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A beam of neutrons with energy E runs horizontally into a crystal. The crystal transmits half the neutrons and deflects the other half vertically upwards. After climbing to height H these neutrons are deflected through 90 degrees onto a horizontal path parallel to the originally transmitted beam. The two horizontal beams now move a distance L down the laboratory, one distance H above the other. After going distance L, the lower beam is deflected vertically upwards and is finally deflected into the path of the upper beam such that the two beams are co-spatial as they enter the detector. Given that particles in both the lower and upper beams are in states of well-defined momentum, show that the wavenumbers k, k^{′} of the lower and upper beams are related by
{\large k \simeq k' \left( 1- \frac{m_{{\small N}}gH}{2E} \right) }
Attempted Solution:
Let E be the kinetic energy of the neutrons in lower beam.
{\large k = \frac{\sqrt{2mE}}{h}}
{\large k' \simeq \frac{\sqrt{2m(E - mgh)}}{h}}
\Rightarrow {\large \frac{k}{k'} \simeq \sqrt{\frac{2mE}{2m(E-mgh)}} = \sqrt{\frac{E}{E-mgh}} }
I have no idea how to go beyond this.
{\large k \simeq k' \left( 1- \frac{m_{{\small N}}gH}{2E} \right) }
Attempted Solution:
Let E be the kinetic energy of the neutrons in lower beam.
{\large k = \frac{\sqrt{2mE}}{h}}
{\large k' \simeq \frac{\sqrt{2m(E - mgh)}}{h}}
\Rightarrow {\large \frac{k}{k'} \simeq \sqrt{\frac{2mE}{2m(E-mgh)}} = \sqrt{\frac{E}{E-mgh}} }
I have no idea how to go beyond this.