Permittivity and conductivity of building materials
[
calculates the relative permittivity, conductivity, and complex relative permittivity for
the specified material at the specified frequency. The methods and equations modeled in the
epsilon
,sigma
,complexepsilon
] = buildingMaterialPermittivity(material
,fc
)buildingMaterialPermittivity
function are presented in Recommendation ITU-R P.2040
[1].
Calculate relative permittivity and conductivity at 9 GHz for various building materials as defined by textual classifications in ITU-R P.2040, Table 3.
material = ["vacuum";"concrete";"brick";"plasterboard";"wood"; ... "glass";"ceiling-board";"chipboard";"floorboard";"metal"]; fc = repmat(9e9,size(material)); % Frequency in Hz [permittivity,conductivity] = ... arrayfun(@(x,y)buildingMaterialPermittivity(x,y),material,fc);
Display the results in a table.
varNames = ["Material";"Permittivity";"Conductivity"]; table(material,permittivity,conductivity,'VariableNames',varNames)
ans=10×3 table
Material Permittivity Conductivity
_______________ ____________ ____________
"vacuum" 1 0
"concrete" 5.31 0.19305
"brick" 3.75 0.038
"plasterboard" 2.94 0.054914
"wood" 1.99 0.049528
"glass" 6.27 0.059075
"ceiling-board" 1.5 0.0064437
"chipboard" 2.58 0.12044
"floorboard" 3.66 0.085726
"metal" 1 1e+07
Calculate the relative permittivity and conductivity for concrete at frequencies specified.
fc = ((1:1:10)*10e9); % Frequency in Hz [permittivity,conductivity] = ... arrayfun(@(y)buildingMaterialPermittivity("concrete",y),fc);
Plot the relative permittivity and conductivity of concrete across the range of frequencies.
figure yyaxis left plot(fc,permittivity) ylabel('Relative Permittivity') yyaxis right plot(fc,conductivity) ylabel('Conductivity (S/m)') xlabel('Frequency (Hz)') title('Permittivity and Conductivity of Concrete')
material
— Building material"vacuum"
| "concrete"
| "brick"
| "plasterboard"
| ...Building material, specified as vector of strings including one or more of these options:
"vacuum" | "glass" | "very-dry-ground" |
"concrete" | "ceiling-board" | "medium-dry-ground" |
"brick" | "floorboard" | "wet-ground" |
"plasterboard" | "chipboard" | |
"wood" | "metal" |
Example: ["vacuum" "brick"]
Data Types: char
| string
fc
— Carrier frequencyCarrier frequency in Hz, specified as a positive scalar.
Note
fc
must be in the range [1e6, 10e6] when the
material
is "very-dry-ground"
,
"medium-dry-ground"
or "wet-ground"
.
Data Types: double
epsilon
— Relative permittivityRelative permittivity of the building material, returned as a nonnegative scalar or
row vector. The output dimension of epsilon
matches that of the
input argument material
. For more information about the computation
for the relative permittivity, see ITU Building Materials.
sigma
— ConductivityConductivity, in Siemens/m, of the building material, returned as a nonnegative
scalar or row vector. The output dimension of sigma
matches that of
the input argument material
. For more information about the
computation for the conductivity, see ITU Building Materials.
complexepsilon
— Complex relative permittivityComplex relative permittivity of the building material, returned as a complex scalar or row vector of complex values.
The output dimension of complexepsilon
matches that of the
input argument material
. For more information about the computation
for the complex relative permittivity, see ITU Building Materials.
Section 3 of ITU-R P.2040-1 [1] presents methods, equations, and values used to calculate real relative permittivity, conductivity, and complex relative permittivity at carrier frequencies up to 100 GHz for common building materials.
The buildingMaterialPermittivity
function uses equations from ITU-R P.2040-1 to
compute these values.
The real part of the relative permittivity is calculated as
epsilon
=
afb.
The computation of epsilon
is based on
equation (58). f is the frequency in GHz. Values for
a and b are specified in Table 3 from ITU-R
P.2040-1.
The conductivity in Siemens/m is calculated as
sigma
=
cfd.
The computation of sigma
is based on equation
(59). f is the frequency in GHz. Values for c
and d are specified in Table 3 from ITU-R P.2040-1.
The complex permittivity is calculated as
complexepsilon
= epsilon
–
1i
sigma
/
(2πfcε0).
The computation of complexepsilon
is based on
Equations (59) and (9b). f is the frequency in GHz.
c is the velocity of light in free space.
ε0 = 8.854187817e-12 Farads/m, where
ε0 is the electric constant for the permittivity of free
space.
For cases where the value of b or d is zero, the
corresponding value of epsilon
or sigma
is
a or c, respectively and independent of
frequency.
The contents of Table 3 from ITU-R P.2040-1 are repeated in this table.
The values a, b, c, and
d are used to calculate relative permittivity and conductivity. Except
as noted for the three ground types, the frequency ranges given in the table are not hard
limits but are indicative of the measurements used to derive the models. The
buildingMaterialPermittivity
function interpolates or extrapolates relative
permittivity and conductivity values for frequencies that fall outside of the noted limits.
To compute relative permittivity and conductivity for different types of ground as a
function carrier frequencies up to 1000 GHz, see the earthSurfacePermittivity
function.
Material Class | Real Part of Relative Permittivity | Conductivity (S/m) | Frequency Range (GHz) | ||
---|---|---|---|---|---|
a | b | c | d | ||
Vacuum (~ air) | 1 | 0 | 0 | 0 | [0.001, 100] |
Concrete | 5.31 | 0 | 0.0326 | 0.8095 | [1, 100] |
Brick | 3.75 | 0 | 0.038 | 0 | [1, 10] |
Plasterboard | 2.94 | 0 | 0.0116 | 0.7076 | [1, 100] |
Wood | 1.99 | 0 | 0.0047 | 1.0718 | [0.001, 100] |
Glass | 6.27 | 0 | 0.0043 | 1.1925 | [0.1, 100] |
Ceiling board | 1.50 | 0 | 0.0005 | 1.1634 | [1, 100] |
Chipboard | 2.58 | 0 | 0.0217 | 0.78 | [1, 100] |
Floorboard | 3.66 | 0 | 0.0044 | 1.3515 | [50, 100] |
Metal | 1 | 0 | 107 | 0 | [1, 100] |
Very dry ground | 3 | 0 | 0.00015 | 2.52 | [1, 10] only(a) |
Medium dry ground | 15 | – 0.1 | 0.035 | 1.63 | [1, 10] only(a) |
Wet ground | 30 | – 0.4 | 0.15 | 1.30 | [1, 10] only(a) |
Note (a): For the three ground types (very dry, medium dry, and wet), the noted frequency limits cannot be exceeded. |
[1] ITU-R P.2040-1. "Effects of Building Materials and Structures on Radiowave Propagation Above 100MHz." International Telecommunications Union - Radiocommunications Sector (ITU-R). July 2015.
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