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Electron Diffraction Experiment by Eric Cotner (presenting) and Yukun Zhang.

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Presentation on theme: "Electron Diffraction Experiment by Eric Cotner (presenting) and Yukun Zhang."— Presentation transcript:

1 Electron Diffraction Experiment by Eric Cotner (presenting) and Yukun Zhang

2 Apparatus Electron gun Voltage supply Multimeter Carbon diffraction grating Phosphorescent screen

3 Electronics Electron gun accelerating voltage controlled by power supply Accelerating voltage determines kinetic energy (and wavelength) of electrons Current is limited to avoid burning out the filament

4 Theory De Broglie hypothesis: matter can actually be described with wavelike properties (p=h/λ, E=hf) From λ= ℎ /(2mE) 1/2, the wavelength of an electron is inversely proportional to the square root of its kinetic energy We expect that accelerated electrons will be diffracted from a sufficiently small spacing, such as the crystals in a carbon lattice

5 Derivation of Results Electrons are diffracted by carbon lattice; 2 different spacings will create 2 concentric rings obeying the law nλ=dγ where γ=2θ, n=1, and d is the crystal spacing Using E=hf and p=h/λ, we can calculate λ in terms of accelerating voltage in the following way: – E = p 2 /2m = (h/λ) 2 /2m – λ = h/(2m e eV) 1/2 – λ = (1.23 V -1/2 ) nm Using small angle approximation, γ=D’/2L Setting λ = dγ = (1.23 V -1/2 ) nm allows us to calculate d (in nm) from the slope of V -1/2 = d(γ/1.23) by plotting γ vs. V -1/2

6 Calculation of D’ Find D’ from ratios of similar triangles using the radius of curvature of the phosphorescent screen Equation to use:

7 Diffraction Ring Data V (V)1400 2500 D 1 (mm)68.5566.8466.9867.2952.5052.6753.1052.74 D 2 (mm)39.7242.3641.0641.2833.6031.1932.2730.67 V (V)16001700180019002000210023002700 D 1 (mm)63.9962.6061.1057.7558.6356.3355.1950.65 D 2 (mm)38.3238.7236.9935.1933.5732.5832.0229.86 4 measurement for 2 different voltages: 1 measurement for 8 different voltages:

8 Derived Quantities V (V)1400 2500 D’ 1 (mm)73.4071.3071.4771.8554.5554.7455.2254.82 D’ 2 (mm)40.5843.4142.0142.2534.1131.6032.7231.08 λ (nm).0329.0246 γ1γ1.242.236.237.238.186.188.186 γ2γ2.140.150.145.146.119.110.114.108 V (V)16001700180019002000210023002700 D’ 1 (mm)67.8666.2064.4360.5361.5458.8957.5952.48 D’ 2 (mm)39.0939.5137.6835.7834.0833.0532.4630.22 λ (nm).0308.0298.0290.0282.0275.0268.0256.0237 γ1γ1.226.221.216.204.207.199.195.179 γ2γ2.135.137.131.124.119.115.113.106

9 D 1 ’ d 1 /(1.23x10 -6 2L) vs. V -1/2 d 1 = 0.128 nm

10 D 2 ’ d 2 /(1.23x10 -6 2L) vs. V -1/2 d 2 = 0.220 nm

11 Error Analysis Used the above error propagation formulae For d 1, evaluated at D 1 ’=57.5 mm, V=2000 V, δD 1 ’=1.73 mm, δV=50 V – δd 1 =0.0044 nm For d 2, evaluated at D 2 ’=30 mm, V=2000 V, δD 2 ’=1.55 mm, δV=50 V – δd 2 =0.0138 nm

12 Comparison to accepted values Accepted values: – d 1 =0.123 nm and d 2 =0.213 Derived values: – d 1 =0.128 ± 0.004 nm and d 2 =0.220 ± 0.014 Accepted values fall within uncertainties of derived values, strong support for validity of accepted values

13 Conclusions 4% error for spacing of d 1 3.3% error for spacing of d 2 Strong support for de Broglie wave theory of moving particles Strong support for accepted crystal structure of carbon


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