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36C3 - Climate Modelling

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    36C3 preroll music
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    Herald: ... so I'm looking forward and I
    hope you are, too. I am looking forward to
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    be told the difference between..
    laughs ... we will all be told the
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    difference between an input model and a
    climate model, and we are going to be told
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    this difference by karlabyrinth.
    There you go.
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    applause
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    karlabyrinth: Thank you. Hello and
    welcome, everyone. I would like to see my
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    slides. Are the slides ...? Ah, OK.
    laughs nice. So welcome, everyone, to my
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    talk about Climate Modeling - the science
    behind climate reports. First of all, I
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    will shortly introduce myself and what I
    do. I work at the UFZ. That's the
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    Helmholtz Center for Environmental
    Research in Leipzig and I work for the ESM
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    project, which is short for 'advanced earth
    system' modelling capacity. I am also a PhD
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    student at the University of Potsdam and I
    am part of the developer team for the
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    middle scale hydrologic model, which is an
    impact model. And I'm also a scientist for
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    future and an artist. So what this talk is
    about? This talk is partitioned into three
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    sections, mainly. First is the
    introduction where I will introduce some
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    nomenclature like what is weather, what is
    climate and what we can say about
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    predictions. For example, why we can't
    tell the weather in three years but we can
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    say something about the climate, and what
    are climate models. Then the second part
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    will be the longest, the science behind
    warming graphs. I will show you a graph
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    that's typically shown when people tell
    you about climate change, and I will
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    explain that graph in detail and what is
    behind it. The third part would be
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    installing an impact model to your local
    PC if there is time. If there is no time I
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    will skip that. And in the end, there is, as
    always, a summary and conclusion. So
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    starting with the introduction. Weather is
    defined as the physical state of the
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    atmosphere at a given time whilst climate
    is averaged weather. Most of the time a
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    time period of 30 years is taken for that
    averaging but also other time periods
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    could be taken. So, while, the main
    question was, while we
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    are not able to predict whether at a
    specific date in a
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    decade, for example, let's say the 27th of
    December in 50 years or so. Why does it
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    still make sense to propose general trends
    for the climate? That is a question that
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    often arises when... and I'll answer that.
    So, first of all, it is about average.
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    Average cloud coverage gives us
    information on average reflection. And
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    average reflection is ... has an impact on
    the warmth on the earth. And the same is
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    true for another scenario. For example,
    average precipitation - meaning rain or snow
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    and temperature - has an impact on
    vegetation and vegetation influences the
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    carbon cycle. And that again influences
    the warming or cooling and that has an
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    influence on the ice coverage. And that,
    again, on the reflection. So there are
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    lots of processes that are connected to
    each other and if we know something about
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    the average of some of these physical
    state of the atmosphere, we can say
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    something about the climate trends. So the
    question is, what is a climate model? And
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    the AR5 defines a climate model is a
    numerical representation of the climate
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    system. The AR5 is a source I will cite
    quite often. So I have one slide
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    with the whole citation. It's the fifth
    IPCC report. IPCC is the
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    Intergovernmental Panel on Climate Change
    and the fifth assessment report is, yeah,
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    so AR5 is the abbreviation for fifth
    assessment report. But coming back to a
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    climate model. So a climate model could,
    for example, be a GCM - a general
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    circulation model - which is a global
    climate model that usually consists of an
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    ocean and atmosphere circulation. An RCM
    is not a GCM but it's a regional climate
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    model, meaning a climate model at a
    limited area, and mainly it has a higher
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    resolution. And for it is at a limited
    area, that usually means that there is
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    some input and output going in because
    it's not a closed system. And an impact
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    model again has usually a higher
    resolution in time and space and it's not
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    a climate model, but it's for simulating
    extreme weather events
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    like floods. So if you want to build a
    dam or a dike and you want to know how
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    high this dike or dam should be, then you
    would usually run an impact model that
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    gives you information about water height
    over decades or longer or so. And then
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    you would decide on the height. So this is
    the use for impact models. So that's for
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    the introduction part. Now I come to the
    main part and I will start with a
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    question: is it proven? Or with a climate
    graph. As that, I will show you a graph, a
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    typical image people would show you when
    they address climate change. This graph
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    has an x-axis with a time scale and you
    see it's reaching far into the future. And
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    it also has three or four regions
    and the first region is only in the past.
