Chapter 30 Inductors and self Inductance - UCSB...•Basically a mutual inductance device between...
Transcript of Chapter 30 Inductors and self Inductance - UCSB...•Basically a mutual inductance device between...
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Chapter 30 – Inductors and self Inductance
Inductance is to Capacitance what current is to a stationary charge. They are both defined
relative to the voltage produced.
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Goals for Chapter 30
• Mutual inductance
• Self-inductance
• Magnetic-field energy
• R-L circuits
• L-C circuits
• L-R-C circuits
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Introduction
–A charged coil can create a
field that will induce a
current in a neighboring
coil.
– Inductance can allow a
sensor to trigger the traffic
light to change when the car
arrives at an intersection..
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Mutual inductance– A coil in one device
generates a field that
creates a current in a
neighboring coil. This
is the basis for a
transformer.
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Mutual inductance—examples– Two solenoid coil one with N1
turns and the other with N2 turns
– How do they interact?
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Self and Mutual Inductance
• We define inductance L as magnetic flux/current
• Here N is the number of coil turns
• In multiple coil systems there is magnetic coupling between the coils – hence Mutual inductance M
• Here L12 = L21 = M
• Energy stored in multiple coils
.
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EMF and Flux change
• The time derivative of the magnetic flux = EMF
• In general dL/dt = 0 (the inductance does not change) – This is NOT always true – rail gun example
• If L = constant then:
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Energy in inductors
• We can related the power (I*V) to inductance and current change
• Hence we can equate WL = energy = ½ L I2
• Note the similarity to energy in a capacitor
• WC = ½ C V2
• Where does the energy reside?
• In the magnetic and electric fields
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Mutual Inductance and Self Inductance
• k is the coupling coefficient and 0 ≤ k ≤ 1,
• L1 is the inductance of the first coil
• L2 is the inductance of the second coil.
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Induced voltage with self and mutual inductance
• V1 is the voltage across the inductor of interest
• L1 is the inductance of the inductor of interest
• dI1 / dt is through the inductor of interest
• dI2 / dt is through the inductor that is coupled to the first inductor
• M is the mutual inductance.
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Transformers – Voltage Ratios• Basically a mutual inductance device between two
inductors – primary and secondary
• Vs is the voltage across the secondary inductor
• Vp is the voltage across the primary inductor (the one connected to a power source)
• Ns is the number of turns in the secondary inductor
• Np is the number of turns in the primary inductor.
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Transformers – Current Ratios
• Is is the current through the secondary inductor
• Ip is the current through the primary inductor (the one connected to a power source)
• Ns is the number of turns in the secondary inductor
• Np is the number of turns in the primary inductor
• Note – Power IP VP = IS VS is conserved in an IDEAL transformer
• In real transformers there is loss - heat
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Self-inductance
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Applications and calculations
• There are many cases where self and mutual inductance are important.
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Magnetic field energy
• Your car uses the collapse of the magnetic field in a transformer to create the spark in your sparkplug.
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The R-L circuit
• The LR circuit is like the RC circuit from capacitance. In a capacitor energy was stored in the electric field. In an inductor energy is stored in the magnetic field.
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R-L circuit II
• LR and RC circuits both have a time constant. For RC = RC for LR = L/R
• Recall reactance for a capacitor and inductor are:
• ZC = 1/ i C
• ZL = i L
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The L-C circuit
• Electric and magnetic field energy transfer
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Applications and comparisons
•
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The L-R-C circuit - Dissipation
• In an ideal L-R-C circuit the only dissipation is through the resistor. The L and C have no dissipation and are lossless. The resistor converts the electrical energy into heat. Thus decay of voltage and current.