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The photoelectric and photovoltaic effects | Physics | Khan Academy

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    - If you shine particular kinds
    of light on certain metals,
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    electrons will be ejected.
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    We call this the photoelectric
    effect because light is photo
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    and electrons being ejected is electric.
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    And this was one of the key experiments
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    that actually helped us
    discover a completely
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    new model of light.
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    But how exactly you ask,
    well, let's find out.
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    What's interesting here is
    that this effect depends on
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    the color of light.
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    For example, if this metal
    was, say potassium, okay,
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    then if you shine blue light,
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    then we will get electrons being ejected,
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    photoeletric effect happens.
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    But if you were to shine
    red light on potassium,
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    we will not get
    photoeletric effect at all.
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    Regardless of how bright you make it.
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    Even if you were to make
    it blindingly bright,
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    we will not get photoeletric effect.
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    This is what puzzled physicists.
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    I mean, think about the
    model over here we have atoms
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    with electron clouds
    over here and the nucleus
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    at the center, okay?
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    When you shine light,
    the energy of the light
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    gets transferred to the electrons
    and they're able to escape
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    the clutches of the nucleus and go out.
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    But why can't that happen
    over here with red light?
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    Think about it, I'm shining bright light,
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    very high intensity, incredible
    amount of energy over here,
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    and yet electrons are not
    able to absorb it and get out.
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    Why does the photoeletric
    effect depend on the color?
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    That was a big question
    that didn't make any sense.
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    So what do we do over here?
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    Well, we do more careful experiments.
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    First, let's only look at the color
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    and then think about the
    brightness later, okay.
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    So what is color representing
    electromagnetic waves?
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    Remember that color
    basically depends on the wave
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    length of light.
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    For example, red color is
    the wavelength of light
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    could be somewhere around 650 nanometers.
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    What we find is that at 650 nanometers
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    we don't get any photoelectric
    effect for potassium.
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    We don't know why, but
    now what we can do is
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    let's reduce the wavelength
    and see what happens
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    if I keep reducing the
    wavelength, and let's say
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    I come to orange light of 600 nanometers,
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    see I've reduced it.
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    I still get no photoeletric
    effect, I don't know why,
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    but I'm just doing an experiment.
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    This is an observation, okay?
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    I keep reducing.
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    I keep reducing the wavelength
    until I hit 541 nanometers.
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    At this point, I now start
    seeing photoeletric effect,
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    and in this particular case,
    electrons are barely ejected
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    from the metal.
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    That's why I've drawn very
    tiny arrow marks over here,
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    they have hardly have any kinetic energy.
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    I just get some photoeletric effect
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    and then if I reduce it even
    further, that's where I get my
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    blue light at about say 500 nanometers.
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    These are rough numbers, okay?
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    At 500 nanometers, I now
    get photoelectric effect,
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    but the electrons coming
    out with even more energy.
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    What happens if I reduce it even further?
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    I find that electrons are coming
    out with even more energy.
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    So what's our observation over here?
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    We see that if we lower the
    wavelength, we get more energy
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    for the electrons coming out over here.
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    We can also talk in terms of frequency.
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    Remember, bigger the wavelength,
    smaller the frequency,
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    because if you have big wavelength,
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    there are less waves passing per second.
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    So this is low frequency
    and this is high over here.
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    So we can say when it comes to frequency,
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    more the frequency, more
    the energy of the electrons.
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    And you also have some kind
    of a cutoff over here, right?
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    So for example, if the wave
    length is above 541 nanometers
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    for potassium, for potassium,
    if it's above 5 41 nanometers,
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    no photoeletric effect, only below it,
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    we will get photoelectric effect.
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    And so every metal will
    have its own cutoff.
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    We call that the threshold wavelength,
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    or you can also say threshold frequency.
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    But the whole idea is if
    the wavelength is below
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    that threshold wavelength
    only then you get
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    photoelectric effect, if
    it's about you won't get it.
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    Different metals have
    different threshold wavelengths
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    and similarly different
    threshold frequencies.
