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    • CommentAuthorwookey
    • CommentTimeSep 26th 2012
     
    I've never understood psi-values (as opposed to U-values). I think djh explained it once as 'linear U-values (maybe k-values?)', but I still don't know how to use or calculate them, which annoys me.

    You could fix this by cutting-in a column of foamglas or thermix blocks at the corner. Not a trivial job, but possible.
    • CommentAuthorTimber
    • CommentTimeSep 26th 2012 edited
     
    Sorry for the lateness of the response, I have been out and about.

    The PSI value is essentially the reduction in U-Value at the junction.

    As for the pretty colours on the isotherms, red and white is good (i.e. warm) blue is bad as it is cold. The colour inbetween are the temps inbetween. The colours on the heat flux are heat flows - red and white are the largest heat losses.

    I don't see that insulating the party wall will help a huge amount, but I could run the numbers again tomorrow with 50mm of EPS on the party wall (very simple model) to get an idea.

    Obviously adding EWI will help over 95% or more of the building, but you guys asked what the thermal bridge was, so there it is! :tongue:
    • CommentAuthordjh
    • CommentTimeSep 26th 2012
     
    Posted By: wookeyI've never understood psi-values (as opposed to U-values). I think djh explained it once as 'linear U-values (maybe k-values?)', but I still don't know how to use or calculate them, which annoys me.

    Using them is easy, you just type them into PHPP. Boom, boom!!

    Linear U-values is a pretty good description - W/m.K instead of W/m²K. You just multiply the length of the thermal bridge by the temperature difference by the psi value and it tells you how many watts of heat you're losing over and above what the U-values for the two adjacent areas haven't accounted for.

    And that, as I understand it, kind of tells you how to calculate them. You model what happens in a perfect interface-less world and then model with the interface in place. The difference is the psi-value. But that's all hand-waving, of course, and I confess I don't know the true answer.
  1.  
    Hi Dave,

    I'm not understanding this either. If you multiply W/mK x length you still don't get a measure of heat loss The height would need to be factored in as well wouldn't it to get W/m2K - and hence the actual heat loss by calculation?

    As I asked above, I'snt the PSI value meaningless if you cannot put a number on the actual loss?
    •  
      CommentAuthorfostertom
    • CommentTimeSep 27th 2012
     
    Posted By: TimberThe PSI value is essentially the reduction in U-Value at the junction
    Posted By: djhYou just multiply the length of the thermal bridge by the temperature difference by the psi value and it tells you how many watts of heat you're losing over and above what the U-values for the two adjacent areas haven't accounted for ... You model what happens in a perfect interface-less world and then model with the interface in place
    I went on the Therm course and never understood that, so neatly put - so thanks. Mind you, I was struggling with a misbehaving borrowed laptop at the time, and I'm offered a re-run half price.
    • CommentAuthorEd Davies
    • CommentTimeSep 27th 2012
     
    What djh wrote supports my somewhat vague understanding of what psi (linear conductance) values are. Let's see if I can a) check my understanding and b) explain it with an example:

    Suppose you have a wall with a U-value of 0.1 W/m²·K with a studding or something with a psi value of 0.2 W/m·K. If the wall is 2.5 metres high and 4 metres wide with studs on 1 metre centres (yes, I know, rather implausible in the UK but let's keep the arithmetic simple). There are three studs, each 2.5 metres long for a total length of 7.5 metres.

    The total heat loss co-efficient of the wall would be area × U-value + stud-length × psi-value = (2.5 × 4 × 0.1) + (7.5 × 0.2) = 1 + 1.5 = 2.5 W/K.

    If the temperature differential is 20 °C (i.e., 20 K) then the heat loss would be 20 × 2.5 = 50 W.

    The bit I'm rather vague on is the idea that the psi value is in addition to the basic U-value; I think it's the incremental loss over the basic U-value. It doesn't have a width as such as that's already taken into account in its evaluation. E.g., a particular I-beam in particular insulation would have some psi value. If you doubled the thickness of the I-beam or changed the insulation you'd have to find a new psi value. On the other hand, if you decided to go from 600 mm centres to 400 mm then you'd just have to increase the total length you multiply the psi value by in order to calculate the total heat-loss coefficient.
    •  
      CommentAuthorfostertom
    • CommentTimeSep 27th 2012
     
    In that case , would you get the same answer as the alternative approach - proportional area?

