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Question #43751

Difficulty: 8/10 | 🟢 Free

The Question

A photocell is connected in series with a load resistor RL=200 kΩR_L = 200 \ \text{k}\Omega and an ideal DC voltage source of EMF E=15 VE = 15 \ \text{V}. The potential difference across the photocell, VpV_p, is measured by finding the null point on a potentiometer wire of length L=100 cmL = 100 \ \text{cm}. The potentiometer wire is connected across a separate ideal standard cell of 10 V10 \ \text{V}. In the operating region, the photocell is near saturation, and its non-ideal current-voltage characteristic is given by I=I0+VprdI = I_0 + \frac{V_p}{r_d}, where I0I_0 is the ideal saturation current proportional to the incident light intensity, and rd=200 kΩr_d = 200 \ \text{k}\Omega is the dynamic resistance of the photocell. Initially, the photocell is illuminated such that I0=25 μAI_0 = 25 \ \mu\text{A}, and the potentiometer null point is obtained at a distance x1x_1 from the high-potential end. The light intensity is then increased such that I0I_0 becomes 45 μA45 \ \mu\text{A}, and the new null point is at x2x_2. Calculate the magnitude of the shift in the null point, ∣Δx∣=∣x2−x1∣|\Delta x| = |x_2 - x_1|.

Options

  • A.

    20 cm20 \ \text{cm}

  • B.

    40 cm40 \ \text{cm}

  • C.

    10 cm10 \ \text{cm}

  • D.

    30 cm30 \ \text{cm}

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Correct Answer

Step-by-Step Solution

Explanation

How the Examiner Thinks

Multi-Concept_Bridge

Master problems that require linking physics and math concepts to solve complex competitive questions.

Concepts Behind This Question

Photoelectric Saturation|Dynamic Resistance (AC Resistance)|Potentiometer Null Point|Calculus (Derivatives)

Why This Question Is Tricky

Common Mistakes

This question tests the student's ability to integrate non-ideal device characteristics with standard circuit analysis, specifically targeting the misconception that a photocell in saturation acts as an ideal current source.

Students commonly memorize that photoelectric current in saturation depends only on light intensity and is independent of voltage.

If they misapply this by ignoring the dynamic resistance (rd→∞r_d \to \infty), they will use I=I0I = I_0 and calculate Vp=E−I0RLV_p = E - I_0 R_L.

This incorrect assumption yields Vp1=10 VV_{p1} = 10 \ \text{V} and Vp2=6 VV_{p2} = 6 \ \text{V}, leading to a null point shift of 40 cm40 \ \text{cm} (Option B).

By forcing the intersection of the potentiometer's linear load line with the diode's non-linear saturation region, the problem evaluates whether the student can mathematically model the physical reality of the Schottky effect (finite dynamic resistance) in a vacuum diode.

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Question Information

SubjectPhysics
ChapterDual Nature of Radiation and Matter - Class 12
ConceptPhotoelectric Saturation
Difficulty8
Cognitive Load7
Target Solve Time160 sec
AccessFree