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    So that's the effect of
    wavelength of frequency.
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    We see that the wavelength
    of the frequency controls
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    the energy with with
    the electrons come out
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    and that cannot be explained as to why.
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    Why does the wavelength of
    the frequency control it?
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    Why am I not getting photoeletric effect?
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    If it's about the threshold wavelength,
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    it doesn't make any sense.
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    But anyways, the next
    question could be for us,
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    how does the brightness
    affect this whole thing?
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    Does it have any effect?
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    The answer is yes.
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    Remember, brightness or the
    intensity of light is basically
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    how big the valleys and
    the peaks are, right?
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    So if you were to make the light brighter,
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    then it will look somewhat like this.
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    You can imagine it this way.
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    This is brighter light, okay?
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    Now what we find is that we
    get more electrons, okay?
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    It doesn't change the energy
    with these electrons come out.
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    See they're coming out with
    much the same energy as before,
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    but we now get more electrons.
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    Of course, if you're above
    the threshold wavelength,
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    you'll not get photo
    photoelectric effect at all,
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    regardless of the brightness.
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    It doesn't matter, okay?
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    So if you decrease the
    brightness or intensity,
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    you get less electrons.
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    If you increase the intensity,
    you get more electrons.
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    So intensity only controls
    the number of electrons,
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    but it's the wavelength of
    the frequency that controls
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    the energy with visual electrons come out,
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    it also controls whether we
    get photoeletric effect or not.
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    The big question was why the
    wave model just cannot explain
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    this because according to wave model,
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    you should get photoeletric
    effect for all colors
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    of light, right?
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    If you make light bright
    enough, electrons should be able
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    to absorb it and just get,
    you know just get admitted.
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    But that doesn't happen.
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    And this is why physicists
    back then were puzzled
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    and we were desperately in
    need of an answer for this.
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    So what did we do?
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    Well, to explain these
    observations, we came up with
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    a completely brand new model of light.
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    Instead of thinking of
    light as waves that carry
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    energy continuously and that can transfer
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    energy continuously,
    we thought maybe light
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    is made of discrete packets
    of energy, not waves,
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    but packets of energy,
    which we call photons.
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    And then light is being
    absorbed by say electrons.
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    You also absorb it as packets.
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    You'll either absorb no
    light or you'll absorb
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    one packet of light or
    two packets of light
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    and so on and so forth,
    nothing in between.
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    We call this discrete,
    which is exactly opposite
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    of what happens in wave model,
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    there you can absorb continuously.
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    Okay, so how does this explain
    the photoelectric effect,
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    the observations over here?
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    Well, let's see.
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    The key thing over here is
    that the energy of the photons
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    or the packets notice
    depends on the color.
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    If you're dealing with long wavelength
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    or low frequency light,
    then we have less energy
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    of the packet, the
    photons have less energy.
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    And if you're dealing
    with short wavelength
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    or high frequency light, you
    can see that the packets have
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    more energy.
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    So shorter the wavelength
    or more the frequency,
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    there is more energy in the packet.
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    There is a relationship between
    energy and the wavelength,
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    which we'll not get into.
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    But lemme just give you
    some rough numbers over here
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    because the numbers is
    gonna help us over here.
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    So here are some numbers.
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    So it turns out that if
    you consider red light
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    of 650 nanometers, the energy
    of the packet, the energy
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    of the photon is about 1.9 electron volt.
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    Yeah, maybe wondering,
    shouldn't we be measuring
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    energy in joules?
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    Well, joule turns out to
    be a big unit of energy.
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    So we use a smaller unit of energy,
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    which we call electron volts.
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    Don't worry too much
    about the units over here,
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    it's just the numbers.
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    You can see these
    packets have tiny energy,
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    but this packet has much bigger energy.
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    2.8 electron volts, you
    can see that, right.
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    Now for potassium it turns out,
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    if you want to pluck an electron,
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    if electron needs to be
    ejected, the minimum energy
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    that you need is about 2.3 electron volts.
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    This is for potassium.
