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DIELECTRIC CONSTANT VALUES ( Relative permittivity )

From Wikipedia, the free encyclopedia
Relative permittivities of some materials at room temperature under 1 kHz[citation needed]
Materialεr
Vacuum1 (by definition)
Air1.00058986 ± 0.00000050
(at STP, for 0.9 MHz),[1]
PTFE/Teflon2.1
Polyethylene2.25
Polyimide3.4
Polypropylene2.2–2.36
Polystyrene2.4–2.7
Carbon disulfide2.6
Mylar3.1[2]
Paper3.85
Electroactive polymers2–12
Mica3-6[2]
Silicon dioxide3.9 [3]
Sapphire8.9–11.1 (anisotropic) [4]
Concrete4.5
Pyrex (Glass)4.7 (3.7–10)
Neoprene6.7[2]
Rubber7
Diamond5.5–10
Salt3–15
Graphite10–15
Silicon11.68
Ammonia26, 22, 20, 17
(−80, −40, 0, 20 °C)
Methanol30
Ethylene glycol37
Furfural42.0
Glycerol41.2, 47, 42.5
(0, 20, 25 °C)
Water88, 80.1, 55.3, 34.5
(0, 20, 100, 200 °C)
for visible light: 1.77
Hydrofluoric acid83.6 (0 °C)
Formamide84.0 (20 °C)
Sulfuric acid84–100
(20–25 °C)
Hydrogen peroxide128 aq–60
(−30–25 °C)
Hydrocyanic acid158.0–2.3
(0–21 °C)
Titanium dioxide86–173
Strontium titanate310
Barium strontium titanate500
Barium titanate1250–10,000
(20–120 °C)
Lead zirconium titanate500–6000
Conjugated polymers1.8–6 up to 100,000[5]
Calcium copper titanate>250,000[6]
Temperature dependence of the relative static permittivity of water
The relative permittivity of a material is its dielectric permittivityexpressed as a ratio relative to the permittivity of vacuum.
Permittivity is a material property that expresses the force between two point charges in the material. Relative permittivity is the factor by which the electric field between the charges is decreased or increased relative to vacuum.
Likewise, relative permittivity is the ratio of the capacitance of acapacitor using that material as a dielectric, compared to a similar capacitor that has vacuum as its dielectric. Relative permittivity is also commonly known as dielectric constant, a term deprecated in physics and engineering.

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