A few weeks back, I mentioned that I had an energy audit performed on my family’s home (a nineteenth century farmhouse on a stone basement in upstate New York, which we moved into last year). I outlined the findings and the proposals that my local energy efficiency contractor had suggested. Although we had 1980s vintage insulation in the walls, the attic, and the basement, the audit turned up a lot of issues:
- Portions of the interior walls upstairs communicated with the attic airspace, meaning that the only thing preventing heat leaking through those walls was a single layer of drywall.
- The basement was wet, drafty, and the unenclosed and ragged fiberglass insulation was unlikely to be performing well.
- The house was very leaky: a blower door test revealed a very high level of air exchange.
- Use heavy plastic, drainage channels, a sump pump and a dehumidifier to manage moisture in the basement.
- Air seal the basement.
- Correct the air leakage issues in the attic and add more insulation there.
- Replace various old, inefficient appliances with much more efficient modern equivalents.
I had thought this would be reasonably simple, but it turned out that initially the energy inflows and outflows were out of balance by a factor of two and I had to do a lot of further exploration to figure out why that might be. In this process, I was helped a lot by Steve Andrews who, in addition to being an ASPO-USA founder, was a green building consultant for many years. He reviewed my spreadsheet several times and made a number of helpful suggestions. I also discovered things about the house that I didn’t know (like the 1/2″ of styrofoam between the old clapboards and the vinyl siding on the house).
Eventually, I got the inflow and outflow on the house to within 10% of each other and decided to call it quits – there are too many uncertainties that simply can’t be practically resolved to attempt to model things more accurately than that. Here’s the summary of my energy balance model for the house as it functions at present:
The units here are millions of British Thermal Units summed over the six month heating season October-March. (I apologize to my European readers for the irrational units over here). The right column shows all the energy inputs I was able to document coming into the house. The major factors were the wood heat and electricity. However, although our house was not designed with passive solar heating in mind, it was necessary to account for solar gain through the windows to get close enough. I also worked out approximations for things like body heat (based on assuming 2/3 of dietary calories ended up as heat in the house) and solar gains through the walls, but those turned out to be relatively minor contributions.
At this point, I’m going to make some notes about how to go about making this kind of calculation for the benefit of anyone who wants to do the same for their own home (or critique my approach). If you don’t care for the technical details, you may want to skip these next bullet points.
- Wood – I knew how many cords I had bought and went out and measured the woodpile to figure out how much was left, then made allowance for the remainder of March. Then I used heat values for maple/beech (our main local species) from this Engineering Toolbox page, but corrected for our stove being rated as 75% efficient vs 65%.
- Electricity – I included the entire electric usage from the utility bills for the heating season. This is probably a decent approximation: in addition to the baseboard electric heat our house came with, most appliances – refrigerators, computers, stoves, etc – will end up with all their electricity usage being heat inside the building. The one partial exception is hot water, where some of the heat will end up in the basement or exiting the house via the drains – I didn’t attempt to model that.
- Solar gain – I used this excellent online solar gain calculator, along with having measured the window area on each wall of the house.
- For infiltration, my auditor supplied me with a blower door measurement that at 50Pa pressure difference, the fan was pushing 5155 cubic feet per minute. One divides this by the “LBL number” to get an estimate of the natural rate air movement through the house – for a two story house in my area, the number is 15, so I get 345cfm as the estimated average air movement through the house. Next we need to know the heat capacity of that air which works out to 0.0262 btu per cubic foot per degree Fahrenheit. Multiply these two factors by a third: the number of minutes in a day and you get the number of BTU per “degree day”. This is basically the amount of heat required to heat the outside air for a whole day by one degree F. Then you need the number of degree days (eg from a map like this) which in my climate is about 7000. That’s it. Note that there is pretty much no way to get close on the infiltration heat loss without a blower door test of the house.
- Then there’s the conductance loss through the various house elements. I started out with various crude approximations but had to refine them as I tried to get energy inflow and outflow on the house to balance. The most complex is the walls so let me illustrate with that. My walls consist of 1″ hardwood paneling inside 3 1/2″ studs with blown in cellulose in the cavities. Outside the studs is a layer of clapboards, then about half an inch of styrofoam, then vinyl siding that was installed over the clapboards by the previous owners. I estimate the R value of this assemblage at about 15 as follows: 0.5 for inner air boundary layer, 1 for the wood paneling, 0.75 for the clapboards, 2.5 for the styrofoam and an extra 0.5 for the still air in the clapboard/vinyl arrangement. Then then there’s the stud/cellulose, which I estimate at a combined effective 10 (the cellulose is about 12.5 and the stud is about 3.5 and we have to add these in weighted reciprocal so 16/(1.5/3.5+14.5/12.5) (noting that these are 1.5″ thick studs and are 16″ on center). Then 10 + 2 x 0.5 + 2.5 + 1 + 0.75 = 15.25. On the downstairs, where the IR camera found some indication of settling and voidage in the cellulose, I took a 10% discount from this number.
- Once you have an R value, then the heat loss per degree day is given by 24*A/R where A is the area in square feet. Measure the area of the walls, subtract the area of the windows to be treated separately but similarly with their own R value, and then multiply by the number of heating degree days for your climate.
- The attic and basement are similar except that it’s necessary to guesstimate how effective the ragged unenclosed fiberglass in the basement really is. I gave my floor assemblage credit for R-6.
- Finally, I had an unknown fraction of the interior upstairs walls in thermal communication with the attic. I guesstimated about 1/4 of the wall surface area was effectively in that state, and assumed an R value of 2 for that area (under Steve’s guidance – the air layers next to the drywall need to be counted not just the R of the drywall itself or this heat loss will be overestimated).
Clearly – there are a lot of things here that are not known precisely. There’s no way to be certain about that upstairs interior wall loss, the exact efficiency of our stove, the exact microclimate at our hill farm elevation, etc. But I felt this model was good enough to be useful for making estimates of the likely effect of the work. I will take that up in a second post shortly.