What is the product of uncertainties determined in Exercise 60 and 61? Explain.

Short Answer

Expert verified

The product of uncertainty in position and momentum is 2, which is in accordance with the uncertainty principle.

Step by step solution

01

The concepts and formulas used to solve the given problem.

The uncertainty principle states that the position and momentum of an atom cannot be measured simultaneously. It gives uncertainty in position if we have uncertainty in momentum.

The expression for the uncertainty principle.

ΔxΔph2

Here,Δxis the change in position, Δpis the change in momentum and h is the reduced Planck's constant. Write the expression for uncertainty in position.

Δx=12h2mk1/4 …… (1)

Here, xis the uncertainty in position, h is reduced Planck's constant, m is the mass and k is the constant.

The expression for uncertainty in momentum.

Δp=h2(mk)1/4 …… (2)

Here, pis the uncertainty in momentum, is reduced Planck's constant, m is the mass and k is the constant.

02

Step 2:Product

Multiply equation (1) and (2).

ΔxΔp=12h2mk1/4h2(mk)1/4

=h2

The product of uncertainties is equal to h2which is in accordance with the Uncertainty principle.

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Most popular questions from this chapter

Sketchψ(x) . Would you expect this wave function to be the ground state? Why or why not?

It is possible to take the finite well wave functions further than (21) without approximation, eliminating all but one normalization constant C . First, use the continuity/smoothness conditions to eliminate A, B , andG in favor of Cin (21). Then make the change of variables z=x-L/2 and use the trigonometric relations

sin(a+b)=sinacosb+cosasinband

cos(a+b)=cosacosb-sinasinbon the

functions in region I, -L/2<z<L/2. The change of variables shifts the problem so that it is symmetric about z=0, which requires that the probability density be symmetric and thus that ψ(z)be either an odd or even function of z. By comparing the region II and region III functions, argue that this in turn demands that (α/k)sinkL+coskL must be either +1 (even) or -1 (odd). Next, show that these conditions can be expressed, respectively, as αk=tankL2 and αk=-cotkL2. Finally, plug these separately back into the region I solutions and show that

ψ(z)=C×{eα(z+L/2)          z<L/2coskzcoskL2          -L/2<z<L/2e-α(z-L/2)          z>L/2


or

ψ(z)=C×{eα(z+L/2)          z<L/2-sinkzsinkL2          -L/2<z<L/2e-α(z-L/2)          z>L/2

Note that Cis now a standard multiplicative normalization constant. Setting the integral of |ψ(z)|2 over all space to 1 would give it in terms of kand α , but because we can’t solve (22) exactly for k(or E), neither can we obtain an exact value for C.

Write out the total wave functionψ(x,t).For an electron in the n=3 state of a 10nm wide infinite well. Other than the symbols a and t, the function should include only numerical values?

Where would a particle in the first excited state (first above ground) of an infinite well most likely be found?

Show that the uncertainty in the momentum of a ground state harmonic oscillator is 2mk1/4.

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