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What is the longest-wavelength EM radiation that can eject a photoelectron from silver, given that the binding energy is 4.73 eV? Is this in the visible range?

Short Answer

Expert verified

The longest wavelength of EM radiation is 263nm and the EM radiation is not in visible range.

Step by step solution

01

The longest-wavelength EM radiation can eject a photoelectron

The kinetic energy of the electron is given by

KEe = hf -BE ...(1)

HereKEe is the kinetic energy, his the plank constant, f is the frequency of the EM radiation and is the binding energy.

Now we know that the wavelength of EM radiation is given by

\[\lambda=\frac{c}{f}\] ...(2)

Where cis the speed of light.

So equation becomes,

\[K{E_e}=\frac{{hc}}{\lambda}-BE\] ...(3)

02

Determination of the maximum wavelength

For wavelength to be maximum, the kinetic energy of the electron must be zero. Hence we have

The given value is

\begin{aligned}BE=4.73\,{\rm{eV}}\\=(4.73\,{\rm{eV}})\left({1.60\times{{10}^{19}}\,\frac{{\rm{J}}}{{{\rm{eV}}}}} \right)\\= 7.57 \times {10^{ - 19}}\,{\rm{J}}\end{aligned}

We also know:

\begin{aligned}h=6.63\times{10^{-34}}\,{\rm{J}}{\rm{.s}}\\c=3\times{10^8}\,{{\rm{m}}\mathord{\left/{\vphantom{{\rm{m}}{\rm{s}}}}\right\{\rm{s}}}\end{aligned}

h = 6.63×10-34 J s

c = 3×108m/s

Substitute all the values in the above equation, and we get:

\begin{aligned}\lambda=\frac{{\left({6.63\times{{10}^{ -34}}\,{\rm{J}}{\rm{.s}}} \right)\left({3\times {{10}^8}\,{{\rm{m}} \mathord{\left/{\vphantom {{\rm{m}} {\rm{s}}}} \right\{\rm{s}}}}\right)}}{{\left({7.57\times{{10}^{-19}}\,{\rm{J}}}\right)}}\\=2.63\times{10^{-7}}\,{\rm{m}}\\ = 263\,{\rm{nm}}\end{aligned}

Hence the maximum wavelength of the EM radiation that can remove electrons from silver is 263nm

Therefore the longest-wavelength EM radiation can eject a photoelectron 263

Hence, the EM radiation is not in the visible range.

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Most popular questions from this chapter

Suppose the velocity of an electron in an atom is known to an accuracy of 2.0 x 103 (reasonably accurate compared with orbital velocities). What is the electron’s minimum uncertainty in position, and how does this compare with the approximate 0.1 nm size of the atom?

(a) Calculate the energy in \({\rm{eV}}\) of an \({\rm{IR}}\) photon of frequency \({\rm{2}}{\rm{.00 \times 1}}{{\rm{0}}^{{\rm{13}}}}{\rm{ Hz}}\).

(b) How many of these photons would need to be absorbed simultaneously by a tightly bound molecule to break it apart?

(c) What is the energy in \({\rm{eV}}\) of a \(\gamma \) ray of frequency \({\rm{3}}{\rm{.00 \times 1}}{{\rm{0}}^{{\rm{20}}}}{\rm{ Hz}}\)?

(d) How many tightly bound molecules could a single such \(\gamma \) ray break apart?

Question: Red light having a wavelength of \({\rm{700 nm}}\) is projected onto magnesium metal to which electrons are bound by \({\rm{3}}{\rm{.68 eV}}\). (a) Use \({\rm{KEe = hf-- BE}}\) to calculate the kinetic energy of the ejected electrons. (b) What is unreasonable about this result? (c) Which assumptions are unreasonable or inconsistent?

Question: (a) Calculate the energy in \({\text{eV}}\) of an \({\text{IR}}\) photon of frequency \({\text{2}}{\text{.00 \times 1}}{{\text{0}}^{{\text{13}}}}{\text{ Hz}}\).

(b) How many of these photons would need to be absorbed simultaneously by a tightly bound molecule to break it apart?

(c) What is the energy in \({\text{eV}}\) of a \(\gamma \) ray of frequency \({\text{3}}{\text{.00 \times 1}}{{\text{0}}^{{\text{20}}}}{\text{ Hz}}\)?

(d) How many tightly bound molecules could a single such \(\gamma \) ray break apart?

Calculate the frequency in hertz of a \(1.00 - MeV\)\(\gamma \)-ray photon.

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