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A hydrogen atom (with the Bohr radius of half an angstrom) is situated

between two metal plates 1 mm apart, which are connected to opposite terminals of a 500 V battery. What fraction of the atomic radius does the separation distance d amount to, roughly? Estimate the voltage you would need with this apparatus to ionize the atom. [Use the value of in Table 4.1. Moral:The displacements we're talking about are minute,even on an atomic scale.]

Short Answer

Expert verified

The separation distance amounts to 4.6×10-6 times the atomic radius and the voltage required to ionize the atom is 108V.

Step by step solution

01

Given data

The distance between metal plates is: x=1mm=1mm×1m1000mm=0.001m.

The emf of the battery is: V=500V.

02

Values of fermi constant, electric charge and atomic radius

The Fermi constant is:α=7.32×10-41C×m2/V .

The electric charge is: e=1.6×10-19C.

The atomic radius is: R=0.5×10-10m.

03

Separation distance and voltage required to ionize atom

The expression for electric field is:

E=V/x

Substitute the values of in the above equation and get

E=500V/0.001m=5×105V/m

The expression for the dipole moment is,

p=αE=ed

Thus,

d=αEe

Substitute the values in the above equation and get

d=7.34×10-41C.m2/V×5×105V/m1.6×10-19C=2.2×10-16m

The ratio of the separation distance to the atomic radius is

r=d/R

Substitute the values in the above equation and get

r=2.2×10-16m0.5×10-10m

Thus, the separation distance is 4.6×10-6 times the atomic radius.

The expression for the voltage required to ionize the atom is

Vi=Rexα

Substitute the values in the above equation and get

Vi=0.5×10-10m×1.6×10-19C×0.001m7.32×10-41C.m2/V=108V

Thus, the voltage required to ionize the atom is 108V.

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Most popular questions from this chapter

A point dipole p is imbedded at the center of a sphere of linear dielectric material (with radius R and dielectric constant εr). Find the electric potential inside and outside the sphere.

role="math" localid="1658748385913" [Aanswer:pcosθ4πε°ù21+2r3R3εr-1εr+2,r≤R:pcosθ4πε0r23εr+2,r≥R]

Suppose the field inside a large piece of dielectric is E0, so that the electric displacement is D0=ε0E0+P.

(a) Now a small spherical cavity (Fig. 4.19a) is hollowed out of the material. Find the field at the center of the cavity in terms of E0and P. Also find the displacement at the center of the cavity in terms of D0and P. Assume the polarization is "frozen in," so it doesn't change when the cavity is excavated. (b) Do the same for a long needle-shaped cavity running parallel to P (Fig. 4.19b).

(c) Do the same for a thin wafer-shaped cavity perpendicular to P (Fig. 4.19c). Assume the cavities are small enough that P,E0, and D0are essentially uniform. [Hint: Carving out a cavity is the same as superimposing an object of the same shape but opposite polarization.]

Show that the energy of an ideal dipole p in an electric field E isgiven by

U=−p⋅E∈

When you polarize a neutral dielectric, the charge moves a bit, but the total remains zero. This fact should be reflected in the bound charges σb and ÒÏb· Prove from Eqs. 4.11 and 4.12 that the total bound charge vanishes.

Question:A (perfect) dipole p is situated a distance z above an infinite grounded conducting plane (Fig. 4.7). The dipole makes an angle θwith the perpendicular to the plane. Find the torque on p . If the dipole is free to rotate, in what orientation will it come to rest?

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