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    And the y-axis is the global surface
    temperature change, meaning how much
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    degrees in Celsius or in Kelvin, if it's
    different it's the same, we will have in
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    future or we had already. And then, you
    see several lines and different colors and
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    with the names RCP something. And I will
    explain all the numbers and everything
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    about that graph because it's a pretty
    important graph. So first of all, I will
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    tell you... no, no. I will tell you
    something about the numbers and
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    uncertainties. The uncertainties are the
    transparent colors behind the lines. I
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    will tell you something about the
    representative concentration pathways,
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    which is short RCP, and so it's reflecting
    the colors of the lines. I will tell you
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    something about the source of the graphs.
    So where does this graph actually come
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    from? So I will tell you something about
    the assessment report. And first of all, I
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    will answer the question: is it proven or
    is there scientific evidence that we will
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    face that climate change? So, you will see
    that graph quite often. First of all, I
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    took a definition for proof, for
    scientific evidence, from Wikipedia. The
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    strength of scientific evidence is
    generally based on the results of
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    statistical analysis and the strength of
    scientific controls.
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    Meaning, you make an experiment over and
    over again and you change basically some
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    influences on the experiments where you
    want to know that this does not influence
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    the output. So you can narrow it down and
    know what is the source of your results
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    and so you can prove a physical law or
    something. Yeah, I took this comic from
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    xkcd because it's a nice... it's somehow
    connected. So there is a person who pulls
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    a trigger and then gets struck by a bolt
    or some something. Something bad happens,
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    for example climate change. And then,
    yeah, there are two scenarios. For
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    example, a person usually would decide,
    okay, I would not pull the lever again.
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    But scientists usually or more often would
    say, okay, maybe: Does that happen every
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    time if I do so? Because yeah, that's
    basically how you prove something. That's
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    experiments. But in case of climate
    change, even scientists say you shouldn't.
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    Although it's pretty interesting for us
    from a scientific perspective. But the
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    problem is we only have one earth. We
    cannot do this experiment very often,
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    except we had a time machine. Then we
    could go back, but we haven't so we
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    shouldn't do that experiment. And that's
    something scientists before, long ago in
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    1957 said already: "Human beings are now
    carrying out a large-scale geophysical
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    experiment of a kind that could not have
    happened in the past nor be reproduced in
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    the future." So another question is, yeah,
    if you ask this question if it is proven
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    or that it probably is not happening or so
    to climate deniers, they usually would
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    tell you: Okay, maybe it's not happening.
    And the other side would take the position
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    and ask you, okay, if you stand in front
    of a road and you want to cross the road
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    and there's a car approaching very fast,
    would you cross that road? Because it
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    could happen that the car stops or makes a
    U-turn or something. But well, usually it
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    doesn't. And sadly, we know lots about
    this experiment, because it's done very
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    often before. We know
    something about traffic, and that it's
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    pretty dangerous. So let's change the
    factors a little so that we don't know so
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    much about that situation. Let's say a
    cube approaches us with a high velocity on
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    something that is maybe not a road. Would
    you still cross that something? The answer
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    is you still probably wouldn't. And why
    wouldn't you do so although you know
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    nothing about this situation? Well, you do
    know something. You know conservation of
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    the momentum, which is a physical law you
    know about. So you have a situation, you
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    know not so much about. You have never had
    an experience before, but you still are
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    able to make some assumptions because you
    know the physical laws behind it. And
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    that's basically the same we do with, in
    fact, in the context of climate. So we
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    have, let's say, just an earth and the sun
    and the sun has some radiation and that
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    comes to the earth and gets partially
    reflected and the earth radiates itself
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    because it has some temperature. We know
    something about this sun. We know the
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    solar insolation. And we know parts of the
    light is reflected. And the factor that is
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    reflected is usually called albedo. And so
    the reflected energy is albedo times the
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    solar insulation and albedo is something
    about 30 percent. And we know then that
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    the light that is absorbed must be all the
    remaining energy. So the energy of the
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    surface is 1 minus albedo times the solar
    insolation. Then knowing Stefan-Boltzmann
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    law for energy emissions where the
    temperature goes in to the power of four
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    and with the Stefan-Boltzmann constant we
    can actually find find out the surface
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    temperature which then is derived to -19.5
    degrees Celsius. Well, we know, probably
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    we know, that the earth is much warmer,
    and that's because our model in this case,
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    which is maybe a climate model, is far too
    simple. So we change something about that.
