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A light-emitting diode (LED) emits light over a narrow range of wavelengths - AQA - A-Level Physics - Question 2 - 2021 - Paper 3

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A light-emitting diode (LED) emits light over a narrow range of wavelengths. These wavelengths are distributed about a peak wavelength \(\lambda_p\). Two LEDs \(L_G... show full transcript

Worked Solution & Example Answer:A light-emitting diode (LED) emits light over a narrow range of wavelengths - AQA - A-Level Physics - Question 2 - 2021 - Paper 3

Step 1

Determine \(N\), the number of lines per metre on the grating.

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Answer

To find the number of lines per metre, we can use the diffraction formula:

dsinθ=nλd \sin \theta = n \lambda

Where:

  • (d) is the distance between grating lines (in metres)
  • (\theta) is the diffraction angle (76.3°)
  • (n) is the order of the maximum (5th order)
  • (\lambda) is the wavelength corresponding to (\lambda_p)

First, we convert the angle to radians for calculations: [ \theta = 76.3^{\circ} \approx 1.33 \text{ radians} ]

Now we can rearrange the formula to calculate (d) as:

d=nλsinθd = \frac{n \lambda}{\sin \theta}

If we take (\lambda_p) as 650 nm (0.00065 m) for calculations: [ d = \frac{5 \times 0.00065}{\sin(76.3^{\circ})} \approx 0.000104 m ]

The number of lines per metre (N ) is given by: [ N = \frac{1}{d} \approx \frac{1}{0.000104} \approx 9615 \text{ lines/m} ]

Step 2

Suggest one possible disadvantage of using the fifth-order maximum to determine \(N\).

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Answer

One potential disadvantage is that the fifth-order maximum is more susceptible to measurement errors due to reduced intensity and potential overlap with other maxima. This can cause inaccuracies in determining the exact angle for the fifth-order maximum, leading to errors in the calculated value of (N). Additionally, higher orders can be less distinct, making them harder to measure accurately.

Step 3

Determine, using Figure 4, \(V_A\) for \(L_R\).

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Answer

To find (V_A) for (L_R), we need to extrapolate the linear region of the current-voltage characteristic in Figure 4 to the x-axis. This involves drawing a straight line through the linear portion of the curve until it intersects the x-axis. The x-coordinate at this intersection gives (V_A). After analyzing Figure 4, we find that (V_A \approx 1.80 V) for (L_R).

Step 4

Deduce a value for the Planck constant based on the data given about the LEDs.

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Answer

Using the equation for the activation voltage: VA=hceλpV_A = \frac{hc}{e \lambda_p}

We can rearrange this to solve for the Planck constant (h): h=VAeλpch = \frac{V_A e \lambda_p}{c}

Substituting values:

  • (V_A \approx 2.00 V) (for (L_G))
  • Charge of an electron, (e \approx 1.6 \times 10^{-19} C)
  • Speed of light, (c \approx 3.0 \times 10^8 m/s)
  • Wavelength, (\lambda_p \approx 650 \times 10^{-9} m)

Now plug in the values: h=2.00×(1.6×1019)×(650×109)3.0×1081.054×1034Jsh = \frac{2.00 \times (1.6 \times 10^{-19}) \times (650 \times 10^{-9})}{3.0 \times 10^8} \approx 1.054 \times 10^{-34} J s

Step 5

Deduce the minimum value of \(R\).

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Answer

We use Ohm's law, which states: V=IRV = I R

Given:

  • Total voltage of the supply is 6.10 V.
  • The maximum current (I) in (L_R) should not exceed 21.0 mA (0.021 A).

Thus, we rearrange Ohm's law: R=VIR = \frac{V}{I}

Substituting the values: R=6.100.021290.48ΩR = \frac{6.10}{0.021} \approx 290.48 \Omega

Therefore, the minimum resistance (R) must be at least 290.48 Ω (rounded to the nearest standard resistor value, 330 Ω could be used).

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