    Is the point of psi-value, that once calcd, you can apply it 'per m' all over the place?
    And to calc it in the first place you model 1m x 1m of the junction in Therm.

    If that is say a wall/window jamb junction, then in Therm you get a heat loss for that 1m x 1m that is higher than:
    0.5 x 1m of mid-wall (no edge in sight) plus 0.5 x 1m of mid-window (no edge in sight) value
    and the difference is the psi value per m of that junction?
    • CommentAuthorEd Davies
    • CommentTimeSep 27th 2012 edited
     
    Posted By: fostertomIs the point of psi-value, that once calcd, you can apply it 'per m' all over the place?

    Yes.

    And to calc it in the first place you model 1m x 1m of the junction in Therm.

    I think you'd model 1 metre of the junction in Therm; 1 m × 1 m wouldn't make sense for a linear feature.
    •  
      CommentAuthorfostertom
    • CommentTimeSep 27th 2012
     
    Yeah, the Therm model is 1m long along the junction, but how wide ea side of that does the model spread?
    • CommentAuthorTimber
    • CommentTimeSep 27th 2012
     
    The therm model has no length. The 1m is how far to either side of the junction the model must extend to ensure that the heat flux and isotherms can stabalise. Also the 1m is not set in stone. The model should extend to three times the thickness of the element (wall) or at least 1m, whichever is smaller. Although this is not often followed as 1m tends to do the trick in most cases.
    •  
      CommentAuthorfostertom
    • CommentTimeSep 27th 2012
     
    Ah of coarse (Mad mag). But how does that zero-length snapshot of heat flux get translated into a 'per m' quantity?
    • CommentAuthorMike George
    • CommentTimeSep 27th 2012 edited
     
    Apparently, the way this works is that the PSI value is used to calculate a Y-value, which is measured in the units we all love and understand - W/m2K. This can then be used to determine the actual heat loss.

    All is explained here http://www.pinewood-structures.co.uk/content/1/95/psi-values--y-values-and-thermal-bridging.html
    •  
      CommentAuthorfostertom
    • CommentTimeSep 27th 2012
     
    Hmm - the way that reads is as mystfication to make us buy Pinewood's expertise/product. I did however learn from it that psi's lead to a Y-value to add to the familiar W/K figure. Now I can stop accounting for psi's by guess/fiddling effective frontal areas of elements.
    • CommentAuthorMike George
    • CommentTimeSep 27th 2012 edited
     
    Yes, best to ignore the blag and just get to the explanation of what's what

    Though I'd still like to see it all put into context. IE.

    Overall predicted heat loss and the contribution a thermal bridge makes to it.
    •  
      CommentAuthorfostertom
    • CommentTimeSep 27th 2012 edited
     
    Wouldn't that be (Y + W/K) (the building's total loss) versus Y (the building's totalled thermal bridge losses)?
    Or (Y + W/K) versus (psi x L) (the loss of each individual bridge)?
  2.  
    Yes, of course. There's actually a worked example on the link:shamed:
    •  
      CommentAuthorSteamyTea
    • CommentTimeSep 28th 2012
     
    Isn't psi a vector problem, so you can establish it from Pythagoras (sum of the hypotenuse equals the sum of the other two sides) for right angles. Or tangents when not a right angles (assuming homogeneous material).
    Then put the limits in (area of internal wall, thickness of wall, length, area of junction, temperature differences etc.), this gets around the divide by zero problem.
    This may help a bit:
    http://www.nhbc.co.uk/NHBCPublications/LiteratureLibrary/Technical/TechnicalExtra/filedownload,44601,en.pdf
    • CommentAuthorTimber
    • CommentTimeSep 28th 2012
     
    Well I have just re-done some calcs.

    I actually got the first ones slightly wrong - in-so-far-as I tweeked the model to the one shown in the pics, but forgot (DUR!) to re-run the calculations. The PSI value of the justion that I showed is actaully 0.198 W/mK. Not as bad as 0.3 that I quoted previously but still poor.

