AQA A-Level Physics Paper 3 (3BE), June 2025: Question 3
8 marks · Medium difficulty · Short Answer
Analyze a multi-stage light-intensity monitor using a photodiode and operational amplifiers, including drawing a non-inverting amplifier circuit and determining the threshold irradiance from a calibration graph.
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Question text
03.1 A photodiode can be used in either photovoltaic mode or photoconductive mode.
State one advantage of using a photodiode in photoconductive mode.
[1 mark]
A light-intensity monitor uses a photodiode in reverse bias. The photodiode responds
to the irradiance of light incident on it.
Irradiance is a measure of the power of the light incident on unit surface area and is
measured in W m−2.
Figure 7 shows the three stages that make up the light-intensity monitor.
Figure 7
Each stage uses an operational amplifier. The power rails to the operational
amplifiers are 0 V and +12 V; these are not shown in Figures 8, 9 or 10.
Figure 8 shows the circuit for stage 1.
Figure 8
When the photodiode detects light within its sensitive range, there is a reverse
photocurrent ID in the circuit. This current depends on the irradiance of the light.
The output voltage Vout of the circuit is proportional to ID.
Point X is a virtual earth.
03.2 Explain what is meant by a virtual earth.
[1 mark]
03.3 The output signal Vout from stage 1 is used as the input signal Vin for stage 2.
Figure 9 is an incomplete circuit diagram of stage 2.
Figure 9
Complete Figure 9 to show how an operational amplifier is configured to produce a
voltage gain of +34
In your answer:
• label resistors with their values within the range 1 kΩ to 100 kΩ
• show the inverting (−) and non-inverting (+) inputs to the operational amplifier
• do not show the power supplies or power rails for the operational amplifier.
[2 marks]
03.4 Stage 3 uses an operational amplifier as a comparator to determine whether the
irradiance detected by the photodiode in stage 1 exceeds a critical value.
Figure 10 shows the stage 3 circuit diagram.
Figure 10
Figure 11 shows part of the data sheet for the photodiode.
Figure 11
Determine the minimum irradiance that must be detected by the photodiode in
stage 1 in order to turn on the LED in stage 3.
[3 marks]
irradiance = W m−2
03.5 When the monitor is tested, the LED turns on fully.
However, the LED does not turn off fully when the irradiance falls below the
critical value.
Suggest one reason why the LED does not turn off fully.
In your answer, refer to a limitation of real operational amplifiers.
[1 mark]
Mark scheme
Show the mark scheme
Question Answers Additional comments/Guidance Mark AO
03.1 One from: Accept other correct answers. 1 AO1
• shorter response time
• current varies linearly with illumination
03.2 A virtual earth is a point that sits at 0 V (due to the configuration of Accept the idea that it acts as if grounded. 1 AO1
the circuit) even though there is no direct physical connection to
ground OWTTE
03.3 Condone lack of connection blobs on this 2 AO2
occasion.
Condone the use of an input resistor on the
non-inverting input but cannot be used as
part of gain calculation.
mp1 - general configuration for operational
amplifier giving a non-inverting amplification
including correctly labelled input terminals
mp2 - use of resistors within the defined
Rf
range giving = +33
R1
– A-LEVEL PHYSICS – –
03.4 Identify that the switching voltage in stage 3 is 6.8 V. 3 AO3
6.8
Output from stage 1 must be = 0.2 V 1
their MP1 value
ID in stage 1 is 2 Expect to see ID (= 20 μA) 2
10 kΩ
–2 )
Uses their mp2 value to calculate an irradiance from the graph. 3 Expect to see an irradiance of ( 4 W m 3
03.5 The idea that real op amps may saturate at a value > 0 V 1 AO2
(This may leave sufficient voltage to activate the LED)
Total 8
How to answer it
Op-Amp Light Monitor & Photodiode Circuit Analysis
This question assesses your understanding of op-amp circuits and optical sensors (AQA Option: Turning Points / Electronics):
- Photodiode modes: Advantages of photoconductive (reverse-biased) mode over photovoltaic mode.
- Virtual Earth Concept: What it means for an op-amp inverting input to be held at 0 V.
- Non-inverting amplifier design: Circuit configuration and gain equation v = 1 + (Rf / R1) .
- Multi-stage circuit deduction & log-log graph reading: Tracing backwards through a comparator, amplifier, and current-to-voltage converter.
- Real vs. Ideal Op-Amps: Output saturation limits (rail-to-rail limitations).
Part 03.1: Photodiode Operation Modes
Advantage of photoconductive mode [1 mark]
✅ Accepted Answers
- Shorter response time / faster switching speed
- Linear relationship: Photocurrent varies linearly with illumination / irradiance
💡 Key Knowledge
In photoconductive mode, the diode is reverse-biased. The applied reverse voltage increases the depletion region width, which dramatically reduces junction capacitance (leading to much faster response) and ensures photocurrent is directly proportional to incident light power over many decades.
Part 03.2: Virtual Earth Concept
Explaining the virtual earth at Point X [1 mark]
✅ Correct Answer
A point that sits at 0 V (due to circuit configuration and feedback) even though there is no direct physical connection to ground / 0 V (it acts as if grounded).
