2022
DOI: 10.1016/j.jcis.2021.10.137
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Conductive substrates-based component tailoring via thermal conversion of metal organic framework for enhanced microwave absorption performances

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Cited by 32 publications
(7 citation statements)
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“…Microwave absorption in FM-350 and FM-650 relies mainly on eddy current loss (Figure 6f−h). Meanwhile, impedance matching (Z = |Z in / Z 0 |), considered a prerequisite for the entry of incident microwaves, can be analyzed through characteristic input impedance 43,44 The 1/4 wavelength model, shown in Figure 6i−l, can provide insights into the relationship between the RL, matching thickness, and frequency. The RL curves for specific thicknesses reach the RL min at the frequency where Z is close to 1, particularly for FM-550, and the t m values fall near the λ/4 curves.…”
Section: Resultsmentioning
confidence: 99%
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“…Microwave absorption in FM-350 and FM-650 relies mainly on eddy current loss (Figure 6f−h). Meanwhile, impedance matching (Z = |Z in / Z 0 |), considered a prerequisite for the entry of incident microwaves, can be analyzed through characteristic input impedance 43,44 The 1/4 wavelength model, shown in Figure 6i−l, can provide insights into the relationship between the RL, matching thickness, and frequency. The RL curves for specific thicknesses reach the RL min at the frequency where Z is close to 1, particularly for FM-550, and the t m values fall near the λ/4 curves.…”
Section: Resultsmentioning
confidence: 99%
“…Microwave absorption in FM-350 and FM-650 relies mainly on eddy current loss (Figure f–h). Meanwhile, impedance matching ( Z = | Z in / Z 0 |), considered a prerequisite for the entry of incident microwaves, can be analyzed through characteristic input impedance , Z = | Z in / Z 0 | = μ r ε r nobreak0em0.1em⁡ tan nobreak0em0.25em⁡ normalh ( j 2 π fd c μ normalr ε normalr ) …”
Section: Resultsmentioning
confidence: 99%
“…Obviously, it is insufficient to express the complex permittivity of a material using simply the ideal Debye equation; the influence of conductivity must also be taken into account. Therefore, formula can be rewritten as follows ε = ( ε s ε ) 2 π f τ 1 + false( 2 π f false) 2 τ 2 + σ 2 π f ε 0 where ε 0 = 8.85 × 10 –12 F/M represents the vacuum dielectric constant and σ is the conductivity of materials . The ideal Debye formula can be written as the Cole–Cole circle true( ε false′ ε normals + ε 2 true) 2 + false( ε false″ false) 2 = true( ε normals ε 2 true) 2 If the material is in an ideal Debye state, with ε ′ as abscissa and ε ″ as ordinate, the complex permittivity of the material will form a semicircle with a center of ( ε s ε 2 ) …”
Section: Resultsmentioning
confidence: 99%
“…The sources of magnetic loss of materials are as follows: (1) the hysteresis loss caused by the change of the magnetic induction intensity due to the irreversible movement of the domain wall or the magnetic moment with the strength of the applied magnetic field, (2) induced current under alternating magnetic field and Joule heat generated by the ferromagnet, which causes the eddy current loss, and (3) natural resonance loss under the action of an external magnetic field due to the presence of a magnetocrystalline anisotropy field. ,, However, hysteresis loss needs to be generated under a large magnetic field, and the alternating magnetic field that generates electromagnetic waves is small. Therefore, the sources of magnetic loss of absorbing materials are natural resonance loss and eddy current loss.…”
Section: Resultsmentioning
confidence: 99%
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