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    Now is a great time for
    you to pause the video
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    and see if you can try and come up
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    with an explanation over here.
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    Alright, let's see.
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    The big idea over here is
    that if you want to knock off
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    an electron, I mean like you know,
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    make that electron escape,
    then a single photon
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    should have at least this much energy.
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    If the photons do not have
    at least this much energy,
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    then the electron will absorb it,
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    but it's not enough to escape,
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    and so it'll just reradiate it back.
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    And therefore, if you
    have consider red light,
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    it does not have a single photon,
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    does not carry enough energy.
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    And that's the reason
    why electrons are not
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    getting injected over here.
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    And that's why these lights are unable
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    to give you photoelectric effect.
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    Over here, we have just enough energy
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    for photoelectric effect
    and therefore electrons
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    barely make it out over here,
    because all of the energy
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    is used up in just
    releasing the electrons.
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    There's hardly any energy left over here,
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    so there'll be hardly moving.
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    But over here, notice you
    have more than the necessary
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    energy over here and therefore
    some residual energy is left.
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    And so electrons after coming
    out have some extra energy
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    remaining that goes out as kinetic energy.
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    And since this has even more energy,
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    each photon has even more
    energy while electrons now
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    eject with even more kinetic energy,
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    'cause there's more residual
    energy after getting ejected.
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    But what about the intensity?
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    Well, if you increase the
    intensity in this model,
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    we are increasing the number
    of photons, that's it.
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    Over here notice if a
    single photon does not have
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    enough energy, then I don't
    care how many photons you shine,
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    it's just not going to work.
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    That's why here I will still not get any,
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    you know, photoelectric effect.
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    But over here now I'm shining
    more number of photons,
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    so more electrons can absorb that energy
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    and therefore more electrons
    can escape per second.
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    And that's why I get
    more electrons over here,
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    putting it all together.
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    Since the wave of the
    frequency decides the energy
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    of an individual photon that
    decides the kinetic energy,
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    shorter the wavelength,
    stronger, more is the energy
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    of the photon and more
    is the kinetic energy.
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    If the wavelength is
    bigger and it's too big,
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    the energy of the photon is very tiny,
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    it'll not be able to knock off anything
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    and you'll not get any
    photoelectric effect.
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    And since intensity is
    basically the number of photons,
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    if you have more number of
    photons, you'll get more number
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    of electrons coming out.
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    But over here, it doesn't matter
    how many photons you shine,
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    and therefore it doesn't
    matter what the brightness is,
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    you will not get photoelectric effect.
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    Beautiful, isn't it?
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    So wait, does this mean
    that light is not a wave?
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    It's actually particles?
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    Well, not quiet.
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    You see certain phenomena
    of light like diffraction
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    or interference means that
    light must have wave properties
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    and certain other phenomenon
    like photoelectric effect,
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    black body radiation, scattering of light,
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    and other such effects makes us believe
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    that light must also
    have the particle nature,
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    the photon nature, which
    means a light must have
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    a dual nature, both particle and waves.
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    It's not that light
    sometimes behaves as waves
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    and sometimes wears as particle.
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    No, no, no.
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    Light has both wave and particle nature.
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    And if you're wondering, well,
    how does that make any sense?
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    How can something be both waves
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    and particles at the same time?
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    Well, unfortunately, there's
    no way to really visualize it
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    because in our macroscopic world,
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    we don't have any experience
    of things having both wave
  • 10:50 - 10:52
    and particle nature.
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    But this is one of the reasons
    why sometimes when we are
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    showing photons, we show it this way
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    with a tiny wave packet,
    but this doesn't mean
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    that the photons are wiggling up and down.
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    Okay, that's a misconception
    that I used to have.
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    It's not like that.
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    A better way to sort of
    think about this is that
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    light is not a wave in
    the traditional sense.
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    It's not a particle in
    the traditional sense,
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    it's a brand new object,
    which we don't have
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    experience within our daily life.
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    This object has both wave properties
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    and particle properties,
    and we call such an object,
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    a quantum object.
