R
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p212c31: 21
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p212c31: 23 The Driven L-R-C Circuit i L qq q C R v(t)= Vcos( t)
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p212c31: 24
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p212c31: 25 Q/Q resonance o
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