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Physics 6C Photons Prepared by Vince Zaccone For Campus Learning Assistance Services at UCSB

Physics 6C

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Physics 6C. Photons. Prepared by Vince Zaccone For Campus Learning Assistance Services at UCSB. Photoelectric Effect. metal plate. incoming light. Here is the basic setup for the experiment. Light shines on the metal plate, and the electrons absorb that light energy. e -. e -. e -. e -. - PowerPoint PPT Presentation

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Page 1: Physics 6C

Physics 6C

Photons

Prepared by Vince ZacconeFor Campus Learning Assistance Services at UCSB

Page 2: Physics 6C

Prepared by Vince ZacconeFor Campus Learning Assistance Services at UCSB

incoming light

e-

e-

e-

e-

e-

e-

e-

e-metal plate

Photoelectric Effect

Here is the basic setup for the experiment.

Light shines on the metal plate, and the electrons absorb that light energy.

Page 3: Physics 6C

Prepared by Vince ZacconeFor Campus Learning Assistance Services at UCSB

e-

e-

e-

e-

e-

e-

e-

e-

metal plate

Photoelectric Effect

Here is the basic setup for the experiment.

Light shines on the metal plate, and the electrons absorb that light energy.

Sometimes the electrons gain enough energy to escape and they are ejected from the metal plate, creating a current in the circuit.

Surprisingly, whether or not the electrons are freed does not depend on the brightness of the light.

Instead, it depends on the FREQUENCY of the incoming light.

ejected electron

Page 4: Physics 6C

Prepared by Vince ZacconeFor Campus Learning Assistance Services at UCSB

e-

e-

e-

e-

e-

e-

e-

e-

metal plate ejected

electron

This result is not easily explained with the wave theory of light. Instead, if we think of light as ‘photons’ it makes some sense. Each photon of light has an energy (proportional to its frequency), and the electrons can only interact with one photon at a time. This is why the electrons are not ejected by frequencies that are too low, even when the light is very bright.

As soon as the frequency of the photon is above some threshold, the electrons can get ejected, with any leftover energy going toward their kinetic energy.

Here is the basic setup for the experiment.

Light shines on the metal plate, and the electrons absorb that light energy.

Sometimes the electrons gain enough energy to escape and they are ejected from the metal plate, creating a current in the circuit.

Surprisingly, whether or not the electrons are freed does not depend on the brightness of the light.

Instead, it depends on the FREQUENCY of the incoming light.

Photoelectric Effect

Page 5: Physics 6C

Prepared by Vince ZacconeFor Campus Learning Assistance Services at UCSB

e-

e-

e-

e-

e-

e-

e-

e-

metal plate

Here are the relevant formulas:

Energy of a photon:ejected electron

chfhEphoton

hfKmax

Φ, the ‘work function’ of the metal, tells you how much energy is required to free the electron. Think of it as a binding energy if you like. Each metal has a different value for work function.

seV1014.4hsJ1063.6h

15

34

Planck’s constant:

Leftover kinetic energy:

One more thing you will need to do is convert between Joules and electron-volts:

J106.1eV1 19

Photoelectric Effect

Page 6: Physics 6C

Prepared by Vince ZacconeFor Campus Learning Assistance Services at UCSB

Example: The maximum wavelength an electromagnetic wave can have and still eject an electron from a copper surface is 264nm. What is the work function of a copper surface?

Page 7: Physics 6C

Prepared by Vince ZacconeFor Campus Learning Assistance Services at UCSB

Example: The maximum wavelength an electromagnetic wave can have and still eject an electron from a copper surface is 264nm. What is the work function of a copper surface?

The given wavelength is right at the threshold for ejecting electrons, so there is no leftover kinetic energy when they are freed from the metal plate. This means the energy of the photon must be equal to the work function.

Page 8: Physics 6C

Prepared by Vince ZacconeFor Campus Learning Assistance Services at UCSB

Example: The maximum wavelength an electromagnetic wave can have and still eject an electron from a copper surface is 264nm. What is the work function of a copper surface?

The given wavelength is right at the threshold for ejecting electrons, so there is no leftover kinetic energy when they are freed from the metal plate. This means the energy of the photon must be equal to the work function.

eV7.4m10264)103)(seV1014.4(chfhE 9

sm815

photon

Page 9: Physics 6C

Prepared by Vince ZacconeFor Campus Learning Assistance Services at UCSB

Example: White light, with frequencies ranging from 4.0x1014 Hz to 7.9x1014 Hz, is incident on a potassium surface. Given that the work function of potassium is 2.24 eV, finda) the maximum kinetic energy of photoelectrons ejected from this surface andb) the range of frequencies for which no electrons are ejected.

