Foam Sandwich

26th September 2022


I’ve been looking at this bike camper idea some more. I realized that it tickles my brain because it’s sort of an insoluble problem. There’s so many axes to simultaneously optimize, and many conflict. For example, strength vs. weight for towing, cost vs. not-spending-a-ridiculous-amount-on-a-silly-idea, large sleeping space vs. drag while towing, etc. As a bonus, it’s also 100% un-useful and impractical which always makes things more fun!

Standard little “foamies” are built from XPS (pink/blue rigid insulation), Titebond II glue, canvas cloth, and coats of exterior paint. Depending on the size and shape, there’s generally additional support pieces made using traditional wood, aluminum, or steel.

For a bike trailer in particular though, and preferably non-ebike, I’d like to really emphasize the “lightweight” axis while still keeping it usable.

So! I’m learning what I assume is some first-year engineering. That is, Real Engineering that involves atoms, not the pretend software-style that largely concerns itself with trolling on Twitter1 while waiting for the linker.

(I apologize in advance if I use engineering terminology improperly and/or butcher your discipline, please feel encouraged to send corrections.)

XPS rigid insulation (foam) has very good compression strength, and so it’s a great material if any forces applied to it are spread out. But the surface isn’t very tough (sort of squishy on top, and pieces easily chip off), and it’s quite flexible and will yield and crack very easily unless it’s extremely thick. So, the good points:

Another material used in place of fibreglass or canvas (by RC plane makers, I believe) is kraft paper. This is moderately thick paper, pretty much like a brown paper shopping bag from the grocery store.

When this is stuck to the foam, it gets surprisingly much more rigid. So I’m attempting to Do A Science to get a guess as to whether a trailer made out of only foam, paper, glue, and paint would be durable and lightweight enough to be useful.

The first round of tests are intended to get an idea of how the tensile strength is improved. I did this by setting up pieces of 3” by 24” foam that’s 1” thick.

The kraft paper is first wetted down, a layer of glue applied to the foam surface, the paper laid, then more glue applied to the top of paper and then rolled in. For the multiple layer samples, the lower layers are allowed to fully dry (24h+) before doing the next layer.

This all results in a delicious foam and paper sandwich.

How does this affect the tensile strength? Imagining that you’re pushing down on the middle, the sandwich helps because the paper doesn’t stretch (very much). This means that the bottom side of the foam can’t get longer and the top side can’t get shorter (at least until the sandwich breaks in some way), so it makes it less bendy.

To measure how well this works, the test pieces are laid across a gap as if they were a bridge and put a weight on the very middle of the span, measuring how much it bends (deflects).

Deflection untreated Measuring deflection of an untreated foam sample

Deflection kraft single layer Measuring deflection of a foam sample covered in kraft paper

Starting with untreated, measure the distance from the table to the foam with and without one and two pound weights added. This is also done twice flipping the sample over, and taking the average because the foam tends to have a natural bend one way or the other.

I repeated these measurements with various samples:

In all cases, the covers are attached with Titebond II glue, in particular for the fibreglass – it’s not using resin or epoxy, it’s just glued on too.

Here’s the raw deflection data.

Untreated

Nominal 1 lb 2 lb
3.5405 3.0680 2.6805
3.5115 3.0980 2.7355

Kraft 1/1

Nominal 1 lb 2 lb
3.3840 3.3425 3.3100
3.6470 3.5475 3.4795

Kraft 2/2

Nominal 1 lb 2 lb
3.9165 3.8750 3.8220
3.1490 3.0895 3.0415

Fibreglass 2.6 oz

Nominal 1 lb 2 lb
3.6415 3.5830 3.5195

Kraft 1/2

Nominal 1 lb 2 lb
3.5790 3.5295 3.4810
3.5340 3.5115 3.4740

Kraft 2/3

Nominal 1 lb 2 lb
3.4040 3.3635 3.3425
3.7310 3.7085 3.6910

There’s two measurements for each type, testing with both sides up because there’s a curve. “Fibreglass B” is missing because I did such a bad job of fibreglassing that the bubbles on that side made it impossible to measure. Also note that there’s substantially more accuracy implied by the number of digits after the decimal point than there really was.

