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EEE 205 / ECE 202 Electronic Devices and Circuits Fall 2010 Lecture 5: Zener Diodes
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2 Diode Applications – Rectifier Circuits Block diagram of a DC power supply. One of the most important applications of diodes is in the design of rectifier circuits. Rectifier circuits can be classified in two groups: 1. Half-wave (HW) rectifier 2. Full-wave (FW) rectifier
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3 Zener Diodes FIGURE 3-1 Zener diode symbol. IZIZ VZVZ + -
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4 Zener Diodes Zener Diode Characteristics Unlike ordinary diodes, zener diodes are used in the reversed biased mode, in the breakdown region. Zener diodes can maintain a constant voltage across its terminal despite large variations in the zener current. Therefore, they are used to get reasonably regulated dc voltage when the input voltage and load resistance vary.
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5 Zener Diodes General diode I-V characteristic
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6 Zener Diodes The application of too negative a voltage across the zener diode results in a sharp change in the I-V characteristics. The current increases at a very rapid rate in a direction opposite to that of the positive voltage region. The reverse-bias potential that results in this dramatic change in characteristics is called the Zener potential or the Zener voltage and is given the symbol V Z. As the voltage across the diode increases in the reverse-bias region, the velocity of the minority carriers responsible for the reverse saturation current I s also increases. Zener Diode Characteristics
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7 Zener Diodes 1.Avalanche Breakdown 2.Zener Breakdown 1. Avalanche Breakdown As the voltage across the diode increases in the reverse-bias region, the velocity of the minority carriers responsible for the reverse saturation current Is also increases. Eventually, their velocity and associated kinetic energy will be sufficient to release additional carriers through collisions with otherwise stable atomic structures. That is, an ionization process will result whereby valence electrons absorb sufficient energy to leave the parent atom. These additional carriers can then aid further ionization to the point where a high avalanche current is established and the avalanche breakdown region determined. Diode Breakdown Mechanism
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8 Zener Diodes 2. Zener Breakdown The avalanche region (V Z ) can be brought closer to the vertical axis by increasing the doping levels in the p- and n-type materials. However, as V Z decreases to very low levels, such as 5 V, another mechanism, called Zener breakdown, will contribute to the sharp change in the characteristic. It occurs because there is a strong electric field in the region of the junction that can disrupt the bonding forces within the atom and “generate” carriers. Although the Zener breakdown mechanism is a significant contributor only at lower levels of V Z, this sharp change in the characteristic at any level is called the Zener region and diodes employing this unique portion of the characteristic of a p- n junction are called Zener diodes. Diode Breakdown Mechanism
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9 Zener Diodes Ideal Zener Diode model VzVz
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10 Zener Diodes IV Characteristics: Zener Diode Voltages V ZK, I ZK – Zener knee voltage and current, zener just turns on V Z – Nominal zener voltage at zener test current I ZT, the diode should be operated around this point V Z0 – Intersect of the slope at the operating point Q r z – Resistance of the zener diode at point Q V = I.r z – Change in the diode voltage due to change in the current
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11 Zener Diodes Practical Zener Diode Model V Z0
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12 Zener Diodes Practical Zener Diode Model
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13 Zener Diodes Q IV Characteristics: Zener Diode Currents
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14 Zener Diodes Analysis of Zener Diode Circuits: Line Regulation Analysis of Zener Diode Circuits: Line Regulation Line regulation, V 0 / V IN (mV/V), is a measure of fluctuation in the output voltage due to variation in the supply voltage.
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15 Zener Diodes Analysis of Zener Diode Circuits: Load Regulation Analysis of Zener Diode Circuits: Load Regulation Load regulation, V 0 / I L (mV/mA), is a measure of fluctuation in the output voltage due to variation in the load current.
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16 Exercise Zener Diodes V Z =6.8V, I Z =5 mA, r z = 20 ohm, I ZK =0.2 mA. The nominal supply voltage V + = 10 V, and can vary by ±1 V. a. Find V 0 with no load and V + at its nominal value. b. Find the change in V 0 resulting from the ±1V change in V +. (Line regulation) c. Find the change in V 0 resulting from connecting a load resistance R L that draws a current I L =1mA. Find load regulation. d. Find V 0 when R L =2 K ohm. Find change in V 0. e. Find V 0 when R L =0.5 Kohm. f. What is the minimum value of R L for which the diode still operates in the breakdown region?
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