Page 10: Physics 6C

Prepared by Vince ZacconeFor Campus Learning Assistance Services at UCSB

Example: White light, with frequencies ranging from 4.0x1014 Hz to 7.9x1014 Hz, is incident on a potassium surface. Given that the work function of potassium is 2.24 eV, finda) the maximum kinetic energy of photoelectrons ejected from this surface andb) the range of frequencies for which no electrons are ejected.

a) Since photon energy increases with frequency, we should use 7.9x1014 Hz in the formula.

hfKmax

Page 11: Physics 6C

Prepared by Vince ZacconeFor Campus Learning Assistance Services at UCSB

Example: White light, with frequencies ranging from 4.0x1014 Hz to 7.9x1014 Hz, is incident on a potassium surface. Given that the work function of potassium is 2.24 eV, finda) the maximum kinetic energy of photoelectrons ejected from this surface andb) the range of frequencies for which no electrons are ejected.

a) Since photon energy increases with frequency, we should use 7.9x1014 Hz in the formula.

eV03.1eV24.2)Hz109.7)(seV1014.4(KhfK

1415max

max

Page 12: Physics 6C

Prepared by Vince ZacconeFor Campus Learning Assistance Services at UCSB

Example: White light, with frequencies ranging from 4.0x1014 Hz to 7.9x1014 Hz, is incident on a potassium surface. Given that the work function of potassium is 2.24 eV, finda) the maximum kinetic energy of photoelectrons ejected from this surface andb) the range of frequencies for which no electrons are ejected.

a) Since photon energy increases with frequency, we should use 7.9x1014 Hz in the formula.

eV03.1eV24.2)Hz109.7)(seV1014.4(KhfK

1415max

max

b) If the photon energy is below the work function, no electrons will be ejected. This gives us the cutoff frequency:

Hz104.5seV1014.4eV24.2fhf 1415

Page 13: Physics 6C

Prepared by Vince ZacconeFor Campus Learning Assistance Services at UCSB

Example: White light, with frequencies ranging from 4.0x1014 Hz to 7.9x1014 Hz, is incident on a potassium surface. Given that the work function of potassium is 2.24 eV, finda) the maximum kinetic energy of photoelectrons ejected from this surface andb) the range of frequencies for which no electrons are ejected.

a) Since photon energy increases with frequency, we should use 7.9x1014 Hz in the formula.

eV03.1eV24.2)Hz109.7)(seV1014.4(KhfK

1415max

max

b) If the photon energy is below the work function, no electrons will be ejected. This gives us the cutoff frequency:

Hz104.5seV1014.4eV24.2fhf 1415

So the range of frequencies that do not eject electrons is 4.0x1014 Hz to 5.4x1014 Hz.

Page 14: Physics 6C

Prepared by Vince ZacconeFor Campus Learning Assistance Services at UCSB

Example: Zinc and cadmium have photoelectric work functions of 4.33 eV and 4.22 eV, respectively. If both metals are illuminated by white light (wavelengths between 400nm and 700nm), which one gives off photoelectrons with the greater maximum kinetic energy?

Page 15: Physics 6C

Prepared by Vince ZacconeFor Campus Learning Assistance Services at UCSB

Example: Zinc and cadmium have photoelectric work functions of 4.33 eV and 4.22 eV, respectively. If both metals are illuminated by white light (wavelengths between 400nm and 700nm), which one gives off photoelectrons with the greater maximum kinetic energy?

Assuming electrons are ejected from both metals, the answer should be cadmium, because it has a lower work function – less energy to overcome means more leftover kinetic energy.Is this a good assumption?

Page 16: Physics 6C

Prepared by Vince ZacconeFor Campus Learning Assistance Services at UCSB

Example: Zinc and cadmium have photoelectric work functions of 4.33 eV and 4.22 eV, respectively. If both metals are illuminated by white light (wavelengths between 400nm and 700nm), which one gives off photoelectrons with the greater maximum kinetic energy?

Assuming electrons are ejected from both metals, the answer should be cadmium, because it has a lower work function – less energy to overcome means more leftover kinetic energy.Is this a good assumption?No – we need to check to see if any electrons are ejected at all.

Page 17: Physics 6C

Prepared by Vince ZacconeFor Campus Learning Assistance Services at UCSB

Example: Zinc and cadmium have photoelectric work functions of 4.33 eV and 4.22 eV, respectively. If both metals are illuminated by white light (wavelengths between 400nm and 700nm), which one gives off photoelectrons with the greater maximum kinetic energy?

Assuming electrons are ejected from both metals, the answer should be cadmium, because it has a lower work function – less energy to overcome means more leftover kinetic energy.Is this a good assumption?No – we need to check to see if any electrons are ejected at all.The most energetic photon available in the given range will be the 400nm light (short wavelength = high energy)

Page 18: Physics 6C

Prepared by Vince ZacconeFor Campus Learning Assistance Services at UCSB

Example: Zinc and cadmium have photoelectric work functions of 4.33 eV and 4.22 eV, respectively. If both metals are illuminated by white light (wavelengths between 400nm and 700nm), which one gives off photoelectrons with the greater maximum kinetic energy?

