19 Quantum Flashcards

You may prefer our related Brainscape-certified flashcards:
1
Q

Definition of photoelectric effect

A

The emission of photoelectrons from a metal surface when electromagnetic radiation of a sufficiently high frequency is incident on it.

How well did you know this?
1
Not at all
2
3
4
5
Perfectly
2
Q

How to tell if photoelectric emission has occurred at the emitter?

A

The ammeter registers a current due to the electrons from the emitter reaching the collector and completing the circuit.

How well did you know this?
1
Not at all
2
3
4
5
Perfectly
3
Q

What is the purpose of adjusting the variable DC supply?

A

The potential of the collector is made more positive or negative with respect to the emitter to accelerate or decelerate the emitted electrons.

How well did you know this?
1
Not at all
2
3
4
5
Perfectly
4
Q

Relationship between stopping potential and intensity of incident light

A

The two are independent.

How well did you know this?
1
Not at all
2
3
4
5
Perfectly
5
Q

Relationship between photoelectric current and intensity of incident light

A

The two are proportional.

How well did you know this?
1
Not at all
2
3
4
5
Perfectly
6
Q

Definition of a photon

A

A photon is a small discrete quanta of electromagnetic energy from a beam of light.

How well did you know this?
1
Not at all
2
3
4
5
Perfectly
7
Q

Formula for energy of a single photon E

A

E = hf = hc/λ

Planck constant h = 6.63 x 10^-34
Electron-volt eV = 1.6 x 10^-19 (same as elementary charge)
E is proportional to f.

How well did you know this?
1
Not at all
2
3
4
5
Perfectly
8
Q

Definition of work function Φ

A

The minimum amount of energy that will remove an electron from the surface of the metal.

How well did you know this?
1
Not at all
2
3
4
5
Perfectly
9
Q

Formula for work function Φ

A

Φ = hf0 = hc/λ0

How well did you know this?
1
Not at all
2
3
4
5
Perfectly
10
Q

Definition of threshold frequency f0

A

The minimum frequency of an incident photon that will remove an electron from the surface of the metal.

Note:
A photon’s energy cannot be shared among multiple electrons, one electron can only absorb one photon.

How well did you know this?
1
Not at all
2
3
4
5
Perfectly
11
Q

Einstein’s equation for photoelectric effect (energy conservation)

A

E = Φ + Ekmax

How well did you know this?
1
Not at all
2
3
4
5
Perfectly
12
Q

Definition of stopping potential Vs

A

The minimum potential difference between the metal and collector that will prevent an ejected photoelectron from reaching the collector.

How well did you know this?
1
Not at all
2
3
4
5
Perfectly
13
Q

Formula for stopping potential, Vs

A

Ekmax = 1/2 mvmax^2 = eVs

Graph of stopping potential against frequency of incident light:
y = Vs
x = f
m = h/e
y-intercept = -Φ/e
x-intercept = f0
How well did you know this?
1
Not at all
2
3
4
5
Perfectly
14
Q

Formula for intensity of incident radiation I

A

I = power/area = (energy/time)/area = [(Np/t)(hf)]/A = (Np/t)(hf/A)

Np/t = rate of photon arrival on metal surface

How well did you know this?
1
Not at all
2
3
4
5
Perfectly
15
Q

Definition of saturation current

Formula for saturation current isat

A

At saturation current, all photoelectrons emitted will reach the collector

isat = Q/t = Nee/t = (Ne/t)e

Ne/t = rate of photoelectron emission from metal surface

How well did you know this?
1
Not at all
2
3
4
5
Perfectly
16
Q

Explanation for existence of threshold frequency

A

Wave theory:
Photoelectric emission occurs for any frequency of monochromatic incident light.
Energy transfer is continuous, electrons accumulate energy until it has sufficient to escape.

Quantum theory:
Energy of incident photon must be larger than work function of metal for photoelectric emission to occur.
Increasing intensity of monochromatic incident light only increases number of photons arriving on metal surface per unit time, energy of each photon is not affected.

17
Q

Explanation for no time delay in emission of photoelectrons

A

Wave theory:
At low intensity light, there is less energy, electrons need time to accumulate sufficient energy to escape metal surface, causing time lag between emission of photoelectrons and incidence of light on surface.

Quantum theory:
For frequencies of incident photons more than threshold frequency of target metal, energy of photon is sufficient to overcome work function of metal to be ejected.
Photoelectrons are emitted immediately after light is incident on metal surface regardless of intensity.
Electrons cannot accumulate energy through absorption of multiple photons, each can only absorb one.

18
Q

Explanation for stopping potential independent of intensity of incident light

A

Wave theory:
Increasing incident light intensity causes greater amount of incident energy on surface, giving liberated electrons more energy.
Maximum kinetic energy possessed by ejected photoelectrons increases, stopping potential increases.

Quantum theory:
Increasing incident light intensity at constant frequency causes higher photon arrival rate.
Energy of each incident photon is unchanged.
Each photoelectron is liberated by one photon, maximum kinetic energy possessed by ejected photoelectron is unchanged, stopping potential is unchanged.

19
Q

Explanation for photocurrent proportional to intensity of incident light

A

Wave theory:
Intensity of wave is energy incident per unit area per unit time.
More incident energy liberates more electrons, increasing photocurrent.

Quantum theory:
Higher intensity of incident light of constant frequency causes greater number of photons arriving on metal surface per unit time.
More ejected photoelectrons per unit time, increasing photocurrent.

20
Q

Formula for de Broglie wavelength

A

λ = h/p = h/mv

21
Q

How does the existence of line spectra provides evidence for existence of discrete electron energy levels in isolated atoms

A

Each line on the line spectrum corresponds to a single wavelength, hence a single frequency of light
Energies of photons emitted are discrete
Since energy level of photons correspond to energy difference between two energy levels in an atom,
Energy levels of electrons within the atom are discrete as well

22
Q

Emission line spectrum

A

When a high potential difference is applied across a discharge tube containing the gas at low pressure the atoms of the gas are excited through inelastic collisions
Excited atoms are highly unstable and will quickly de-excite to lower energy states
Excited atoms emit photons while de-exciting

23
Q

Absorption line spectrum

A

White light consisting of photons of a continuous range of frequencies passes through a discharge tube containing the gas at low pressure and temperature
Photons which have the energies that correspond to the energy difference between two discrete energy levels are absorbed,
causing electrons to be excited from ground state to higher levels and subsequently de-excite, emmiting photons of similar energies to those absorbed randomly in all directions.
Hence the intensity of these photons is reduced, forming dark lines

24
Q

Heisenberg uncertainty principle

A

The heisenberg Uncertainty Principle states that it is impossible to measure the exact position and momentum at the same time

△x △p ≥ h