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Daniella Garcia-Loos
Saarah Hasan
Daniella Garcia-Loos
Saarah Hasan
The idea that light exhibits particle properties was first suggested by Einstein when he showed that light transferred energy just like a particle(E=mc^2). Compton expanded the groundwork of this idea further in 1923 when he showed that light has momentum and can undergo elastic collisions. From multiple physicists' work, we now know that light behaves like a stream of photons, which can be illustrated by the photoelectric effect:
The photoelectric effect is the phenomenon in which electrons are emitted from a metal surface when it is exposed to light.
Here are some key points about the photoelectric effect at an AP Physics level:
When light shines on a piece of metal, some of the photons enter the surface of the metal, collide with the atoms and get absorbed, giving energy to the metal’s surface electrons. If this energy is great enough, the electrons can jump from their bound state and fly off. These electrons that break free are known as photo-electrons.
There would be a large time delay between the point when the light shined on the metal and when the electrons would break off.
Increasing the intensity of light would cause the photo-electrons to be ejected with greater kinetic energy, since a wave’s energy is related to its intensity.
All frequencies of light would cause photoelectrons to eject, as long as the intensity was high enough. What actually happened:
Electrons broke off within a few billionths of a second after getting shined on.
Increasing the intensity of light didn’t increase the photoelectron’s kinetic energy. More electrons flew off as the intensity increased, but there was a certain maximum photoelectron kinetic energy.
For each metal, there was a specific threshold frequency, f0. If the light’s frequency was lower than the f0, then no electrons flew off. The intensity of the light wasn’t a factor. The energy of a photon can be found by:
E=hf
where h = Planck’s constant = 6.63 ∗ 10^−34 J*s
f = frequency
Remember that:
f=c/λ
E=hf➡️
E=hc/λ
In order for the metal’s surface electrons to break free, a certain amount of energy has to be transferred to them. This is known as the metal’s work function(Φ). If an electron absorbed a photon with an energy (E) greater than Φ, then it would eject with a maximum kinetic energy of: K(max)=E-Φ ➡️ Kmax= hf-Φ
The threshold frequency can be expressed as: f_0=Φ/h
Some things to keep in mind:
B) frequency of light is increased
C) intensity of light is decreased
D) intensity of light is increased
E) velocity of light is increased
B) 2.0 eV
C) 2.7 eV
D) 4.0 eV
E) 6.0 eV
B) B
C) C
D) D
E) E
C) C
D) D
E) E
B) III only
C) I and II only
D) II and III only
E) I, II, and III
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Daniella Garcia-Loos
Saarah Hasan
Daniella Garcia-Loos
Saarah Hasan
The idea that light exhibits particle properties was first suggested by Einstein when he showed that light transferred energy just like a particle(E=mc^2). Compton expanded the groundwork of this idea further in 1923 when he showed that light has momentum and can undergo elastic collisions. From multiple physicists' work, we now know that light behaves like a stream of photons, which can be illustrated by the photoelectric effect:
The photoelectric effect is the phenomenon in which electrons are emitted from a metal surface when it is exposed to light.
Here are some key points about the photoelectric effect at an AP Physics level:
When light shines on a piece of metal, some of the photons enter the surface of the metal, collide with the atoms and get absorbed, giving energy to the metal’s surface electrons. If this energy is great enough, the electrons can jump from their bound state and fly off. These electrons that break free are known as photo-electrons.
There would be a large time delay between the point when the light shined on the metal and when the electrons would break off.
Increasing the intensity of light would cause the photo-electrons to be ejected with greater kinetic energy, since a wave’s energy is related to its intensity.
All frequencies of light would cause photoelectrons to eject, as long as the intensity was high enough. What actually happened:
Electrons broke off within a few billionths of a second after getting shined on.
Increasing the intensity of light didn’t increase the photoelectron’s kinetic energy. More electrons flew off as the intensity increased, but there was a certain maximum photoelectron kinetic energy.
For each metal, there was a specific threshold frequency, f0. If the light’s frequency was lower than the f0, then no electrons flew off. The intensity of the light wasn’t a factor. The energy of a photon can be found by:
E=hf
where h = Planck’s constant = 6.63 ∗ 10^−34 J*s
f = frequency
Remember that:
f=c/λ
E=hf➡️
E=hc/λ
In order for the metal’s surface electrons to break free, a certain amount of energy has to be transferred to them. This is known as the metal’s work function(Φ). If an electron absorbed a photon with an energy (E) greater than Φ, then it would eject with a maximum kinetic energy of: K(max)=E-Φ ➡️ Kmax= hf-Φ
The threshold frequency can be expressed as: f_0=Φ/h
Some things to keep in mind:
B) frequency of light is increased
C) intensity of light is decreased
D) intensity of light is increased
E) velocity of light is increased
B) 2.0 eV
C) 2.7 eV
D) 4.0 eV
E) 6.0 eV
B) B
C) C
D) D
E) E
C) C
D) D
E) E
B) III only
C) I and II only
D) II and III only
E) I, II, and III
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