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    We add atmosphere, and atmosphere has some
    interesting impact. So atmosphere has some
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    trace greenhouse gases,
    for example CO2 but also H2O, ozone,
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    methane, O2 and nitrous oxide. And these
    greenhouse gases reflect the radiation of
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    earth back to earth, partially. Meaning
    the atmosphere has a transparency and this
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    transparency we call t is something
    between 15 percent and 30 percent. So it's
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    not fixed. And that's another interesting
    fact. The atmosphere emits energy, which
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    we call j atmos, and that goes out in
    space and to earth and the energy that
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    goes into the atmosphere is 1 minus the
    transparency times the energy. So we know
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    two equations. The first is the energy
    that goes into the atmosphere also goes
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    out of the atmosphere. The second is that
    the surface energy of the earth
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    is the term we had before,
    1 minus albedo times the solar
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    insolation plus the one part of the energy
    that is reflected by the atmosphere. And
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    so we have two formulas, two equations
    with two unknowns and with the Stefan-
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    Boltzmann law from before we can derive
    the surface temperature, which is 15
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    degrees of Celsius. And that actually is
    not so far from what it actually is. In
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    2000 it was measured that the surface
    temperature is 14.5 degrees. So, I did
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    this for a specific t which is 22.5
    percent but when we change that t a little
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    to, for example, 20 percent, so we add
    more CO2 because, for example, we would
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    add a factory that would do carbon
    emissions. Then the transparency goes down
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    and the temperature rises to, for example,
    16.6 degrees in case of 20 percent. This
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    is also a very old knowledge. So this is
    maybe a little much on a slide but it is
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    still very interesting because it is
    copied directly from a paper that was
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    published from Svante Arrhenius in 1896
    already. And it's on the influence of
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    carbon acid in the air upon the
    temperature of the ground. And carbon acid
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    is the old term for carbon dioxide. So if
    we have a look to the percentage... So he
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    investigated: What if we change
    carbon dioxide? So what is the impact of
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    our behavior? Let's say carbon dioxide
    in our atmosphere would
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    double, so would increase by a factor of
    2, then the average temperature rise in
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    Leipzig in December, so I choose the
    region for Leipzig, would be 6.1 degrees.
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    Well, that's probably a little high, but
    what we can't see is already that
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    Arrhenius back then already knew that
    there is a seasonal impact on
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    climate... that climate change is seasonal
    and also spatial. So it is not just one...
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    not the average temperature is the only
    interesting knowledge we get. So
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    Arrhenius said something like the
    temperature in case of carbon acid doubled
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    would be around four to six degrees. And
    the current models predict something like
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    an increase of two to four degrees for
    that scenario. So there is maybe overlap
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    already with that simple model from back
    then. So, then I come to the question...
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    a climate model represents physical laws.
    That's what we learned. Where do the
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    uncertainties come from? So if we know all
    the physics laws and we would just
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    calculate everything with this physics
    laws, why are there even uncertainties?
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    And there are some reasons for that. For
    example, the initial conditions is one
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    main source of uncertainties, meaning how
    is the current state of the climate system
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    now? How fast does something move?
    Where are the clouds exactly?
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    And so on. We don't
    know these precise initial
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    conditions and therefore errors
    occure. Second, would be the
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    resolution of a model. So the
    temporal and spatial step length, meaning
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    we can't... always represent our
    climate system with differential equations
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    and we approximate everything. We have not
    the movement of every molecule but we have
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    some average on cells. And if we increase
    the resolution then usually the
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    uncertainties go down. But sometimes they
    even don't for some question, for some
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    questions it's better to have a lower
    resolution. But mostly it's better to have
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    a higher. Then, truncation, so we have
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    computational limits. And lack of
    understanding, for example, clouds. Clouds
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    are not understood pretty well. And when I
    read the fifth assessment report, I found
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    a sentence a little amusing:
    Climate model... Clouds in climate models
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    usually tend to rain too early. Yeah, so
    but if you know all these sources of
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    uncertainty, why is there no such thing as
    the one best climate model? Meaning, why
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    can't we go to the highest resolution and
    to the best... the best computer we get
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    and do everything just in the best way and
    then we would have our best climate model?
