(a) what voltage must be applied to an X-ray tube to obtain0.0100 fm wavelength X-rays for use in exploring the details of nuclei? (b) What is unreasonable about this result? (c) Which assumptions are unreasonable or inconsistent?

Short Answer

Expert verified

a. Hence, the minimum voltage required to accelerate the electron is 1.24 x 1011eV.

b. The unreasonable thing about the answer is the requirement of extremely high voltage.

c. We are considering electron to generate such a small wavelength. Since the electrons are very light, the momentum will be very small and, hence, making wavelength such small will require huge energy.

Step by step solution

01

Definition of wavelength

A waveform signal that is carried in space or down a wire has a wavelength, which is the separation between two identical places (adjacent crests) in the consecutive cycles.

02

The minimum voltage required to accelerate the electron

(a)

The wavelength is \(\lambda = 0.0100\,{\rm{fm}} = 0.0100 \times {10^{ - 15}}\,{\rm{m}}\)

Hence, the energy of the photon is

\({E_\lambda } = \frac{{hc}}{\lambda }\)

Here h is the plank constant (6.62 x 10-34J.s); c is the speed of light (\(3 \times {10^8}\,{\rm{m/s}}\)) and \(\lambda \) is the wavelength (\(0.0100 \times {10^{ - 15}}\,{\rm{m}}\)).

Substitute all the value in the above equation.

\(\begin{array}{c}{E_\lambda } = \frac{{\left( {6.62 \times {{10}^{ - 34}}\,{\rm{J}}{\rm{.s}}} \right)\left( {3 \times {{10}^8}\,{\rm{m/s}}} \right)}}{{\left( {0.0100 \times {{10}^{ - 15}}\,{\rm{m}}} \right)}}\\ = 1.98 \times {10^{ - 8}}\,{\rm{J}}\\ = \frac{{1.98 \times {{10}^{ - 8}}\,{\rm{J}}}}{{1.6 \times {{10}^{ - 19}}\,{\rm{J/eV}}}}\\ = 1.24 \times {10^{11}}\,{\rm{eV}}\end{array}\)

Hence, the minimum voltage required to accelerate the electron is 1.24 x 1011eV.

03

Unreasonable result

(b)

The unreasonable thing about the answer is the requirement of extremely high voltage.

04

Step 4: Assumptions are unreasonable or inconsistent

(c)

We are considering electron to generate such a small wavelength. Since the electrons are very light, the momentum will be very small and, hence, making wavelength such small will require huge energy.

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Most popular questions from this chapter

Integrated Concepts

In a Millikan oil-drop experiment using a setup like that in Figure 30.9, a 500 - V potential difference is applied to plates separated by 2.50 cm.

(a) What is the mass of an oil drop having two extra electrons that is suspended motionless by the field between the plates?

(b) What is the diameter of the drop, assuming it is a sphere with the density of olive oil?

How do the allowed orbits for electrons in atoms differ from the allowed orbits for planets around the sun? Explain how the correspondence principle applies here.

Particles called muons exist in cosmic rays and can be created in particle accelerators. Muons are very similar to electrons, having the same charge and spin, but they have a mass 207 times greater. When muons are captured by an atom, they orbit just like an electron but with a smaller radius, since the mass in\({{\bf{a}}_{\bf{B}}}{\bf{ = }}\frac{{{{\bf{h}}^{\bf{2}}}}}{{{\bf{4}}{{\bf{\pi }}^{\bf{2}}}{{\bf{m}}_{\bf{e}}}{\bf{kq}}_{\bf{e}}^{\bf{2}}}}{\bf{ = 0}}{\bf{.529 \times 1}}{{\bf{0}}^{{\bf{ - 10}}}}{\bf{\;m is 207}}{{\bf{m}}_{\bf{e}}}\)

(a) Calculate the radius of then = 1 orbit for a muon in a uranium ion\(\left (Z = 92).

(b) Compare this with the7.5 - fmradius of a uranium nucleus. Note that since the muon orbits inside the electron, it falls into a hydrogen-like orbit. Since your answer is less than the radius of the nucleus, you can see that the photons emitted as the muon falls into its lowest orbit can give information about the nucleus.

If atoms exist, why can’t we see them with visible light?

The wavelength of the four Balmer series lines for hydrogen are found to be 410.3, 434.2, 486.3, and 656.5 nm. What average percentage difference is found between these wavelength numbers and those predicted by\[\frac{{\bf{1}}}{{\bf{\lambda }}}{\bf{ = R}}\left( {\frac{{\bf{1}}}{{{\bf{n}}_{\bf{f}}^{\bf{2}}}}{\bf{ - }}\frac{{\bf{1}}}{{{\bf{n}}_{\bf{i}}^{\bf{2}}}}} \right){\bf{?}}\]It is amazing how well a simple formula (disconnected originally from theory) could duplicate this phenomenon.

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