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    Now this sounds very theoretical, right?
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    But there are so many
    applications of the fact
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    that light is a quantum object.
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    Let me tell you one of them, okay?
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    Now, in photoelectric effect from light,
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    we get electrons ejected, right?
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    Now there's a very similar,
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    slightly different effect
    called (indistinct)
  • 11:43 - 11:45
    when you shine light,
    you can generate voltage.
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    We call such an effect,
    a photovoltaic effect.
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    Now, the way that works is we
    need to first create a crystal
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    in which there's an already
    inbuilt electric field.
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    It's possible to do that.
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    We'll not get too much
    details of how we build
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    such crystals, but using semiconductors,
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    we can build crystals like that.
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    We don't have to hook it up
    to any battery or anything.
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    It'll have an inbuilt electric field.
  • 12:09 - 12:11
    The crystals is built in
    such a way that one side
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    of the crystal has slightly
    different properties compared
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    to another side of the crystal.
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    And because of the
    difference in properties,
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    an electric field gets built up.
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    Now the important point is
    there are electrons everywhere,
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    but if you focus on this
    region, there are a lot of
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    electrons, but they're
    all bonded and they're not
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    free to move.
  • 12:28 - 12:30
    So even if there's an electric
    field pushing on them,
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    they cannot move because
    they're stuck in bonds.
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    You can imagine that this is
    like the sea of electrons.
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    They're all kind of
    fixed inside the crystal,
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    they cannot move.
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    But if we shine light in this region,
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    and if the light has
    the suitable frequency
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    or the suitable wavelength,
    then the electrons can absorb
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    that energy, but it won't get emitted.
  • 12:51 - 12:53
    Okay, that's the difference over here.
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    In photo effect, it gets emitted.
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    But here, instead of getting emitted,
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    it just gets enough
    energy to escape the bond.
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    And as a result, now it's
    free to move and therefore
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    it'll get accelerated to
    the left in this diagram,
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    because electric field to the
    right electrons are negatively
  • 13:06 - 13:08
    charged the experience of force
    in the opposite direction.
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    And as a result, it will
    now come to the left side
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    and it'll leave behind a gap.
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    Now, other electrons, under
    electrons, which are bonded,
  • 13:18 - 13:21
    can swoop into this gap,
    which makes the gap go
  • 13:21 - 13:24
    to the right, and then the
    other electrons can swoop into
  • 13:24 - 13:25
    this gap and so on and so forth.
  • 13:25 - 13:29
    So it kind of feels that this
    gap, this latency will move in
  • 13:29 - 13:31
    to the other side.
  • 13:31 - 13:34
    This way, a lot of electrons
    and a lot of vacancies
  • 13:34 - 13:36
    can be created.
  • 13:36 - 13:38
    And so look, if you can
    complete this circuit,
  • 13:38 - 13:41
    electrons would love
    to go from here to here
  • 13:41 - 13:42
    through that external circuit.
  • 13:42 - 13:46
    In other words, there
    is a voltage created.
  • 13:46 - 13:49
    And so what we have done is
    we have used the energy from
  • 13:49 - 13:53
    light to create voltage
    photovoltaic effect.
  • 13:53 - 13:58
    If you put a lot of these
    together, we create a solar panel.
  • 13:59 - 14:01
    That's how solar cells
    and solar panels work.
  • 14:01 - 14:05
    They work on the photovoltaic effect.
  • 14:05 - 14:07
    Whether you consider them
    on the roofs of the houses
  • 14:07 - 14:10
    or you consider the ones
    which are in the spacecraft,
  • 14:10 - 14:12
    they all use the same idea.
  • 14:12 - 14:14
    At the end of the day,
    we are using the fact
  • 14:14 - 14:17
    that light is a quantum
    object to harness the power
  • 14:17 - 14:19
    of light, which we get from the sun.
Title:
The photoelectric and photovoltaic effects | Physics | Khan Academy
Description:

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Video Language:
English
Team:
Khan Academy
Duration:
14:20

English subtitles

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