🧠 Exam Technique
Always state both elements:
1. The potential is 0 V (or at earth potential).
2. It is not directly connected to earth / ground.
❌ Common Errors
Simply stating "it is connected to earth" loses the mark completely—the entire definition of "virtual" means it is not actually connected to the ground rail!
Part 03.3: Designing the Non-Inverting Amplifier
Complete circuit diagram for a voltage gain of +34 [2 marks]
📐 Calculation of Resistors
For a non-inverting amplifier:
Voltage Gain = 1 + (Rf / R1)
- Given Gain = +34:
34 = 1 + (Rf / R1) ⇒ (Rf / R1) = 33 - Select standard resistor values within 1 kΩ to 100 kΩ:
Let R1 = 1 kΩ
Then Rf = 33 × 1 kΩ = 33 kΩ - (Alternatively: R1 = 2 kΩ, Rf = 66 kΩ or R1 = 3 kΩ, Rf = 99 kΩ ).
✅ Circuit Diagram Description
- Op-Amp Inputs: Draw op-amp triangle. Input signal Vin connects directly to the non-inverting (+) terminal.
- Feedback Loop: Feedback resistor Rf = 33 kΩ connected between output Vout and inverting (–) terminal.
- Ground Resistor: Resistor R1 = 1 kΩ connected from inverting (–) terminal down to the 0 V line.
❌ Common Errors
- Forgetting the "+1" in the non-inverting formula and using Rf / R1 = 34 .
- Swapping the (+) and (–) inputs, which creates an inverting amplifier or positive feedback oscillator.
- Choosing values outside the stated range (1 kΩ to 100 kΩ), e.g., 330 Ω and 10 Ω.
• MP1: General circuit configuration for non-inverting amplifier with correctly labelled (+) and (–) input terminals. [1 mark]
• MP2: Correct resistor pair chosen in the 1 kΩ to 100 kΩ range giving ratio Rf / R1 = 33. [1 mark]
Part 03.4: Determining the Minimum Irradiance
Multi-stage circuit deduction & graph reading [3 marks]
📐 Step-by-Step Solution
- Step 1: Identify switching voltage of Stage 3 (Comparator)
The non-inverting input of Stage 3 is held at 6.8 V by the zener diode.
For the op-amp output to go high and turn ON the LED, the non-inverting (+) input must exceed inverting (–) input, so the switching threshold is:
Vswitch = 6.8 V - Step 2: Calculate Stage 1 Output (Input to Stage 2)
Stage 2 has a gain of +34. Therefore:
Vout(Stage 1) = Vin(Stage 2) = 6.8 V / 34 = 0.20 V [1 mark, MP1] - Step 3: Calculate Photodiode Current ID in Stage 1
Stage 1 is a transimpedance amplifier (current-to-voltage converter) with feedback resistor R = 10 kΩ .
Since point X is a virtual earth (0 V), all photocurrent ID flows through the 10 kΩ resistor:
ID = Vout(Stage 1) / 10 kΩ = 0.20 V / (10 × 10³ Ω) = 2.0 × 10⁻⁵ A = 20 µA [1 mark, MP2] - Step 4: Read Irradiance from Log-Log Graph (Figure 11)
Locate reverse current = 20 µA on the vertical logarithmic axis.
Follow horizontally to the straight line, then read down to the horizontal axis:
Irradiance = 4 W m⁻² (or 4.0 W m⁻²) [1 mark, MP3]
🧠 Exam Technique: Reading Logarithmic Scales
On Figure 11, the major ticks are powers of 10 (0.1, 1, 10, 100). The intermediate lines between 10 and 100 represent 20, 30, 40, 50, etc. The first grid line above 10 is exactly 20 µA. Trace carefully across to find 4 W m⁻² on the horizontal axis.
❌ Common Errors
Misreading the log scale (e.g., treating grid divisions as linear) or forgetting the 10 kΩ factor when converting Stage 1 output voltage to photocurrent.
• MP1: Identifying 6.8 V switching threshold and calculating Stage 1 output = 6.8 / 34 = 0.2 V.
• MP2: Correctly calculating photodiode reverse current ID = 0.2 / 10 kΩ = 20 µA.
• MP3: Correctly reading irradiance from graph = 4 W m⁻².
Part 03.5: Real Operational Amplifier Limitations
Explaining why the LED does not turn off fully [1 mark]
✅ Correct Explanation
Real op-amps do not output exactly 0 V when saturated low; they saturate at a voltage greater than 0 V (e.g. 1 to 2 V above the negative supply rail). This non-zero voltage can still exceed the turn-on voltage of the LED, leaving it dimly lit.
💡 Ideal vs. Real Op-Amp Limits
- Ideal Op-Amp: Output swings rail-to-rail (from exactly 0 V to +12 V).
- Real Op-Amp: Output voltage is bounded within saturation levels typically 1–2 V inside the rails (e.g., +1.5 V to +10.5 V).
Topics
Optional topics · 3.13 Electronics (A-level only)
Question and mark scheme from the AQA A-Level Physics examination, Paper 3 (3BE), June 2025. QuestionVault is an independent revision resource; questions remain the copyright of the awarding body.