Tin vs. Aluminum: Shielding Properties and the 1940s Material Transition
The phrase “tinfoil hat” refers to a material that has not been commercially available for consumer use since the 1940s. The material we now call “tinfoil” is aluminum. This distinction is not semantic. The two metals have meaningfully different electromagnetic shielding properties.
The Material Transition
Tin foil — actual tin — was the standard household wrapping material from the late 19th century through the early 1940s. Reynolds Metals introduced aluminum foil to the US consumer market in 1947, and aluminum rapidly displaced tin due to lower production costs, greater malleability, and the significant expansion of aluminum production capacity that had been built up during World War II for aircraft manufacturing.
By the mid-1950s, the material commonly called “tinfoil” was universally aluminum. The name persisted. The material did not.
TFRi notes the timeline: the original McBain experiment in 1927 used actual tin. The MIT study in 2005 used aluminum. No comparative study of the two materials’ shielding properties in this application has been published. We find this absence consistent with the broader research gap documented in TFRi Working Paper 2024-03.
Electromagnetic Properties Compared
Tin (Sn)
Electrical conductivity: 8.7 × 10⁶ S/m
Magnetic permeability: Paramagnetic (very slight)
Skin depth at 1 GHz: ~5.4 μm
Corrosion resistance: Excellent (self-passivating oxide layer)
Historical availability: Consumer use through ~1945
Aluminum (Al)
Electrical conductivity: 3.77 × 10⁷ S/m
Magnetic permeability: Paramagnetic (very slight)
Skin depth at 1 GHz: ~2.6 μm
Corrosion resistance: Good (oxide layer, but thinner)
Historical availability: Consumer use from ~1947
Aluminum has roughly four times the electrical conductivity of tin, which translates to a smaller skin depth — the distance electromagnetic waves penetrate before being attenuated by a factor of 1/e. In principle, this makes aluminum a more effective shield per unit thickness at any given frequency.
In principle.
The Geometry Problem
Raw material conductivity is necessary but not sufficient for effective shielding. The geometry of the shielding structure determines its resonance characteristics, and resonance characteristics determine which frequencies are attenuated and which are amplified. This is the central finding of the MIT study: material properties alone do not predict shielding effectiveness.
Aluminum’s higher conductivity means it is a more efficient antenna at its resonant frequencies. The same property that makes it a better broadband shield also makes it a better amplifier at specific frequencies determined by its physical geometry. This is not a paradox — it is basic electromagnetic engineering — but it has implications that the popular discourse has entirely ignored.
The implication: The transition from tin to aluminum in the 1940s may have altered the shielding profile of improvised headwear. Tin’s lower conductivity means weaker attenuation across the board — but also weaker amplification at resonant frequencies. Whether McBain’s 1927 experiment with actual tin would produce the same paradoxical amplification observed in the MIT’s 2005 test with aluminum is an open question.
It is, to TFRi’s knowledge, an unasked question.
The Wartime Production Question
The timing of the material transition invites a question that TFRi raises without answering: the massive expansion of aluminum production capacity during World War II was driven by military aircraft manufacturing. After the war, this production capacity needed civilian markets. Reynolds Metals’ introduction of consumer aluminum foil in 1947 converted wartime industrial capacity into consumer products.
This is standard postwar economic history and is not controversial. What TFRi notes is that the transition coincided with the early expansion of government radio and radar programs, and that the electromagnetic shielding properties of the replacement material differed meaningfully from the material it replaced. Whether this coincidence is meaningful is, again, an open question. We are in the business of documenting open questions.
Implications for Modern Shielding
Modern TFRi-certified products are not made of tin or household aluminum foil. Engineered electromagnetic shielding uses specialized materials — conductive fabrics, nickel-copper mesh, silver-coated textiles — selected for specific frequency response characteristics. The tin-versus-aluminum question is historically interesting but practically moot for current product certification.
However, the question matters methodologically: it demonstrates that material selection has measurable consequences for shielding performance, that the “common knowledge” about tinfoil hats is based on a material that hasn’t existed in consumer form for 80 years, and that the single empirical study on the subject tested the wrong material.
Whether our products address this gap through material science, psychological priming, or sheer force of will is something we discuss internally more than you’d expect.
Material properties sourced from CRC Handbook of Chemistry and Physics, 97th Edition.
Historical production data: Reynolds Metals Company archives, US Bureau of Mines annual reports, 1940–1955.