    Here is the interesting thing though...... insulating the party wall with 50 mm of EPS makes almost NO difference to the PSI value. It goes down to 0.193 W/mK. Hardly worth the effort from a thermal point of view.

    So, there it is, insulating the party wall doesn't offer much (if any) improvement in this sort of situation. And, infact, it makes things worse for your neighbour. Their corner between the party wall and external walls gets slightly colder, as the insulation on 'your' side, reduces the amount of heat you contribute to keeping the party wall warm.
    • CommentAuthordjh
    • CommentTimeSep 28th 2012
     
    Posted By: TimberHere is the interesting thing though...... insulating the party wall with 50 mm of EPS makes almost NO difference to the PSI value. It goes down to 0.193 W/mK. Hardly worth the effort from a thermal point of view.

    AIUI, the idea when switching from external to internal insulation is to have an overlap where there is insulation on both sides of the wall. So I think that as well as insulating a bit of the party wall, you'd also need to internally insulate a bit of the adjacent external wall to achieve a significant reduction in psi-value at the corner.

    Alternatively, as wookey says, you could cut in some structural insulation at the corner.
    • CommentAuthordjh
    • CommentTimeSep 28th 2012
     
    @tom, @mike, I'm having trouble seeing what you find difficult about psi-values. Let me try an example.

    Suppose I have a 2.5 m x 2.5 m wall with a U-value of 0.1. So the heat loss is 0.1 x 2.5 x 2.5 W/K
    Suppose I have a 1 m x 1.5 m window with a U-value of 1. So the heat loss is 1 x 1 x 1.5 W/K

    So if I put the window in the wall, the total heat loss H is 0.1 x (2.5 x 2.5 - 1 x 1.5) + 1 x 1 x 1.5 W/K = 1.975 W/K

    But that's not quite right, because the heat doesn't flow out at right angles where the window meets the wall. It sneakily curves to find the path of least resistance. So the psi-value adjusts for that. Somebody makes a cross-sectional picture of the edge of the window and the wall and the clever program calculates how heat actually flows through it, and what the difference per metre is.

    Suppose it is 0.08. Then you work out the length to apply it over - the perimeter of the window; in this case 1 + 1.5 + 1 + 1.5 = 5, multiply them together 5 x 0.08 = 0.4 and add it to the heat loss H' = 1.975 + 0.4 = 2.375 W/K

    Of course, the psi-value for the sill and jambs and head could all be different, to complicate things further.
    •  
      CommentAuthorikimiki
    • CommentTimeSep 28th 2012
     
    djh's approach is the sort that I naturally gravitate towards.

    SteamyT, Timber -- thoughts?
    •  
      CommentAuthorSteamyTea
    • CommentTimeSep 29th 2012 edited
     
    Posted By: djhIt sneakily curves to find the path of least resistance

    Yes, it is sneaky. It goes from hot to cold, as the internal surfaces (at the very first molecule level) are at the same temperature the heat path is perpendicular, at the next molecule level the windows is slightly colder than the wall (worse U-Value), so some of the heat that is rocketing through the window (ten times faster than the wall in the above example if assume identical thickness for both) goes forwards toward outside, but some will go to heat the wall, this goes on all the way though. Kind of two steps forwards and one to the side and half a one forwards (bit like a knight in chess, or me dancing in the 1970's).
    So it should be possible to do it by vectors if you know the thermal inertia of the wall and window (and any other materials involved), the thickness's/profiles and the temperature gradients, probably end up drawing an ellipse (looks like one on the pictures).
    In 3D it will look like an egg.
    • CommentAuthorTimber
    • CommentTimeSep 29th 2012
     
    As for the comments on the designs - these are just simlple models based on an assumed setup.

    I am sure that there are many many different ways of coming up with a better detail, or indeed the thoughts that although not ideal it still isn't so bad. I would suggest coming up with your own details and modelling them. That way you can see what difference it makes.

    As for me, I am in the camp of 'it would be nice to make it better, but equally there is an overall massive improvement in energy loss so just live with it' as any other method of overlapping insulation or whatever ends up with some other compromise (space, asthetics, whatever).
    •  
      CommentAuthorikimiki
    • CommentTimeSep 29th 2012
     
    It seems to me, that's very well reasoned.
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