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    And there are some reasons for that. For
    example, the so-called dynamic core,
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    including the method for differential
    equations or something like grids.
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    For example, if we have a triangular
    grid or a rectangular grid. On a
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    rectangular grid we usually can
    calculate faster but on a triangular grid
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    we could, for example, increase the
    resolution locally. That might be
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    differences. And both have advantages and
    disadvantages. Also, the parametrization:
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    parameters in our last slide were for
    example the t and the albedo which will
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    probably be not the final parameters
    because they are derived from other
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    parameters, but physical laws or something
    are often represented by rules with
  • 21:01 - 21:07
    parameters, and these parameters can be
    estimated. And they can be calibrated with
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    different error measures.
    And there this is another reason for
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    uncertainties and differences in climate
    models and then their schemes. For
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    example, there are different formulations
    of physical processes, for example, that
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    again, clouds. And last the truncation,
    again, we can also decide how we limit due
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    to our lack of computational power. So,
    yeah, what do we do? We investigate all
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    the models we have. So there are different
    climate models that are representing our
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    climate and we take all the models that
    match certain conditions - I come to that
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    later - and we average the output and then
    we
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    get a climate prediction and also that
    uncertainty band you see. So what climate
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    models do we investigate? They are so-
    called coordinated GCMS. So climate models
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    are compared in so-called coupled model
    intercomparison projects in different
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    phases. These coupled model
    intercomparison projects are called CMIP
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    4, 5 and 6. So there might have been four
    earlier ones. But currently, for the AR6,
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    so for the sixth assessment report CMIP6
    investigated. And I showed you on the
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    map the research centers which took part
    in CMIP6, so which take part in the 6th
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    assessment report. These research centers
    are mainly specialized research centers,
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    university and metereological offices, but
    generally it's open for any institution to
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    participate, as long as they follow a
    protocol for their contribution, where
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    there are some rules so you cannot just do
    anything. These institutions
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    need to produce variables for a set of
    defined experiments and a historical
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    simulation from 1850 to present. This blue
    part is a link, so if you go to my slides
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    afterwards, you can see these variables
    you need to reproduce and then you can do
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    something like this. So we have a graph
    here again. On the x axis, we see again a
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    timescale that reaches from 1850 to today.
    And on the y axis we again see the
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    temperature anomaly or the temperature
    difference between.. so, exactly the
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    temperature difference, so how much the
    earth has warmed up. We see CMIP3 and CMIP5
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    compared, which were the models that were
    investigated for the AR5. So we see a
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    band. This uncertainty with the yellow and
    bluish and the background and then we see
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    these two lines, the blue and the red one
    from CMIP3 and CMIP5 and then we see the
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    black one. And that is what actually was
    observed. And we see that this differs
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    quite a lot. And that's due to there was
    only investigated the natural forces,
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    meaning excluded what the human did. And
    if we
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    also put the human forces into it, then
    it's quite matching. And that is the best
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    kind of proof we can get. And again, I
    said we investigate the physical laws and
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    the physical laws were actually results of
    scientific experiments. And so, yeah,
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    there's this kind of proof. And yeah. So
    maybe a little addition. There are also
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    other coordinated model intercomparisons
    projects that are outside of the IPCC and
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    so the ones that are inside the IPCC
    where the scientific focus is on a
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    subtopic, on something like land surface
    for example (and that's what I do). And
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    they're also published work
    outside from IPCC. So back to the graph.
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    We talked about the part: Is it proven?
    And I hope I convinced you that it is. And
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    now I will talk about the sources of the
    graph. So I talked a lot about the IPCC.
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    The IPCC, the Intergovernmental Panel on
    Climate Change, publishes reports. So for
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    example, the 5th assessment report and
    what you see here is part of the cover.
