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  • In this video, we're going to talk about Planck's constant and blackbody radiation.

  • Now you might be wondering, what is blackbody radiation?

  • Well, any object with a temperature above 0 Kelvin is going to emit some form of electromagnetic radiation.

  • As the temperature increases, the energy of that radiation will increase as well.

  • So imagine if you have a metal, and you heat the metal.

  • As the temperature of the metal goes up, eventually, you'll notice that the metal will have a reddish glow to it.

  • And as you continue to heat up the metal, as the temperature increases, it's going to appear yellow, and then maybe even whitish.

  • Whenever you increase the temperature of an object, the molecules in that object will vibrate with more energy.

  • And the oscillations of the electric charges in those molecules can emit electromagnetic radiation.

  • So let's say you have an atom.

  • Let's say this is a hydrogen atom.

  • This is the first energy level.

  • The second energy level.

  • Let's say this is the third energy level.

  • When an electron in this atom, when it absorbs energy, it can jump to a higher energy level.

  • Now, when that electron returns to its original state, or if it drops to a lower energy level, it's going to emit electromagnetic energy.

  • And so as these electrons, as they oscillate back and forth, they can absorb and emit electromagnetic energy.

  • Now, the energy that is carried by a photon is a multiple of this value, hf.

  • So we're going to put an n, where n is an integer, h is the Planck's constant, f is frequency.

  • The frequency is measured in hertz, or s to the minus 1, and h is Planck's constant, which is 6.626 times 10 to the negative 34 joules times seconds.

  • Now, this equation tells us something very important, and that is that the energy of a photon is quantized.

  • It's not continuous, it can only have discrete values.

  • So it can't be just any value, but it's a multiple of hf.

  • It can be 1hf, it can be 2hf, 3hf, but nothing in between that.

  • So the energy of a photon can only exist in discrete values, it can't take any value.

  • So thus we could say that energy is quantized.

  • Now let's work on some problems.

  • Calculate the energy of a photon with a frequency of 4 times 10 to the 14 hertz.

  • So we could use this formula to get the answer.

  • So we're only dealing with a single photon, so n is going to be 1.

  • Planck's constant, that's 6.626 times 10 to the negative 34, and this is joules times seconds.

  • The frequency is 4 times 10 to the 14 hertz.

  • And hertz is seconds to the minus 1, or 1 over seconds.

  • And so we can see the unit, seconds, will cancel.

  • And this is going to leave behind the unit joules.

  • And so the energy is going to be 2.65 times 10 to the negative 19 joules.

  • So that's the energy of this particular photon.

  • Now what is the energy of a red photon with a wavelength of 700 nanometers?

  • Whenever light has a wavelength of about 700 nanometers, it's going to appear red.

  • Now, in order to do this one, we need an additional formula.

  • The wavelength of light times frequency is equal to the speed of light.

  • So what we need to do first is we need to calculate the frequency.

  • The frequency is the speed of light divided by the wavelength.

  • And the speed of light, which is the same for all types of electromagnetic radiation in a vacuum, is 3 times 10 to the 8 meters per second.

  • The wavelength is 700 nanometers, and a nanometer is 10 to the minus 9 meters.

  • So the unit meters will cancel.

  • Giving us the unit 1 over seconds, which is frequency in hertz.

  • So 3 times 10 to the 8 divided by 700 times 10 to the negative 9.

  • That's going to give us a frequency of 4.286 times 10 to the 14 hertz.

  • Now that we know the frequency, we can calculate the energy of the red photon.

  • So since we're only dealing with a single photon, and there's one, and then we have Planck's constant.

  • And then we have the frequency, 4.286 times 10 to the 14.

  • I'm going to write 1 over seconds for the unit.

  • So I got 2.84 times 10 to the negative 19 joules.

  • So that is the energy of a single red photon.

  • That's how you can calculate it.

  • Now, let's work on one more problem.

  • What is the energy of 5 blue photons with a wavelength of 450 nanometers?

  • So this problem is very similar to number 2.

  • The only difference is we have an n value of 5.

  • So let's begin by calculating the frequency.

  • The frequency is going to be the speed of light divided by the wavelength.

  • That's 3 times 10 to the 8 meters per second divided by 450 nanometers or 450 times 10 to the negative 9 meters.

  • So we're going to cancel the unit meters just like we did before.

  • So this works out to be 6.67 times 10 to the 14 hertz.

  • So now that we know the frequency, let's calculate the energy of the photon.

  • So E is equal to n h f. n is 5 since we're dealing with 5 photons, 5 blue photons. h is always going to be the same, Planck's constant.

  • That's not going to change.

  • So that's just a number you're going to have to commit to memory.

  • And we have a frequency of this value.

  • So 6.67 times 10 to the 14 times Planck's constant times 5 will give us this answer.

  • So the energy of the 5 blue photons combined is going to be 2.21 times 10 to the negative 18 joules.

  • So now you know how to calculate the energy of a single photon or a group of photons if you know the frequency of the photons or their wavelength.

In this video, we're going to talk about Planck's constant and blackbody radiation.

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Planck's Constant and BlackBody Radiation

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    kevin posted on 2024/10/02
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