Assuming electrons are ejected from both metals, the answer should be cadmium, because it has a lower work function – less energy to overcome means more leftover kinetic energy.Is this a good assumption?No – we need to check to see if any electrons are ejected at all.The most energetic photon available in the given range will be the 400nm light (short wavelength = high energy)

eV1.3m10400)103)(seV1014.4(chE 9

sm815

photon

Page 19: Physics 6C

Prepared by Vince ZacconeFor Campus Learning Assistance Services at UCSB

Example: Zinc and cadmium have photoelectric work functions of 4.33 eV and 4.22 eV, respectively. If both metals are illuminated by white light (wavelengths between 400nm and 700nm), which one gives off photoelectrons with the greater maximum kinetic energy?

Assuming electrons are ejected from both metals, the answer should be cadmium, because it has a lower work function – less energy to overcome means more leftover kinetic energy.Is this a good assumption?No – we need to check to see if any electrons are ejected at all.The most energetic photon available in the given range will be the 400nm light (short wavelength = high energy)

eV1.3m10400)103)(seV1014.4(chE 9

sm815

photon

This is not above the work function of either metal, so no electrons are ejected. That makes the answer to the original question “neither”.

Page 20: Physics 6C

Prepared by Vince ZacconeFor Campus Learning Assistance Services at UCSB

Example: Zinc and cadmium have photoelectric work functions of 4.33 eV and 4.22 eV, respectively. If both metals are illuminated by UV light with wavelength 275 nm, calculate the maximum kinetic energy of electrons ejected from each surface.

Page 21: Physics 6C

Prepared by Vince ZacconeFor Campus Learning Assistance Services at UCSB

Example: Zinc and cadmium have photoelectric work functions of 4.33 eV and 4.22 eV, respectively. If both metals are illuminated by UV light with wavelength 275 nm, calculate the maximum kinetic energy of electrons ejected from each surface.

eV30.0eV22.4m10275)103)(seV1014.4(K

eV19.0eV33.4m10275)103)(seV1014.4(K

hcK

9sm815

Cdmax,

9sm815

Znmax,

max

This time let’s just calculate the answers:

Page 22: Physics 6C

Prepared by Vince ZacconeFor Campus Learning Assistance Services at UCSB

Compton Scattering

A photon strikes a stationary electron and scatters off at some angle θ. The electron recoils and carries away some of the energy of the photon, resulting in a photon with less energy that the original (so a longer wavelength).

The shift in the wavelength can be calculated.

This experiment was important because is showed definitively that light can not be thought of as a strictly wavelike phenomenon. The wave theory does not explain Compton’s result.

Photons, or treating the light as a particle when it interacts with matter, yield a simple explanation.

Page 23: Physics 6C

Prepared by Vince ZacconeFor Campus Learning Assistance Services at UCSB

Compton Scattering

Example: X-rays of wavelength λ=0.120nm are scattered from a carbon block. What is the wavelength of a scattered photon detected at an angle of 45°?

m0 =mass of electron=9.11x10-31kg

Page 24: Physics 6C

Prepared by Vince ZacconeFor Campus Learning Assistance Services at UCSB

Only a few photons – not a very clear picture

Photograph - one photon at a time

Page 25: Physics 6C

Prepared by Vince ZacconeFor Campus Learning Assistance Services at UCSB

Only a few photons – not a very clear picture

Photograph - one photon at a time

Page 26: Physics 6C

Prepared by Vince ZacconeFor Campus Learning Assistance Services at UCSB

Only a few photons – not a very clear picture …more photons

Photograph - one photon at a time

Page 27: Physics 6C

Prepared by Vince ZacconeFor Campus Learning Assistance Services at UCSB

Only a few photons – not a very clear picture …more photons Even more photons – we

can tell what the picture is, but it’s still grainy.

Photograph - one photon at a time

Page 28: Physics 6C

Prepared by Vince ZacconeFor Campus Learning Assistance Services at UCSB

Only a few photons – not a very clear picture …more photons Even more photons – we

can tell what the picture is, but it’s still grainy.

…more photons

Photograph - one photon at a time

Page 29: Physics 6C

Prepared by Vince ZacconeFor Campus Learning Assistance Services at UCSB

Only a few photons – not a very clear picture …more photons Even more photons – we

can tell what the picture is, but it’s still grainy.

…more photons …more photons

Photograph - one photon at a time

Page 30: Physics 6C

Prepared by Vince ZacconeFor Campus Learning Assistance Services at UCSB

Only a few photons – not a very clear picture …more photons Even more photons – we

can tell what the picture is, but it’s still grainy.

…more photons …more photons Final picture – can’t see the individual photons anymore.

Photograph - one photon at a time

Page 31: Physics 6C

Prepared by Vince ZacconeFor Campus Learning Assistance Services at UCSB

Double-Slit experiment one photon at a time

Page 32: Physics 6C

Prepared by Vince ZacconeFor Campus Learning Assistance Services at UCSB

Double-Slit experiment one photon at a time

Page 33: Physics 6C

Prepared by Vince ZacconeFor Campus Learning Assistance Services at UCSB

Double-Slit experiment one photon at a time

Page 34: Physics 6C

Prepared by Vince ZacconeFor Campus Learning Assistance Services at UCSB

Double-Slit experiment one photon at a time

Page 35: Physics 6C

Prepared by Vince ZacconeFor Campus Learning Assistance Services at UCSB

Double-Slit experiment one photon at a time