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    But there have been 4 ones before, as the
    name 5th suggests, the first assessment
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    report FAR was published in 1990. The
    second SAR in 1995. Then there was the TAR
  • 26:51 - 26:56
    and then for the 4th assessment report
    they changed the name scheme for some
  • 26:56 - 27:04
    reason to AR4 and then there was AR5,
    which I'm talking about. The IPCC consists
  • 27:04 - 27:09
    of several working groups, including
    Working Group 1 to 3, providing the
  • 27:09 - 27:15
    assessment reports and I mainly focus on
    the assessment report from a working group
  • 27:15 - 27:20
    1, which investigates the scientific
    aspects of the climate system and climate
  • 27:20 - 27:28
    change. But there is also a working group
    investigating on vulnerability and
  • 27:28 - 27:34
    economic impact. And the third one on the
    options of limiting greenhouse gas
  • 27:34 - 27:44
    emissions and others. So I totally show
    you a history of the climate models. In
  • 27:44 - 27:51
    something like the 70s, climate models
    were investigated where there was just an
  • 27:51 - 27:57
    atmosphere, the sun, rain - clouds were
    missing - and CO2 emissions. And
  • 27:57 - 28:03
    I hope you believe that the sun is behind
    the atmosphere and not in this atmosphere.
  • 28:03 - 28:10
    In the mid 80s there was prescribed
    ice added and already clouds and land
  • 28:10 - 28:17
    surfaces and yeah, you see a nice mountain.
    But actually in that time the resolution
  • 28:17 - 28:25
    was so low that the Alps only had one or
    two grid cells, meaning that was not so
  • 28:25 - 28:33
    much about land surface, but it was added.
    And for the first assessment report there
  • 28:33 - 28:39
    was a swamp ocean added, meaning an ocean
    was added, but it was had no depth. For
  • 28:39 - 28:46
    the second assessment report, the ocean
    got some depth. So it was a normal ocean
  • 28:46 - 28:53
    with surface circulation and there was
    added volcano activity and sulphates. For
  • 28:53 - 29:02
    the third assessment report, there was
    added... So this is all about which kind of
  • 29:02 - 29:11
    processes were there in the climate models
    that were investigated in these assessment
  • 29:11 - 29:17
    reports. Meaning there were climate models
    before that already had those processes
  • 29:17 - 29:22
    included, but they were not investigated
    in the assessment reports. So this is a
  • 29:22 - 29:26
    history of which climate models or which
    processes and climate models were
  • 29:26 - 29:31
    investigated in assessment reports. And
    the third assessment report, there was
  • 29:31 - 29:35
    another circulation edit for the ocean,
    the overturning circulations. And there
  • 29:35 - 29:42
    were rivers added, which is interesting
    because I do something with rivers and
  • 29:42 - 29:47
    there were aerosols added and a carbon
    cycle, meaning that the carbon that goes
  • 29:47 - 29:55
    into the atmosphere also goes out. But
    yeah, not everything, or that half-time is
  • 29:55 - 30:02
    not so good. For the AR5, er 4, there was
    chemistry added in the atmosphere and
  • 30:02 - 30:09
    interactive vegetation, and for the AR5
    there was ozone added and biomass burning
  • 30:09 - 30:16
    emissions. And there is a history of
    processes, but there is also a history of
  • 30:16 - 30:21
    computer modeling that might be really
    interesting. It started more or less in
  • 30:21 - 30:31
    1904 with Vilhelm Bjerknes, who found
    equations that could be solved to obtain
  • 30:31 - 30:38
    future states of the atmosphere. And he
    thought about that maybe these equations
  • 30:38 - 30:41
    are really hard to
    solve and that task should be split and
  • 30:41 - 30:48
    distributed to many people. So he
    basically mentioned a human computer and
  • 30:48 - 30:55
    then Lewis Fry Richardson came in 1922 and
    did actually calculate all this.
  • 30:55 - 31:04
    This did a six hour forecast solving the
    equations by hand, alone. And 42 days user
  • 31:04 - 31:09
    time, meaning he himself calculated 42
    days on it. But those 42 days were
  • 31:09 - 31:18
    distributed over two years in total. So he
    was a little behind the weather, only to
  • 31:18 - 31:25
    find out that it didn't give the correct
    answer. audience laughs That was long
  • 31:25 - 31:33
    forgotten. But people said, yea, that's
    not quite practical. We cannot do that.
