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I V Experiment No. 7 EE 312 Basic Electronics Instrumentation Laboratory Wednesday, October 11, 2000
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Objectives: Measure dynamic impedance of a forward-biased diode & Zener diode Learn about small-signal techniques Learn about interference reduction through the use of proper grounding and twisted-pair techniques
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Background: What is dynamic impedance ? R= V I r d = dV d I dynamic resistance resistance
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V-I Characteristics V I R V I V I V I V I slope rdrd dV dI R= VIVI diode transistor Tube Operating Point
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iDiD vDvD slope di D /dv D di D r d = dvDdvD = VDVD iDiD = VdVd IdId IdId VdVd
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I D dc diode current I d ac amplitude i d ac diode current i D total diode current ~ + - dc circuitac circuit IDID idid iDiD idid iDiD IDID IdId X d or D IEEE Standard Notation
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V D dc diode voltage V d ac amplitude v d ac diode voltage v D total diode voltage vdvd vDvD VDVD VdVd ~ + - dc circuitac circuit VDVD vdvd vDvD
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I D, V D I d, V d Small-Signal Condition
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Dynamic Resistance Measurement iDiD vDvD IDID VDVD 2I d 2V d r d = V d I d
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iDiD vDvD IDID VDVD Input Signal Too Large
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iDiD vDvD IDID VDVD Input Signal Too Small noise
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Measurement of r d looks simple. The problem is that v d in the millivolt range for forward bias. Thus, noise and stray pickup may cause trouble if you are not careful.
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Example: Questions: Where does come from ? ! AB Oscilloscope R idid Stray magnetic flux How large is it ?
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Questions: Where does come from ? Answer: 1. Current i ac in power lines on bench & drops from ceiling 2. fluorescent lights 3. AC machines r
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Question: How large is ? rr I
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AB Oscilloscope R 1 meter Area=1 m 2 Assume our experiment is about 2 meters from the power lines: r = 2 m 100 amp. peak60 HZ Peak value is 3.77 mV and this may be comparable to signal amplitudes being measured!
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~ + - Must be concerned about in all parts of circuit.
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How is this problem avoided? remember We have control over A. We can‘t do much about r or I. So, we must minimize A. OSC. Step 1: Make the area smallStep 2: Twist wires together OSC.
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Twisting wires does two things, 1- Holds wires together 2- voltages induced in adjacent sections cancel V1V2 1 2 V 1~ -V 2 So induced signals cancel
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AB Oscilloscope R Keep track of grounded leads
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Single Point Grounding Use Only One Ground Connection Such As CRO ground
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Can only one ground connection be realized? e. g. CRO ground. Not with BNC’s because the each outer connector is another ground.
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Capacitive Coupling 1. Assume 1 pF between your circuit and 120 VAC power lines. 2. 60-Hz current I = j CV where = 377 rad/s at f = 60 Hz, C = 1 pF, and V = 120 VAC(rms)
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3. The voltage produced by I = ZxI where Z is the impedance I flows through. 4. Example: CRO Z = 1 Meg V CRO = 377x1pFx120Vx1Meg = 45 mV(rms) = 130 mVpp
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Procedures: I-Measure dynamic resistance of a Zener diode in the forward bias region. II- Simulation for Part I. (In Bell 242) III- Measure dynamic resistance in the Zener breakdown region.
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Components: Zener Diode 1N4742-12VDC-0.5 W 2 Heathkit Resistance Substitution Boxes 1-kohm & 10 kohm Resistors Decade Capacitor Box
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1- Dynamic Resistance in Forward Region ~ CH. 1CH. 2 + - A 0-20V R1R2 dc circuitac circuit IDID idid C v D, i D
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~ + - A ~10.4V to ~10.8V R1 dc circuit IDID The values of R1 and the voltage source are selected to control the dc bias current I D. Suppose we want I D = 10 mA. Make the dc voltage across R1 = ~10 VDC. Assume V D = 0.7 V. V=10.7 volts & I D =10 mAR1=1000 Ohms ~0.4 to 0.8V ~10 VDC
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~ + - A R2 ac circuit idid C R2 is selected so that ac current peak is ~10% of dc current. R1=1000 OhmsR2=10,000 By setting the dc power supply voltage to ~10.7 VDC & the FG amplitude to ~20 Vpp and R2 to ~10R1, the ac current peak is ~10% of dc current. I. E. I D =10 mA & i d =1 mA. To obtain other values of I D & i d change both R1 & R2 with R2/R1 = ~10. The dc & ac voltage levels in the circuit change very little as R1 & R2 are changed to change the currents I D & i d. ~10.7V ~20Vpp 1 kHz R1
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~ + - A R2 ac circuit idid C R2 is selected so that ac current peak is ~10% of dc current. R1=1000 OhmsR2=10,000 C blocks dc current in the ac circuit & C should be large enough so that capacitance reactance is small compared with R2 Note that R1 must be >> diode dynamic resistance so that most of the ac current goes through the diode & not the dc circuit ~10.7V ~20Vpp 1 kHz
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Selection of R2 The values of R2 and the function generator voltage amplitude V gen should be chosen to make the ac current amplitude i d 10% to 20 % of I D. The corresponding diode peak ac voltage V d will be 10% V to 20 % of nV T where V T = 25 mV at T = 290 K. (~20 C). Thus V d will be 2.5 to 5 mV for n = 1 and the peak-to-peak diode ac voltage will be 5 to 10 mV.
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Fall 2000 Data Table For Forward r d
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n=1 to 2 rtheoretical ?
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1/T d(lnI D ) dV D slope gives n n?
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Examples: I D = 0.2 mA n = 1 r d = 1X25mV /0.2mA = 125 n = 2 r d = 2X25mV/0.2mA = 250
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2- Simulation a- Simulate Part 1 of experiment b- Plot I(D1) and V(2) on separate graphs c- Calculate dynamic impedance of the diode ~ + - 0-20V R1R2 C 0 1 234 D1
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DYNAMIC IMPEDANCE I1 0 1 PWL(0.5M.00249.5M.0025 1M.00499 1M.005 5M.00749 5M.0075 10M) R1 1 2 1.5K D1 2 0 DIODE.MODEL DIODE D((RS=2 IS=2E-9 N=1.8) R2 3 2 15K C1 4 3.22U V1 4 0 SIN(0 5 1KHZ).TRAN.05M 10M 0.05M.PRINT TRAN V(2) i(D1).END ~ + - 0-20V R1R2 C 0 1 234 D1 time [s] [mA]
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3- Dynamic Resistance of Zener in the Breakdown Region ~ CH. 1CH. 2 + - A 0-20V R1R2 dc circuitac circuit IDID idid C v D, i D Choose values of dc bias current so that the dc power dissipation in the diode is less than 1/2 of its max rated power dissipation (1/2 Watt).
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Assume Zener Diode Breakdown Voltage V Z = 12V The values of R1 and the dc voltage source are selected to control the dc bias current I D. Suppose we want I D = 10 mA. Make the dc voltage across R1 = ~5 VDC. Then R1 = ~5 VDC/10mA = 0.5 k . Use the closest value which is 470 . The FG peak voltage is set at 10 V. The value of R2 is selected so that the peak ac current = 10% of the dc current = 0.1 X 10 mA. Thus R2 = ~10V/1mA = 10 k .
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