Now, taking the raw deflection measurements, and using “untreated” as an example, calculate the difference between nominal and with-weight. Then, take the two deflection amounts, and average them:

\[\begin{align} \delta{}C_1 & = 3.5405 in - 3.0680 in = 0.4725 in \\ \delta{}C_2 & = 3.5115 in - 3.0980 in = 0.4135 in \\ \delta{}C & = (0.4725 in + 0.4135 in) / 2 = 0.443 in \\ \end{align}\]

So, untreated, the foam deflected an average of \(0.443 in\) under a 1 lb weight.

Next, bust out the Serious Engineering 101 to calculate the foam’s moment of inertia: \(\frac{width * height^3}{12}\) 2

\[I = (bh^3)/12 = (3 in * (1 in)^3)/12 = 0.25 in^4\]

I assumed this was constant even though it isn’t exactly. For example, the coverings aren’t zero-width.

Then use the moment of inertia to calculate the modulus of elasticity, which is the useful thing: \(\frac{force * length^3}{48 * I \delta{}C}\) 3

\(I\) is the moment of inertia from above, \(\delta{}C\) the deflection measured.

\[E = \frac{FL^3}{48I\delta{}C} = \frac{1 lb * (24 in)^3}{48 * 0.25in * 0.443in} = 2600 PSI\]

Repeat that mess for both one and two pound samples, and for all the candidates. Assuming I did any of that correctly, here’s the PSI measurements.

Sample PSI
Untreated 1lb 2600
Untreated 2lb 2816
Kraft 1/1 1lb 16340
Kraft 1/1 2lb 19080
Kraft 2/2 1lb 22811
Kraft 2/2 2lb 22811
Fibreglass 1lb 19692
Fibreglass 2lb 18885
Kraft 1/2 1lb 32000
Kraft 1/2 2lb 29164
Kraft 2/3 1lb 36571
Kraft 2/3 2lb 45399

Because the force (weight applied) should be factored out, the 1 and 2lb ought to be the same. For the stiffer samples, the 1lb didn’t deflect very much so the measurements were likely poorer. In any case, somewhere between the 1 and 2lb PSI are about what I measured. So averaging the PSI measurements again, and sorting:

Sample PSI (average)  
Untreated 2708  
Kraft 1/1 17710  
Fibreglass 19288  
Kraft 2/2 22811 4
Kraft 1/2 30582  
Kraft 2/3 40985  

Interestingly, this puts a single layer of kraft at almost exactly the same stiffness as a single layer of light fibreglass. With the caveats that I did a terrible fibreglassing job, that the fibreglass is slightly lighter than the paper, that the fibreglass I got was very lightweight, and that my measurements are crappy, this is still pretty cool. Also, 3 layers on the “outside” are more than twice as stiff as a single thin fibreglass layer.

However, given that I did do a terrible fibreglassing job whereas the kraft goes on pretty well even when applied with no skill or practice, I feel pretty good about ploughing onward with kraft paper. My current plan then is either one or two layers on the inside of the structure, and three on the outside (as it’s more likely to get bashed and will be closer to water, etc.).

Speaking of water, another test I really ought to do is a more thorough application of some sort of exterior paint to make sure it can be waterproofed. But I think there’s enough options that that exploration can be deferred until I’m actually ready to paint. Or I’ll just choose something cheap and go for it.

I also noticed that uneven application (i.e. more layers on one side than the other) seems to cause foam to warp, so “Kraft 0/3” probably wouldn’t work that well.


  1. In what I feel is an admirable show of self-restraint, I didn’t even href any SWE’s twitter to “Twitter” here. 

  2. Just because! This is Engineering and I don’t need to hear about “why are doing this?”. This number goes in the next crazy formula, so we’re darn well going to get it. 

  3. Look, we’re second-string programmers pretending to be civil engineers building a bridge out of foam and paper. Just plug the damn numbers in. 

  4. That 2/2 is measured as weaker than 1/2 is not a show of strength for my data. This is likely because 2/2 was the first one I did, and I didn’t wait for a full cure between layers, so it’s probably more like “1.5/1.5” or worse. 


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