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An electron istrapped in a finite well. How "far" (in eV) is it from being free if the penetration length of its wave function into the classically forbidden region 1nm?

Short Answer

Expert verified

The distance of the electron to set free is 0.038eV.

Step by step solution

01

Identification of given data

The penetration length of the classically forbidden region isL=1nm.

02

Concept/Significance of a potential well

A potential well is a place in aforce field, where the atomic nucleus is located and where the potential is much lower than at a point immediately outside it unless aparticle accumulates a significant amount of energy.

03

Determination of the distance of the electron from being free

The distance of the electron is mathematically presented as:

=2mU0-EU0-E=2m22

Here, is the reduce planks constant whose value is 1.05510-34Js , is the mass of the electron whose value is 9.1110-31kg , and U0-Eis the distance of the potential well to free the electron.

Replaceall the values in the above equation:

U0-E=29.1110-31kg10-9m21.05510-34Js2=6.110-21J6.241018eV1J=38.06410-3eV=0.038eV.

Hence, the distance of the electron to set free is 0.038eV.

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Most popular questions from this chapter

Calculate the uncertainty in the particle鈥檚 momentum.

Consider a particle of mass mand energy E in a region where the potential energy is constant U0. Greater than E and the region extends tox=+

(a) Guess a physically acceptable solution of the Schrodinger equation in this region and demonstrate that it is solution,

(b) The region noted in part extends from x = + 1 nm to +. To the left of x = 1nm. The particle鈥檚 wave function is Dcos (109m-1 x). Is also greater than Ehere?

(c) The particle鈥檚 mass m is 10-3 kg. By how much (in eV) doesthe potential energy prevailing from x=1 nm to U0. Exceed the particle鈥檚 energy?

Repeat the exercise 60-62 for the first excited state of harmonic oscillator.

A half-infinite well has an infinitely high wall at the origin and one of finite height U0 at x= L . Like the finite well, the number of allowed states is limited. Assume that it has two states, of energy E1 and E2 , where E2 is not much below U0. Make a sketch of the potential energy, then add plausible sketches of the two allowed wave functions on separate horizontal axes whose heights are E1 and E2 .

Consider a particle bound in a infinite well, where the potential inside is not constant but a linearly varying function. Suppose the particle is in a fairly high energy state, so that its wave function stretches across the entire well; that is isn鈥檛 caught in the 鈥渓ow spot鈥. Decide how ,if at all, its wavelength should vary. Then sketch a plausible wave function.

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