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To show that the potential energy of finite well is U=h2(n1)28mL2

Short Answer

Expert verified

The potential energy of the given infinite wall ish22(n1)28mL2.

Step by step solution

01

The concept and the formula used.

The potential energy is the stored energy that depends upon the relative position of various parts of a system.

The given potential in the finite well is:

U=2k22msec2kL2(n1)<kL<苍蟺n=1,3,5,2k22mcsc2kL2(n1)<kL<苍蟺鈥嬧赌嬧赌嬧赌嬧赌夆赌夆赌夆赌n=2,4,6....

The formula for the potential for even nis given by:

U=2k22mcsc2kL2(n1)<kL<苍蟺...(1)

Here,U is the potential, is the reduced Planck's constant, kis expressed as constant,m is the mass and Lis the depth of the potential well.

02

Calculate the value using the formula.

The expression for a minimum value of k.

k=(n1)L

Here, nis the number of states.

Calculation:

Substitute(n1)lforkin equation (1).


U=22m(n1)22L2csc2L2(n1)L

U==22(n1)22mL2csc2(n1)2

Substitute1 for the minimum value ofcsc2(n1)2 in above equation.

U=22(n1)22mL2

Substitute h2for in the above equation.

U=h22(n1)28mL2

Thus, the potential energy of infinite well ish22(n1)28mL2 .

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Most popular questions from this chapter

Summarize the similarities are differences between the three simple bound cases considered in this chapter.

The uncertainty in a particle's momentum in an infinite well in the general case of arbitrary nis given bynhL .

We learned that to be normalizable, a wave function must not itself diverge and must fall to 0 faster than |x|-1/2as x get large. Nevertheless. We find two functions that slightly violate these requirements very useful. Consider the quantum mechanical plane wave Aei(kx-ax)and the weird functionx0(x)pictured which we here call by its proper name. the Dirac delta function.

(a) Which of the two normalizability requirements is violated by the plane wave, and which by Dirac delta function?

(b) Normalization of the plane wave could be accomplished if it were simply truncated, restricted to the region -b<x<+bbeing identically 0 outside. What would then be the relationship between b and A, and what would happen to A as b approaches infinity?

(c) Rather than an infinitely tall and narrow spike like the Dirac delta function. Consider a function that is 0 everywhere except the narrow region-E<x<+ where its value is a constant B. This too could be normalized, What would be the relationship between s and B, and what would happen to B as s approaches 0? (What we get is not exactly the Dirac delta function, but the distinction involves comparing infinities, a dangerous business that we will avoid.)

(d) As we see, the two "exceptional" functions may be viewed as limits of normalizable ones. In those limits, they are also complementary to each other in terms of their position and momentum uncertainties. Without getting into calculations, describe how they are complementary.

Question: the operator for angular momentum about the z-axis in spherical polar coordinate is -i.find the function f that would have a well-defined z-component of angular momentum.

When is the temporal part of the wave function 0? Why is this important?

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