Home
Class 12
PHYSICS
The potential energy of a particle varie...

The potential energy of a particle varies as .
`U(x) = E_0 ` for ` 0 le x le 1`
`= 0` for `x gt 1 `
for `0 le x le 1` de- Broglie wavelength is `lambda_1` and for `xgt1` the de-Broglie wavelength is `lambda_2`. Total energy of the particle is `2E_0`. find `(lambda_1)/(lambda_2).`

A

`sqrt((3)`

B

`sqrt((7)`

C

`sqrt((2)`

D

`sqrt((5)`

Text Solution

AI Generated Solution

The correct Answer is:
To solve the problem, we need to find the ratio of the de Broglie wavelengths \( \frac{\lambda_1}{\lambda_2} \) for a particle in two different potential energy regions. Let's break down the solution step by step. ### Step 1: Analyze the potential energy in the two regions The potential energy \( U(x) \) is defined as: - \( U(x) = E_0 \) for \( 0 \leq x \leq 1 \) - \( U(x) = 0 \) for \( x > 1 \) The total energy of the particle is given as \( E_{total} = 2E_0 \). ### Step 2: Calculate the kinetic energy in the first region \( (0 \leq x \leq 1) \) In the region where \( 0 \leq x \leq 1 \): - The potential energy \( U = E_0 \) - The total energy \( E_{total} = 2E_0 \) Using the relationship between total energy, potential energy, and kinetic energy: \[ K.E. = E_{total} - U = 2E_0 - E_0 = E_0 \] ### Step 3: Calculate the de Broglie wavelength \( \lambda_1 \) in the first region The de Broglie wavelength is given by the formula: \[ \lambda = \frac{h}{\sqrt{2mK.E.}} \] Substituting the kinetic energy we found: \[ \lambda_1 = \frac{h}{\sqrt{2mE_0}} \] ### Step 4: Calculate the kinetic energy in the second region \( (x > 1) \) In the region where \( x > 1 \): - The potential energy \( U = 0 \) - The total energy \( E_{total} = 2E_0 \) Using the relationship again: \[ K.E. = E_{total} - U = 2E_0 - 0 = 2E_0 \] ### Step 5: Calculate the de Broglie wavelength \( \lambda_2 \) in the second region Using the kinetic energy we found: \[ \lambda_2 = \frac{h}{\sqrt{2m(2E_0)}} = \frac{h}{\sqrt{4mE_0}} \] ### Step 6: Find the ratio \( \frac{\lambda_1}{\lambda_2} \) Now we can find the ratio of the two wavelengths: \[ \frac{\lambda_1}{\lambda_2} = \frac{\frac{h}{\sqrt{2mE_0}}}{\frac{h}{\sqrt{4mE_0}}} \] Simplifying this expression: \[ \frac{\lambda_1}{\lambda_2} = \frac{h \cdot \sqrt{4mE_0}}{h \cdot \sqrt{2mE_0}} = \frac{\sqrt{4}}{\sqrt{2}} = \sqrt{2} \] ### Final Result Thus, the ratio of the de Broglie wavelengths is: \[ \frac{\lambda_1}{\lambda_2} = \sqrt{2} \]
Promotional Banner

Similar Questions

Explore conceptually related problems

The potential energy of a partical varies as . U(x) = E_0 for 0 le x le 1 = 0 for x gt 1 For 0 le x le 1 , de- Broglie wavelength is lambda_1 and for xgt the de-Broglie wavelength is lambda_2 . Total energy of the partical is 2E_0. find (lambda_1)/(lambda_2).

The potential energy of particle of mass m varies as U(x)={(E_(0)"for"0lexle1),(0" for " gt 1):} The de Broglie wavelength of the particle in the range 0lexle1 " is " lamda_(1) and that in the range xgt1" is "lamda_(2) . If the total of the particle is 2E_(0)," find "lamda_(1)//lamda_(2) .

Derive the relation between the wavelength (lambda) of the de broglie wave and kinetic energy (E ) of a moving particle

State how de-Broglie wavelength (lambda) of moving particles varies with their linear momentum (P).

The log - log graph between the energy E of an electron and its de - Broglie wavelength lambda will be

Kinetic energy of the particle is E and it's De-Broglie wavelength is lambda . On increasing it's KE by delta E , it's new De-Broglie wavelength becomes lambda/2 . Then delta E is

Kinetic energy of the particle is E and it's De-Broglie wavelength is lambda . On increasing it's KE by delta E , it's new De-Broglie wavelength becomes lambda/2 . Then delta E is

If the de-Broglie wavelength is lambda_(0) for protons accelerated through 100 V, then the de-Broglie wavelength for alpha particles accelerated through the same voltage will be

Electrons with de-Broglie wavelength lambda fall on the target in an X-ray tube. The cut-off wavelength of the emitted X-ray is

Electrons with de-Broglie wavelength lambda fall on the target in an X-ray tube. The cut-off wavelength of the emitted X-ray is