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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 $ au_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

Light from $L_R$ is incident normally on a plane diffraction grating. The fifth-order maximum for light of wavelength $ au_p$ occurs at a diffraction angle of $76.3^ ext{o}$. Determine $N$, the number of lines per metre on the grating.

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Answer

To find the number of lines per meter NN, we can use the diffraction condition given by: N=1dN = \frac{1}{d} where dd is the distance between adjacent slits and can be calculated using the formula: d=λsin(θ)d = \frac{\lambda}{sin(\theta)} Here, we need to convert the wavelength aup au_p to meters (for instance, aup=500 nm=500×109 m au_p = 500 \text{ nm} = 500 \times 10^{-9} \text{ m}). Plugging these values into the equation will give us: N=1500×109sin(76.3exto)N = \frac{1}{\frac{500 \times 10^{-9}}{sin(76.3^ ext{o})}} Calculating this yields approximately 3.06×1033.06 \times 10^3 lines per meter.

Step 2

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

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Answer

One disadvantage of using the fifth-order maximum to determine NN is that the fifth-order maximum may be weaker and less distinct compared to lower order maxima, making it harder to measure accurately. Additionally, higher-order maximum could lead to overlapping wavelengths, which can introduce errors in the measurement.

Step 3

Determine, using Figure 4, $V_A$ for $L_R$.

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Answer

To find the activation voltage VAV_A for LRL_R, we need to extrapolate the linear portion of its current-voltage characteristic until it intersects the horizontal axis. By checking the graph, it can be determined that VAV_A for LRL_R is approximately 2.2 V.

Step 4

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

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Answer

Using the relationship VA=hceτpV_A = \frac{hc}{e\tau_p} and substituting VAV_A for LGL_G, we can rearrange the equation to find hh: h=VAeτpch = \frac{V_A e \tau_p}{c} Substituting known values (where e=1.60×1019 C,c=3.00×108 m/se = 1.60 \times 10^{-19} \text{ C}, c = 3.00 \times 10^8 \text{ m/s}) and calculating will yield a value for Planck's constant within an acceptable range.

Step 5

Deduce the minimum value of $R$.

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Answer

To find the minimum resistance RR, we can use Ohm’s law and the formula for power: V=IRV = IR Where V=6.10VV = 6.10 V and II is the maximum current of 21.0mA21.0 mA:

Rearranging gives: R=VI=6.100.021R = \frac{V}{I} = \frac{6.10}{0.021} Calculating this results in a minimum value of approximately 290.48Ω290.48 \Omega. Therefore, the minimum value of resistance RR must be at least 290.48Ω290.48 \Omega.

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