  • 31:33 - 31:39
    But then computers came. In 1950, the
    first successful weather model was run on
  • 31:39 - 31:45
    a computer called ENIAC, and in 1950,
    weather predictions were run twice a day
  • 31:45 - 31:53
    on an IBM 701. Nowadays we use
    supercomputers much larger and there's a
  • 31:53 - 31:59
    whole list and rank and I will shortly
    introduce JEWELS to you: the Jülich Wizard
  • 31:59 - 32:04
    for European Leadership Science. That's a
    supercomputer in Jülich and I would have
  • 32:04 - 32:10
    shown you a picture, but you are not
    allowed, you are not simply allowed to
  • 32:10 - 32:17
    take pictures on that campus. But since
    super computers are fancy shiny cupboards
  • 32:17 - 32:25
    anyway, I thought this is OK. So we have
    these cupboards that look at shiny covers
  • 32:25 - 32:31
    and then this covers their blades and each
    blade is called a standard node and
  • 32:31 - 32:40
    consists of, in case of JEWELS, 2 times 24
    cores with 2.7 GHz and it's hyper-
  • 32:40 - 32:45
    threaded, meaning you can actually run 96
    threads or processes on one of these
  • 32:45 - 32:56
    nodes. And these notes have 12 times 8 GB
    of memory. And that's not quite much if
  • 32:56 - 33:01
    you want to run a climate model but
    I'll come to that a little later. And in
  • 33:01 - 33:07
    fact, in case of JEWELS, you have like
    three rows of five of these cupboards or
  • 33:07 - 33:18
    something. And so there are in total 2271
    standard nodes, 240 large memory nodes and
  • 33:18 - 33:26
    56 accelerated nodes having something like
    GPUs. And I tell you about JEWELS, not
  • 33:26 - 33:30
    because it's the
    fastest, actually, it's maybe the 30th,
  • 33:30 - 33:34
    not even because it's the fastest in
    Germany - it was when it was built but
  • 33:34 - 33:41
    that's a while ago - but I told you about
    that because JEWELS provides actually
  • 33:41 - 33:46
    computing budget for the ESM project, the
    Advanced Earth System Modelling Capacity.
  • 33:46 - 33:54
    And so there are actually earth system
    models run on that machine. So what I told
  • 33:54 - 33:57
    you before, there is not so much memory on
    each node.
  • 33:57 - 34:00
    So what you need to do is you need to cut
    down your problem and distribute them over
  • 34:00 - 34:07
    the nodes. And then there needs to be some
    communication. So usually if the task
  • 34:07 - 34:14
    is so simple, you can cut down your grid
    and put a number of grid cells to each
  • 34:14 - 34:19
    node. And then there's communication
    between the nodes on the boundaries to
  • 34:19 - 34:26
    solve the differential equations. Talking
    about grids, I would talk about the
  • 34:26 - 34:30
    resolution. Also, again, a history of
    resolution of the climate models. For the
  • 34:30 - 34:36
    1st assessment report, the region
    resolution was 500 kilometers times 500
  • 34:36 - 34:45
    kilometers. And as I said before, you see
    these two yellow yellowish cells in the
  • 34:45 - 34:52
    middle that are the Alps. For the second
    assessment report, the resolution already
  • 34:52 - 35:00
    doubled or halved, depends on how you want
    to phrase it. For the TAR, it was 180
  • 35:00 - 35:09
    kilometers for AR4, it
    was 120 kilometers. For the AR5, it's a
  • 35:09 - 35:17
    little bit a different section I show you.
    And also, I show you two resolutions.
  • 35:17 - 35:23
    There's a resolution for the higher
    models, which is 87, for example, 87.5
  • 35:23 - 35:30
    kilometers. And for the very high
    resolution, 30 kilometers. And that's
  • 35:30 - 35:35
    because climate models are not just one
    model, but they are different kinds of
  • 35:35 - 35:41
    models that are coupled. And each model
    has its own resolution. So it's more or
  • 35:41 - 35:46
    less like something like this. So we have
    a model for ice, we have a model for
  • 35:46 - 35:52
    atmosphere, for ocean and for terrestrial.
    And this is coupled. So they all sent
  • 35:52 - 35:57
    their data to a coupler or something. And
    that set was there as an input to the
  • 35:57 - 36:02
    other model. So this is more or
    less like how climate models look.
