Rectifier Diodes - Notes for Pre Lab 4 | ECE 3254, Lab Reports of Electrical and Electronics Engineering

Material Type: Lab; Class: Industrial Electronics; Subject: Electrical & Computer Engineer; University: Virginia Polytechnic Institute And State University; Term: Unknown 1989;

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ECE 3254 PreLab 4 notes
Edited 01-19-07
Rectifier Diode – may also be called a switching diode for high frequency use.
The ideal rectifier diode operates as a one-way check valve or switch. Conduction occurs only when the
diode is forward biased. The ideal diode has no forward voltage drop and does not conduct at all when
reverse biased.
A real diode has a typical forward voltage of 0.6V to 0.8V, and a reverse breakdown voltage that is
greater than the diode’s peak inverse voltage (PIV) rating. Conduction in both directions follows an
exponential V-I curve. The diode current I is given by Equation 1 where IS is a scale factor called the
saturation current, q is the charge on an electron , k is Boltzmann's constant, T is the absolute
temperature of the p-n junction and VD is the voltage across the diode. The term kT/q is the thermal
voltage, sometimes written VT, and is approximately 26 mV at room temperature. n is the emission
coefficient, which is typically 1 for most devices.
Equation 1: Silicone saturation current IS ≈ 10-13A
Germanium saturation current IS ≈ 10-8A
Rectifier diode ratings include:
Forward current
PIV
Forward voltage drop
Reverse recovery time
Junction Capacitance
Rectifier diodes are normally only operated in forward condition, forward cutoff, or reverse cutoff. The
PIV rating is not an indication of where reverse conduction actually occurs; it only guarantees that the
diode will not break down before the PIV rating is reached. It is not a good idea to design a circuit that
depends on reverse conduction in a rectifier diode because the reverse conduction voltage can not be
predicted. Because uncontrolled reverse breakdown quickly leads to diode failure, (which can also
damage other circuit components) you should never attempt to operate a rectifier diode in reverse
conduction.
The diode Cathode is identified by a band
on the cathode end.
Prelab 4 Notes - Page 1 of 3
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ECE 3254 PreLab 4 notes

Edited 01-19-

Rectifier Diode – may also be called a switching diode for high frequency use.

The ideal rectifier diode operates as a one-way check valve or switch. Conduction occurs only when the diode is forward biased. The ideal diode has no forward voltage drop and does not conduct at all when reverse biased. A real diode has a typical forward voltage of 0.6V to 0.8V, and a reverse breakdown voltage that is greater than the diode’s peak inverse voltage (PIV) rating. Conduction in both directions follows an exponential V-I curve. The diode current I is given by Equation 1 where IS is a scale factor called the saturation current, q is the charge on an electron , k is Boltzmann's constant, T is the absolute temperature of the p-n junction and VD is the voltage across the diode. The term kT/q is the thermal voltage, sometimes written VT, and is approximately 26 mV at room temperature. n is the emission coefficient, which is typically 1 for most devices.

Equation 1:

Silicone saturation current IS ≈ 10 -13A Germanium saturation current IS ≈ 10 -8A Rectifier diode ratings include:

  • Forward current
  • PIV
  • Forward voltage drop
  • Reverse recovery time
  • Junction Capacitance Rectifier diodes are normally only operated in forward condition, forward cutoff, or reverse cutoff. The PIV rating is not an indication of where reverse conduction actually occurs; it only guarantees that the diode will not break down before the PIV rating is reached. It is not a good idea to design a circuit that depends on reverse conduction in a rectifier diode because the reverse conduction voltage can not be predicted. Because uncontrolled reverse breakdown quickly leads to diode failure, (which can also damage other circuit components) you should never attempt to operate a rectifier diode in reverse conduction. The diode Cathode is identified by a band on the cathode end.

A half wave rectifier produces an output pulse during only one half of the AC input waveform. Note that the forward voltage drop reduces the output voltage by one diode drop (Vd) Half Wave rectifier circuit When a capacitor is connected in parallel with RL, the half wave output becomes a “filtered” DC. As the voltage of the input sine wave increases, the diode will begin to conduct and charge the capacitor. When the input sine wave voltage falls below the capacitor voltage, the diode turns off and the capacitor discharges into the load. The size of the resistor will determine Vmin. As the load resistance is increased: IL decreases, the capacitor discharges less, Vmin increases, Vrms (effective voltage) increases, and Vpp (ripple voltage) decreases. Vmax does not change much because the diode forward voltage drop is relatively constant and Vmax = Vin – Vd. A full wave bridge rectifier produces an output pulse for both halves of the AC input waveform. Note that for each half cycle the output voltage is reduced by two diode drops because there are two legs conducting (each leg has a diode). If a capacitor is connected to the load, the full wave charges the capacitor on both halves of the cycle, producing a higher Vmin , a higher Vrms, and much lower Vpp than a half wave rectifier with the same load resistor.