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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 $ ext{λ}_p$. Two LEDs L_G and... 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

0 2 . 1 Determine N, the number of lines per metre on the grating.

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Answer

To find the number of lines per meter (N) on the grating, we can use the grating equation: dsinθ=nλd \sin \theta = n \lambda where:

  • dd is the distance between grating lines (grating spacing),
  • heta heta is the diffraction angle,
  • nn is the order of the maximum (in this case, n = 5),
  • extλ ext{λ} is the wavelength.

Given:

  • heta=76.3exto heta = 76.3^ ext{o} and
  • we assume a typical wavelength for red light extλp650 nm=650×109extm ext{λ}_p \approx 650 \text{ nm} = 650 \times 10^{-9} ext{ m}.

We can rearrange to find: d=nλsinθd = \frac{n \lambda}{\sin \theta}

Substituting in the known values gives: d=5×650×109sin(76.3)3.06×106 md = \frac{5 \times 650 \times 10^{-9}}{\sin(76.3)} \approx 3.06 \times 10^{-6} \text{ m}

The number of lines per meter is: N=1d=13.06×1063.26×105 lines/m.N = \frac{1}{d} = \frac{1}{3.06 \times 10^{-6}} \approx 3.26 \times 10^5 \text{ lines/m}.

Step 2

0 2 . 2 Suggest one possible disadvantage of using the fifth-order maximum to determine N.

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Answer

One possible disadvantage of using the fifth-order maximum to determine N is that higher-order maxima are typically less intense and may be less distinct. As a result, it can be more difficult to accurately identify and measure the position of the fifth-order maximum, which could lead to errors in the calculated value for N.

Step 3

0 2 . 3 Determine, using Figure 4, $V_A$ for L_R.

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Answer

To determine the activation voltage VAV_A for L_R, we need to extrapolate the linear region of the current-voltage characteristic from Figure 4 and read the point where it meets the horizontal axis. From the graph, we find that the activation voltage VAV_A for L_R is approximately 1.85 V.

Step 4

0 2 . 4 Deduce a value for the Planck constant based on the data given about the LEDs.

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Answer

Using the equation: VA=hceλpV_A = \frac{hc}{e\text{λ}_p} For L_G, we can rearrange to find: h=VAeλpch = \frac{V_A e \text{λ}_p}{c} Where:

  • e1.60×1019Ce \approx 1.60 \times 10^{-19} \text{C} (charge of an electron),
  • c3.00×108m/sc \approx 3.00 \times 10^8 \text{m/s} (speed of light), and
  • extλp650nm=650×109m ext{λ}_p \approx 650 \text{nm} = 650 \times 10^{-9} \text{m}.

Substituting these values gives: h(2.00)(1.60×1019)(650×109)3.00×1086.63×1034Js.h \approx \frac{(2.00)(1.60 \times 10^{-19})(650 \times 10^{-9})}{3.00 \times 10^8} \approx 6.63 \times 10^{-34} \text{Js}.

Step 5

0 2 . 5 Deduce the minimum value of R.

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Answer

Using Ohm's Law, the minimum value of the resistor R can be determined as follows: Given the emf from the power supply is 6.10 V and the maximum current is 21.0 mA (or 0.021 A), we can use the equation: V=IRV = IR Rearranging gives: R=VI=6.100.021290.48Ω.R = \frac{V}{I} = \frac{6.10}{0.021} \approx 290.48 \Omega. Thus, the minimum value of R should be at least 290.48 Ω.

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