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Question Bank (5 marks) · Q3

Q.Explain V-I Characteristics of a power diode.

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[!TLDR]

Forward: small current up to VjV_j, then a linear rise set by RONR_{ON}; reverse: small leakage up to VBRV_{BR}, then avalanche.

The static V-I characteristic of a power diode is drawn with forward current IFI_F (and voltage) in the first quadrant and reverse current (and voltage) in the third quadrant.

Forward characteristic: For small forward voltages, below the knee (threshold) voltage VjV_j (about 0.7 V for silicon), only a very small current flows. Once the junction is forward biased beyond the knee, the current increases, but because of the ohmic resistance RONR_{ON} of the lightly doped drift region the increase is an almost straight line rather than the sharp exponential of a signal diode. The forward drop follows

VAK=Vj+IFRONV_{AK}=V_j+I_F R_{ON}

so the forward branch is linearised with a slope determined by 1/RON1/R_{ON}.

Reverse characteristic: When reverse biased, the diode carries only a small, nearly constant reverse leakage (saturation) current, since the depletion region blocks conduction. This continues up to the reverse breakdown voltage VBRV_{BR} (the peak reverse voltage rating). Beyond VBRV_{BR} avalanche multiplication sets in and the reverse current rises steeply, which can damage the device.

Key points marked on the curve are the forward knee VjV_j, the linear forward conduction region, the small reverse leakage, and the reverse breakdown VBRV_{BR}.

[!ANSWER]

The power-diode V-I curve has a forward branch that stays low until VjV_j and then rises almost linearly (slope set by RONR_{ON}, VAK=Vj+IFRONV_{AK}=V_j+I_F R_{ON}), and a reverse branch of small leakage up to VBRV_{BR}, beyond which avalanche breakdown occurs.

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