Another Bureau of Meteorology failed three month temperature Outlook – Autumn 2013

This month the BoM announced “Seasonal Climate Outlook released today using a new model” but it will take more than a new model and colour scheme to get lipstick onto this pig. The BoM three month Outlooks are useless, should be abandoned and the money saved for more successful and worthy projects.
The temperature Outlook for Autumn has been a typical miserable failure.
Maximum temperature Outlook and real world maximum anomalies result
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Minimum temperature Outlook and real world minimum anomalies result

2 thoughts on “Another Bureau of Meteorology failed three month temperature Outlook – Autumn 2013”

  1. Their forecasts for the SW are clearly influenced by AGW predictions of fewer and weaker Southern Ocean cold fronts.

    In fact this autumn was quite cloudy and wet, in part due to mid-latitude disturbances. My theory is that the decreasing rainfall trend in the SW was due to a decline in mid-latitude disturbances since the 1970s and we are now returning to historically normal levels, and as a result, so will autumn and spring rainfall.

    The BoM got their prediction of declining rainfall in the SW right, but for the wrong reason.

  2. The issue of “net flows” has been stretched literally beyond belief in the climatology world. The Second Law is talking about an isolated system (See Wikipedia – “Laws of Thermodynamics”) and any physicist should be able to tell you that a system in physics has a very specific definition. (Also see Wikipedia “System.”) It can of course have a single component (often represented by a one-way heat transfer between two objects) but if it has more than one component, then the components must be interdependent.

    Now, if radiation from a cooler atmosphere were actually able to add thermal energy to a warmer target on the surface, say a rock beside a tidal lake, then that is the first “component.” The problem then to consider runs like this: if that extra energy is then stored for a while (say, until high tide) and the energy then transfers to some water on the surface by conduction, and then that same parcel of energy eventually gets back into the atmosphere with two further “components” such as evaporative cooling of the water, followed by subsequent release of latent heat, where then is the interdependence between any of these four separate components which you are in effect assuming to be all part of the one system, as defined by the Second Law? Sorry, the very first component (if it could occur) is not just a component of a larger system and it would be an outright and indisputable violation of the Second Law.

    Think of Venus. Every 4-month long day its surface warms by 5 degrees, and then it cools by five degrees as the atmosphere radiates to space during the 4-month night. The surface temperatures are in the vicinity of 730K to 735K approximately. It takes a lot of energy to warm it by 5 degrees, and it doesn’t happen in the first day of sunshine, especially when you remember that such Solar radiation reaching the surface has only about one tenth of the power of that reaching Earth’s surface. So there must be a process in which energy builds up during the 4 month day.

    Now we know that about 97.5% of incident Solar radiation is either reflected or absorbed by the atmosphere, so obviously the atmosphere will warm while the Sun is shining, but gradually over 4 months – say I.25 degree per month.

    Clearly we are not talking about a radiative process warming the surface here, because incident radiation would have to be about 16,100W/m^2 into the surface to have any effect in that temperature range. And if it were it could probably do the job in a few hours, not 4 months. Furthermore, we at PSI would insist that any such radiation having any effect on such a hot surface would have to be directly from a hotter source, namely the Sun. We just don’t believe in non-interdependent components violating the Second Law, so we rule out radiation from the colder atmosphere. In any event, with only about 10W/m^2 of incident insolation entering the surface, there’s not a lot of energy to play with for back radiation, now is there?

    Perhaps you think that the energy entering the TOA will do the trick. Well look at the figures – something like 2,600W/m^2 from memory before any is reflected away, which is much more than half of it. Perhaps we have about 1,000W/m^2 starting on its way into the atmosphere. (That’s to 1 significant figure – it doesn’t matter what the precise figure is.) How could the atmosphere somehow magnify this about 16 times before it comes out of the base of the atmosphere and into the surface, and why would it have so much more success getting through the atmosphere than did the Solar radiation? Remember – no more than 10W/m^2 could be from back radiation that was sending back energy from the surface, which was sending back energy from the Sun. By the way, Science of Doom has a totally incorrect figure of about 158W/m^2 (if I remember correctly) for the incident Solar radiation reaching the Venus surface. You’d think he would have checked the data from the Russian probes before using a figure which is at least 10 times the real one.

    So the Venus surface is not heated by any “runaway greenhouse effect.” If you’re not convinced, then think about how energy gets down into the Uranus atmosphere which is mostly hydrogen and helium. I’m happy to discuss any questions you may have about my explanation of what is happening on these planets – and on Earth, where the Sun cannot heat our surface to 288K with direct Solar radiation alone. Just use SBL to convince yourself of this obvious fact.

    Radiative forcing is not what is the primary determinant of Earth’s mean surface temperature. As on Uranus and Venus, and throughout the universe, temperatures in any atmosphere have a propensity to follow a temperature gradient which is between about 65% and 100% of the quotient of the acceleration due to gravity and the weighted mean specific heat of the gases. The level of the plot is determined by the need for radiative balance, so that Is the “starting point.” Then, at whatever temperature the plot intersects the surface, we have a pre-determined base supporting temperature which slows all radiative and non-radiative cooling at night, enabling the Sun (if applicable) to warm somewhat the next day, this being but a marginal effect, as is the slowing of cooling as the surface comes back towards the base temperature. No big changes in climate will occur without natural changes in the parameters just mentioned. That is the “New School of Thought” which we are starting to talk about at PSI. Keep watching for a new article on such within a few days.

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