Davisson Germer Experiment

The famous Davisson Germer electron diffraction experiment was performed due to the lack of explanation of an atomic model's wave nature's properties. In 1927 scientists C.J. Davisson and L.H. Germer carried out an experiment to explain an electron's wave nature. This was proposed through electron diffraction method. 

This section discusses the experiment and its observation in a detailed manner. The explanations are lucid in nature to help students understand the concepts better. This topic carries heavy weightage in term of marks in the examination. 

With a thorough reading, students can solve the variables and equations related to Davisson Germer experiment easily.

Davisson and Germer Experiment on Electron Diffraction Result

Under the Davisson Germer electron diffraction experiment, a student can get the value of scattering angle θ. They can also find the possible difference V's equivalent value at which electrons' scattering is the highest. The data collected by Davisson and Germer gives two theories or an equation that again shows the same value for λ. If we include De Broglie's duality in a wave-particle, there can be two equations (a) and (b).

The equation that substantiates the De Broglie's wave-particle duality is – 

• λ = h/√2meV2meV

Here one can find V's value to be 54 V

Now we know that λ = 12.27/√5454 which gives us the value 0.167 nm 

If we go through the equation, we find that'd' will have a value of 0.092 nm. It is gained through X-ray scattering. That gives us v's value to be 54 V. The angle of scattering is equal to 500500. 

Now applying this value in a second equation, we get that

• (b) nλ = 2 (0.092 nm) sin( 900−500/2)900−500/2)

Let's take n's value to be 1, while λ is 0.165 nm

This value finally verifies the theoretical explanation of the De Broglie equation. 

Davisson and Germer Electron Diffraction Experiment Observation

To find the presence of an electron in a particle form, a student can use a detector. Davisson Germer electron diffraction experiment indicates that a detector receives electronic current, i.e. electron. Here the strength or intensity of an electric current produced or received and scattered in an angle is studied. This current referred to as electron intensity.

Another observation that students can find here explains how the intensity of a scattered electron is never continuous. One can find both minimum and maximum value analogous to the utmost and least diffraction pattern gained via X-rays.

Scattered electrons have continuous intensity levels, which displays a maximum and the least analogous value to the utmost, and minimum value of a diffraction pattern created by X-rays. This value can be found by studying potential differences and scattering angles.

The Setup of Davisson Germer Experiment

Lastly, under this Davisson Germer electron diffraction experiment, a student can understand the setup formed. Ideally, the thought behind this elaborate experiment was the nature of wave particles reflected.

Davisson and Germer's experiment shows that waves reflected in a Ni crystal that passes two atomic layers contain a constant phase disparity. Students can learn that after reflection, these waves encumber annihilation or construction. This gives rise to the famous diffraction pattern.

It is seen that during the Davisson and Germer experiment, electrons are replaced with wave particles. These electrons combined to form a diffraction pattern. Finally, producing the ultimate result, which is the dual nature of matter.

Davisson Germer experiment electron diffraction chapter is complicated in terms of equation and usage. A student needs to have a clear understanding of the basic topics that carry high marks. This complex topic requires students to depend on guidebooks and study materials that offer only exercises not a valid explanation.