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Analog Circuits Seth Price Department of Chemical Engineering New Mexico Tech Rev. 1/13/16
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Ohm’s Law E = IR – E is the voltage across a component – I is the current through a component – R is the resistance of the component
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Resistor Color Code
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Series/ Parallel Combinations Series: the same current passed through multiple components Req = R1 + R2 + … Parallel: the same voltage is across multiple components 1/Req = 1/R1 + 1/R2 + ….
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Kirchoff’s Current Law (KCL) Any current flowing into a node must also leave the node: – The sum of all currents = 0 – Think “conservation of mass”
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Kirchoff’s Voltage Law (KVL) The sum of the voltages around any closed loop must equal zero – Any voltage generated must be dissipated – Think “conservation of mass”
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Using a Multimeter Measure voltage in parallel – Meter tries to have infinite impedance Measure current in series – Meter tries to have no impedance 3 Point Safety Check – Measure known voltage (ex wall outlet) – Measure voltage on what you think has no power – Measure known voltage again
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Current Limiter All devices have a maximum allowable current A resistor in series drops current in loop http://tinkerlog.com/2009/04/05/driving-an-led-with-or-without-a-resistor/
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Shunt Resistor High currents are hard to measure Instead, place a small resistance (of known value) in series Measure voltage drop across resistor From Ohm’s law: I= V/R http://www.reuk.co.uk/What-is-a-Shunt.htm
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Wheatstone Bridge Easy to detect small voltages R1, R2 and R3 are known Rx is adjustable – Perhaps a sensor As Rx changes, the current from A->C changes, Vg changes http://en.wikipedia.org/wiki/Wheatstone_bridge
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Diodes (PN Junction) Diodes conduct in only one direction Semiconducting device Resistance is non-linear Require a “knee” or “turn-on” voltage – Silicon: 0.6-0.7V – Germanium: 0.3V – LED: 1.7V
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Diode Vs. Sine Wave http://www.duncansonelectric.com/blog/wp- content/uploads/2009/08/23-half-wave-rectifier-1024x368.gif
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IV Curve for Diodes https://learn.sparkfun.com/tutorials/diodes/real-diode-characteristics
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Capacitors Store energy in an electric field Measured in Farads (F) Two physical configurations – Parallel plates – Concentric cylinders
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Capacitor Combinations Series Combination: 1/C eq = 1/C 1 + 1/C 2 + … + 1/C n Parallel Combination: C eq = C 1 + C 2 + … + C n
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Capacitor Voltage Vc(t): Voltage across capacitor at any time Vs: Source voltage T: Time constant t: elapsed time V c(t) = V s (1-e -t/T )
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Inductors Store energy in a magnetic field Measured in Henries (H) Typically a coil of wire Adjustable inductor: slug
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Inductor Combinations Series Combinations L eq = L 1 + L 2 + … + L n Parallel Combinations 1/L eq = 1/L 1 + 1/L 2 + … + 1/L n
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Inductor Voltage V(t): Voltage across Inductor as a function of time L: inductance in Henries di/dt: change in current with respect to time V(t) = -L * di/dt
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Time Constants Time Constant (T): way to characterize time to charge/discharge a capacitor or inductor 1*T: 63% of the maximum charge 5*T: fully charged For a capacitor: T = R*C For an inductor: T = L/R
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Solenoids Changing current induces magnetic field Magnetic field moves plunger Used in starter motors, valves, latches, etc.
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Solenoid Valve
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Transformers Two adjacent inductors that can influence each other Can add an iron core to transformer to increase magnetic field No electron travels between inductors – Isolation Transformer
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Putting it all together… DC Power Supply
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