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. 2025 Apr 27;17(1):235.
doi: 10.1007/s40820-025-01752-x.

Thermally Conductive Ti3C2Tx Fibers with Superior Electrical Conductivity

Affiliations

Thermally Conductive Ti3C2Tx Fibers with Superior Electrical Conductivity

Yuxiao Zhou et al. Nanomicro Lett. .

Abstract

High-performance Ti3C2Tx fibers have garnered significant potential for smart fibers enabled fabrics. Nonetheless, a major challenge hindering their widespread use is the lack of strong interlayer interactions between Ti3C2Tx nanosheets within fibers, which restricts their properties. Herein, a versatile strategy is proposed to construct wet-spun Ti3C2Tx fibers, in which trace amounts of borate form strong interlayer crosslinking between Ti3C2Tx nanosheets to significantly enhance interactions as supported by density functional theory calculations, thereby reducing interlayer spacing, diminishing microscopic voids and promoting orientation of the nanosheets. The resultant Ti3C2Tx fibers exhibit exceptional electrical conductivity of 7781 S cm-1 and mechanical properties, including tensile strength of 188.72 MPa and Young's modulus of 52.42 GPa. Notably, employing equilibrium molecular dynamics simulations, finite element analysis, and cross-wire geometry method, it is revealed that such crosslinking also effectively lowers interfacial thermal resistance and ultimately elevates thermal conductivity of Ti3C2Tx fibers to 13 W m-1 K-1, marking the first systematic study on thermal conductivity of Ti3C2Tx fibers. The simple and efficient interlayer crosslinking enhancement strategy not only enables the construction of thermal conductivity Ti3C2Tx fibers with high electrical conductivity for smart textiles, but also offers a scalable approach for assembling other nanomaterials into multifunctional fibers.

Keywords: Density functional theory simulation; Equilibrium molecular dynamics simulation; High electrical conductivity; Interlayer crosslinking; Thermally conductive Ti3C2Tx fibers.

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Conflict of interest statement

Declarations. Conflict of Interest: The authors declare no interest conflict. They have no known competing financial interests or personal relationships that could have appeared to influence the work reported in this paper. Junwei Gu is an editorial board member for Nano-Micro Letters and was not involved in the editorial review or the decision to publish this article. All authors declare that there are no competing interests.

Figures

Fig. 1
Fig. 1
Preparation and characterization of Ti3C2Tx nanosheets and dispersion. a Schematic for fabrication of Ti3C2Tx. b SEM image of Ti3AlC2. c SEM, d AFM, e TEM, f HR-TEM and its FFT diffraction pattern (the inset), and g SAED images of Ti3C2Tx. POM images of Ti3C2Tx dispersion at concentrations of h 5 mg mL−1, i 15 mg mL−1, and j 25 mg mL−1
Fig. 2
Fig. 2
Fabrication, morphology, and chemical characterization of Ti3C2Tx fibers. a Schematic for fabricating Ti3C2Tx fibers. Photographs of Ti3C2Tx fibers b wound on the bobbin and c-d woven. SEM images of Ti3C2Tx fibers: e overall, f cross section, and g side-section views. h XPS full spectra, and XPS narrow spectra of i Ti 2p and j O 1s of Ti3C2Tx powder and Ti3C2Tx fiber
Fig. 3
Fig. 3
Structural characterization, mechanical, and electrical properties of Ti3C2Tx fibers. a DFT calculations of borate ester bond between adjacent Ti3C2Tx nanosheets. b XRD patterns, c WAXS and SAXS (inset) patterns graphs, d plots of azimuthal angle according to the WAXS patterns, e density and porosity, f tensile strength and Young’s modulus, and g electrical conductivity of Ti3C2Tx fibers with different Na2B4O7 contents. h Comparisons of electrical conductivity versus tensile strength of Ti3C2Tx fibers prepared with 0.75 wt% Na2B4O7 against reported Ti3C2Tx-based fibers and Ti3C2Tx fibers
Fig. 4
Fig. 4
ITR between Ti3C2Tx nanosheets and thermal conductivity of Ti3C2Tx fibers. a Schematic illustration of EMD simulation of borate ester covalently bonded Ti3C2Tx nanosheets. b ITR between borate ester covalently bonded Ti3C2Tx nanosheets with different Na2B4O7 contents obtained by EMD simulation. c Extremely fine grid divisions corresponding to the finite element analysis models of Ti3C2Tx fibers with different Na2B4O7 contents. d Temperature distribution of Ti3C2Tx fibers with different Na2B4O7 contents under the same heating temperature and time simulated by finite element analysis. e λ of Ti3C2Tx fibers with different Na2B4O7 contents. f Star-plot of the d-spacing, orientation order, density, ITR, and λ of Ti3C2Tx fibers with different Na2B4O7 contents
Fig. 5
Fig. 5
Joule heating performance of Ti3C2Tx fibers. a Temperature–time curves of single Ti3C2Tx fibers with different Na2B4O7 contents when applied DC voltage of 7 V. b Temperature–time curves of single Ti3C2Tx fibers with 0.75 wt% Na2B4O7 when applied DC voltage of 1 ~ 9 V. c Temperature–time curves and infrared thermal images of single Ti3C2Tx fibers at bending angles of 0° ~ 180°. d Infrared thermal images of Ti3C2Tx fibers with different letter shapes. e Temperature performance retention of Ti3C2Tx fibers after 5000 bending cycles

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