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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 metre (NN), we can use the diffraction grating formula: dimesextsin(heta)=maupd imes ext{sin}( heta) = m au_p where dd is the distance between adjacent lines (grating spacing), heta heta is the diffraction angle, and mm is the order number (5 in this case).

First, we calculate dd: d = rac{ au_p}{m imes ext{sin}(76.3^{ ext{o}})} Substituting values: Assuming aup au_p is about 650 nm (near red light), d = rac{650 imes 10^{-9}}{5 imes ext{sin}(76.3^{ ext{o}})} Calculating gives: N = rac{1}{d} ext{, and thus } N ext{ is approximately } 3.06 imes 10^3 ext{ lines/m}.

Step 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 is that it can be harder to accurately measure the angle due to increased diffraction spread, which can lead to measurement errors. As higher orders can often result in more pronounced overlap of adjacent maxima, leading to difficulties in isolation.

Step 3

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

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To determine the activation voltage VAV_A for LRL_R, we extrapolate the linear portion of the current-voltage characteristic curve intersecting the horizontal axis. From Figure 4, we see this intersection occurs at approximately 2.1 V.

Step 4

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

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From the equation VA=hceτpV_A = \frac{hc}{e \tau_p}, rearranging gives: h=VAeτpch = \frac{V_A e \tau_p}{c} Substituting the known values, where VAV_A for LGL_G is 2.00 V, e=1.6×1019Ce = 1.6 \times 10^{-19} C, c=3.00×108m/sc = 3.00 \times 10^8 m/s, and using an approximate aup au_p value of 650 nm (which is 6.50×107m6.50 \times 10^{-7} m) leads to: h=(2.00)(1.6×1019)(6.50×107)(3.00×108)h = \frac{(2.00)(1.6 \times 10^{-19})(6.50 \times 10^{-7})}{(3.00 \times 10^8)} Calculating this yields a Planck constant value in a range consistent with known values.

Step 5

Deduce the minimum value of $R$.

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Answer

Using Ohm's law and the principle of total voltage in a series circuit, we have: V=IR+VAV = I R + V_A Where the total voltage supplied is 6.10 V and II must be less than or equal to 21.0 mA. Substituting gives: 6.10=(21.0×103)R+2.006.10 = (21.0 \times 10^{-3})R + 2.00 Rearranging to solve for RR provides: R=6.102.0021.0×103R = \frac{6.10 - 2.00}{21.0 \times 10^{-3}} Thus gives a minimum resistance of about 195 Ω.

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