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Question #43453

Difficulty: 8/10 | 🟢 Free

The Question

A small-signal half-wave rectifier circuit uses a p-n junction diode biased at a constant forward DC voltage V0V_0. The circuit employs an inductor filter and a negligible load resistance such that the ripple factor γ\gamma of the output is directly proportional to the diode's dynamic forward resistance rdr_d. The reverse saturation current of the diode is given by Is=CT3exp⁡(−Eg/kT)I_s = C T^3 \exp(-E_g/kT), where CC is a constant, kk is the Boltzmann constant, and EgE_g is the bandgap energy. Due to thermal expansion and electron-phonon interactions, the bandgap decreases with absolute temperature TT as Eg(T)=Eg0−αTE_g(T) = E_{g0} - \alpha T, where Eg0E_{g0} and α\alpha are positive constants. Assuming the diode operates in the region where the forward current is I≈Isexp⁡(eV0/kT)I \approx I_s \exp(eV_0/kT) (with ee being the elementary charge), what is the fractional change in the ripple factor, Δγγ\frac{\Delta \gamma}{\gamma}, for a small increase in temperature ΔT\Delta T?

Options

  • A.

    −(Eg0−eV0+2kTkT2)ΔT-\left( \frac{E_{g0} - eV_0 + 2kT}{kT^2} \right) \Delta T

  • B.

    −(Eg0−αT−eV0+2kTkT2)ΔT-\left( \frac{E_{g0} - \alpha T - eV_0 + 2kT}{kT^2} \right) \Delta T

  • C.

    −(Eg0−eV0+3kTkT2)ΔT-\left( \frac{E_{g0} - eV_0 + 3kT}{kT^2} \right) \Delta T

  • D.

    −(Eg0−αT−eV0+3kTkT2)ΔT-\left( \frac{E_{g0} - \alpha T - eV_0 + 3kT}{kT^2} \right) \Delta T

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Correct Answer

Step-by-Step Solution

Explanation

How the Examiner Thinks

Variable_Constraint

Develop pure symbolic logic skills by mastering algebraic constraints without relying on numerical data.

Concepts Behind This Question

Rectifier Ripple Factor|Energy Band Gap Temperature Dependency|Approximations (Binomial)

Why This Question Is Tricky

Common Mistakes

This question tests the integration of solid-state device physics with analog circuit analysis, specifically targeting the temperature dependence of the quiescent operating point.

The primary trap lies in the differentiation of the Boltzmann factor containing the temperature-dependent bandgap Eg(T)=Eg0−αTE_g(T) = E_{g0} - \alpha T.

Students often mistakenly treat Eg(T)E_g(T) as a static variable during differentiation or directly substitute it back at the end, leading to an erroneous αT\alpha T term in the final expression (Option B).

They fail to realize that exp⁡(αT/kT)=exp⁡(α/k)\exp(\alpha T / kT) = \exp(\alpha/k) is a temperature-independent constant that vanishes upon logarithmic differentiation.

A secondary trap involves forgetting the explicit TT dependence in the numerator of the dynamic resistance formula (rd=kT/eIr_d = kT/eI), which leads to an incorrect coefficient for the kTkT term (Option C).

Quick Facts About This Question

Question Information

SubjectPhysics
ChapterSemiconductor Electronics: Materials, Devices, and Simple Circuits - Class 12
ConceptRectifier Ripple Factor
Difficulty8
Cognitive Load7
Target Solve Time160 sec
AccessFree