Electronic Devices and Circuit Theory

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Presentation transcript:

Electronic Devices and Circuit Theory Boylestad Diode Applications Chapter 2

Load-Line Analysis Ch.2 Summary The load line plots all possible combinations of diode current (ID) and voltage (VD) for a given circuit. The maximum ID equals E/R, and the maximum VD equals E. The point where the load line and the characteristic curve intersect is the Q-point, which identifies ID and VD for a particular diode in a given circuit.

Series Diode Configurations Ch.2 Summary Series Diode Configurations Forward Bias Constants Silicon Diode: VD = 0.7 V Germanium Diode: VD = 0.3 V Analysis (for silicon) VD = 0.7 V (or VD = E if E < 0.7 V) VR = E – VD ID = IR = IT = VR / R

Series Diode Configurations Ch.2 Summary Series Diode Configurations Reverse Bias Diodes ideally behave as open circuits Analysis VD = E VR = 0 V ID = 0 A

Parallel Diode Configurations Ch.2 Summary Parallel Diode Configurations

Half-Wave Rectification Ch.2 Summary Half-Wave Rectification The diode conducts only when it is forward biased, therefore only half of the AC cycle passes through the diode to the output. The DC output voltage is 0.318Vm, where Vm = the peak AC voltage.

PIV (PRV) Ch.2 Summary PIV (or PRV) > Vm Because the diode is only forward biased for one-half of the AC cycle, it is also reverse biased for one-half cycle. It is important that the reverse breakdown voltage rating of the diode be high enough to withstand the peak, reverse-biasing AC voltage. PIV (or PRV) > Vm Where PIV = Peak inverse voltage PRV = Peak reverse voltage Vm = Peak AC voltage

Full-Wave Rectification Ch.2 Summary Full-Wave Rectification The rectification process can be improved by using a full-wave rectifier circuit. Full-wave rectification produces a greater DC output: Half-wave: Vdc = 0.318Vm Full-wave: Vdc = 0.636Vm

Full-Wave Rectification Ch.2 Summary Full-Wave Rectification Bridge Rectifier A full-wave rectifier with four diodes that are connected in a bridge configuration VDC = 0.636Vm

Full-Wave Rectification Ch.2 Summary Full-Wave Rectification Center-Tapped Transformer Rectifier Requires two diodes and a center-tapped transformer VDC = 0.636Vm

Summary of Rectifier Circuits Ch.2 Summary Summary of Rectifier Circuits In the center tapped transformer rectifier circuit, the peak AC voltage is the transformer secondary voltage to the tap. Rectifier Ideal VDC Realistic VDC Half Wave Rectifier VDC= 0.318Vm VDC = 0.318Vm – 0.7 Bridge Rectifier VDC = 0.636Vm VDC = 0.636Vm – 2(0.7 V) Center-Tapped Transformer Rectifier VDC = 0.636Vm – 0.7 V Vm = the peak AC voltage

Diode Clippers Ch.2 Summary The diode in a series clipper “clips” any voltage that does not forward bias it: A reverse-biasing polarity A forward-biasing polarity less than 0.7 V (for a silicon diode)

Biased Clippers Ch.2 Summary Adding a DC source in series with the clipping diode changes the effective forward bias of the diode.

Parallel Clippers Ch.2 Summary The diode in a parallel clipper circuit “clips” any voltage that forward biases it. DC biasing can be added in series with the diode to change the clipping level.

Summary of Clipper Circuits Ch.2 Summary Summary of Clipper Circuits

Summary of Clipper Circuits Ch.2 Summary Summary of Clipper Circuits

Summary of Clipper Circuits Ch.2 Summary Summary of Clipper Circuits

Ch.2 Summary Clampers A diode and capacitor can be combined to “clamp” an AC signal to a specific DC level.

Biased Clamper Circuits Ch.2 Summary Biased Clamper Circuits The input signal can be any type of waveform such as a sine, square, or triangle wave. The DC source lets you adjust the DC camping level.

Summary of Clamper Circuits Ch.2 Summary Summary of Clamper Circuits

Zener Diodes Ch.2 Summary The Zener is a diode that is operated in reverse bias at the Zener Voltage (Vz). When Vi  VZ The Zener is on Voltage across the Zener is VZ Zener current: IZ = IR – IRL The Zener Power: PZ = VZIZ When Vi < VZ The Zener is off The Zener acts as an open circuit

Zener Resistor Values Ch.2 Summary If R is too large, the Zener diode cannot conduct because IZ < IZK. The minimum current is given by: The maximum value of resistance is: If R is too small, IZ > IZM . The maximum allowable current for the circuit is given by: The minimum value of resistance is:

Voltage-Multiplier Circuits Ch.2 Summary Voltage-Multiplier Circuits Voltage multiplier circuits use a combination of diodes and capacitors to step up the output voltage of rectifier circuits. Three common voltage multipliers are the: Voltage Doubler Voltage Tripler Voltage Quadrupler

Voltage Doubler Ch.2 Summary This half-wave voltage doubler’s output can be calculated using: Vout = VC2 = 2Vm where Vm = peak secondary voltage of the transformer

Voltage Doubler Ch.2 Summary Positive Half-Cycle Negative Half-Cycle D1 conducts D2 is switched off Capacitor C1 charges to Vm Negative Half-Cycle D1 is switched off D2 conducts Capacitor C2 charges to Vm Vout = VC2 = 2Vm

Voltage Tripler and Quadrupler Ch.2 Summary Voltage Tripler and Quadrupler

Practical Applications Ch.2 Summary Practical Applications Rectifier Circuits Conversions of AC to DC for DC operated circuits Battery Charging Circuits Simple Diode Circuits Protective Circuits against Overcurrent Polarity Reversal Currents caused by an inductive kick in a relay circuit Zener Circuits Overvoltage Protection Setting Reference Voltages