  • 36:02 - 36:12
    And each of the models, again, has several
    layers. For example, the terrestrial layer
  • 36:12 - 36:18
    has a ground water part and the
    atmosphere. And so there's some input from
  • 36:18 - 36:24
    the atmosphere to the soil and plant
    system. And then there's some water that
  • 36:24 - 36:31
    is sinking into the groundwater and then
    coming out to the rivers. And yeah. So
  • 36:31 - 36:36
    then we have the runoff. So meaning rivers
    get water. And then if you have a look to
  • 36:36 - 36:44
    rivers and want to parallelize rivers,
    then it's not so easy because we have a
  • 36:44 - 36:48
    source somewhere and the water has to go
    from the source or something that happens
  • 36:48 - 36:56
    at the source has an impact to the sink,
    meaning this has to communicate all the
  • 36:56 - 37:06
    way along to the sink. And that's where I
    come in. I actually do. So I show you the
  • 37:06 - 37:12
    Danube, which you probably know better
    with the name Donau. At a resolution of
  • 37:12 - 37:22
    five kilometers and basically cut down the
    Danube into sub river domains. And we
  • 37:22 - 37:29
    need. If we parallelize these we need to
    calculate the subriver domains that are
  • 37:29 - 37:36
    farther away from the sink first and it
    uses that in the first graph a little. So
  • 37:36 - 37:44
    the grayish areas are calculated first and
    then it goes down farther to the sink. So
  • 37:44 - 37:52
    just to tell you about what I do. So now
    we come back to the main question. So we
  • 37:52 - 37:59
    answered where the sources of the graphs
    come from. Now we answer the questions:
  • 37:59 - 38:07
    What is a representative concentration
    pathway? Meaning what we all did before
  • 38:07 - 38:13
    was more or less telling how we get to
    that black line in the first section. And
  • 38:13 - 38:26
    now we concentrate on the colored part
    where we have more graphs than one. So the
  • 38:26 - 38:31
    working group 1 of the IPCC generally
    tests the selection of coupled models, that
  • 38:31 - 38:36
    is what I told you before, matching
    specific conditions and investigates the
  • 38:36 - 38:41
    output assuming different emission
    scenarios. Meaning we have a couple of
  • 38:41 - 38:46
    climate models that are somehow different,
    for example in their grid. And then we
  • 38:46 - 38:53
    have input data. The input scenarios would
    be, for example, the first one where we
  • 38:53 - 38:59
    just do business as
    usual and don't reduce carbon emissions.
  • 38:59 - 39:06
    The second would be we start with our way
    we do it today, but we would slowly change
  • 39:06 - 39:11
    to renewable energy. And the third one
    would be a scenario where we do it
  • 39:11 - 39:16
    spontaneously now or so. And that is an
    input scenario that we put into the
  • 39:16 - 39:23
    systems and then we get out a model output,
    that says something about the future. So
  • 39:23 - 39:29
    there is a black line that says, OK, this
    was our history until today. And from that
  • 39:29 - 39:36
    on, we have three scenarios and they are
    represented upper to lower. So the upper,
  • 39:36 - 39:47
    upper and right line represents the way
    where we do nothing or so. So this is
  • 39:47 - 39:56
    basically what we do with scenarios. And
    the RCPs, Representative Concentration
  • 39:56 - 40:01
    Pathways are scenarios that include time
    series of emissions and concentrations of
  • 40:01 - 40:07
    the full suite of greenhouse gases and
    aerosols and chemical active gases as well
  • 40:07 - 40:16
    as land use and land cover. So that is
    another graph from the AR5 and it shows
  • 40:16 - 40:22
    again in the X-axis the years, it's the
    same timescale as before, but on the Y-
  • 40:22 - 40:29
    axis we now have the rate of forcing, that
    is basically having this impact on our
  • 40:29 - 40:36
    climate. And so each of the RCP scenarios
    has some kind of equivalent in
  • 40:36 - 40:43
    radiative forcing.
    Yeah. So we have a 4 of these scenarios.
  • 40:43 - 40:53
    The data for the RCP scenarios is
    coordinated by again the input4MIPS: input
  • 40:53 - 40:57
    datasets for model and intercomparison
    projects that I told you before. And most
  • 40:57 - 41:02
    of it is freely available and I gave you
    the link. So if you want to run your own
  • 41:02 - 41:08
    climate model and test it with these
    input, you can find it there. And now I
  • 41:08 - 41:11
    will explain the last part. The numbers
    and uncertainties.
  • 41:11 - 41:17
    So first of all, again, to the graph from
    before the numbers behind the RCP refer to
  • 41:17 - 41:24
    the radiative forcing at the end of the
    modeling period of 2100. Meaning if you
  • 41:24 - 41:31
    follow one of these lines, for example,
    the red one to where it crosses the 2100
  • 41:31 - 41:46
    line, then the number there is 8.5. So
    RCP8.5 is the name for this RCP scenario.
  • 41:46 - 41:53
    But then the numbers of these different
    sections are the numbers of models used
  • 41:53 - 42:03
    for this scenario in this time period.
    Yes. So as I said, there are lots of
  • 42:03 - 42:10
    models intercompared and we even have
    different models for the different time
  • 42:10 - 42:19
    periods. So until 2100 there are 39 models
    for the RCP8.5. And of all the all the
  • 42:19 - 42:29
    rest, there are 12. And you see this
    little gap, this line break at 2100. And
  • 42:29 - 42:35
    that is caused by the change of numbers of
    models that took took part in this
  • 42:35 - 42:41
    project. And another interesting thing
    that we see here, and maybe the most
  • 42:41 - 42:49
    important, is we have quite huge model
    uncertainties. So if we compare all the
  • 42:49 - 42:55
    models, there's a huge band where we can't
    exactly say, OK, it's like this or that.
  • 42:55 - 43:06
    But this band is still... About human
    uncertainties are more important, than this
  • 43:06 - 43:13
    model uncertainties. We see tiny overlap,
    but mainly we can say how will the human
  • 43:13 - 43:23
    behave derives our future. And that there
    will be this climate change we are talking
  • 43:23 - 43:31
    about. So that was the main part about
    this three parts. And it's also it is also
  • 43:31 - 43:38
    the most important part. Now, I could
    probably show you how you can install an
  • 43:38 - 43:44
    impact model to your local PC, but
    probably I will have maybe something like
  • 43:44 - 43:53
    three minutes left. So we'll switch to the
    conclusion. And yeah, maybe if it's
  • 43:53 - 44:02
    arising as a question, I can do it. So
    what have we learned? Weather is the
  • 44:02 - 44:06
    physical state of the atmosphere at a
    given time, while climate is average weather
  • 44:06 - 44:14
    over 30 years. A climate model as a
    numerical representation of the climate
  • 44:14 - 44:24
    system. And we learned that the main
    uncertainty is the way we solve a
  • 44:24 - 44:30
    differential equations. I would probably
    have told you what a differential equation
  • 44:30 - 44:37
    is in particular, but that would have
    taken maybe another lecture. Climate
  • 44:37 - 44:43
    change is not proven throughout repeating
    one real experiment over and over again.
  • 44:43 - 44:45
    So there is only one earth it is said. But
    models simulate our
  • 44:45 - 44:51
    past climate pretty, well based
    on physical laws that were proven in real
  • 44:51 - 44:59
    experiments. And then maybe the most
    important message. Human behavior
  • 44:59 - 45:04
    is the primary source of climate change.
    Therefore, we talk about projections and
  • 45:04 - 45:12
    not predictions. Meaning if we wanted to
    predict the climate, then we needed to
  • 45:12 - 45:18
    simulate all human minds. And what we will
    decide on future. But we don't. That would
  • 45:18 - 45:28
    be another talk again. We take what humans
    will decide in future as an input
  • 45:28 - 45:33
    scenario, and with these input scenarios
    we create different output scenarios. So
  • 45:33 - 45:37
    with different inputs scenarios, we get
    these different output scenarios. Where we
  • 45:37 - 45:43
    can tell, OK, when we behave like that,
    this is the output. And human behavior
  • 45:43 - 45:52
    scenarios dominate model uncertainties,
    meaning the question is what do we want?
  • 45:52 - 45:56
    And if you go to a demonstration, the
    answer is usually climate justice. And I
  • 45:56 - 46:11
    think that's a good answer. Thank you.
  • 58:44 - 58:44
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  • 58:44 - 58:45
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Title:
36C3 - Climate Modelling
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Video Language:
English
Duration:
59:16

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