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Research Article

Preparation of highly loaded copper(II) oxide nanoparticle suspensions for LIFT-printing of electronics

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Article: 2316918 | Received 30 Jan 2023, Accepted 05 Feb 2024, Published online: 22 Feb 2024

Figures & data

Figure 1. The principle of LIFT.

Figure 1. The principle of LIFT.

Figure 2. UV–Visible absorption spectra of the CuONPs suspension EG/W (a), 1,3PrG/W (b), and in 1,2PrG/W (c).

Figure 2. UV–Visible absorption spectra of the CuONPs suspension EG/W (a), 1,3PrG/W (b), and in 1,2PrG/W (c).

Figure 3. TEM images of the CuONPs in EG/W (a), 1,3PrG/W (b), and 1,2PrG/W (c).

Figure 3. TEM images of the CuONPs in EG/W (a), 1,3PrG/W (b), and 1,2PrG/W (c).

Figure 4. The viscosity of the samples as a function of shear rate.

Figure 4. The viscosity of the samples as a function of shear rate.

Table 1. Parameters of the Williamson model for the three samples.

Figure 5. Weight % as a function of temperature as obtained from the TGA tests on the samples.

Figure 5. Weight % as a function of temperature as obtained from the TGA tests on the samples.

Figure 6. Heat flow as a function of temperature as obtained from the DSC tests on the samples (a) and the pure media (b), respectively.

Figure 6. Heat flow as a function of temperature as obtained from the DSC tests on the samples (a) and the pure media (b), respectively.

Table 2. Peak data obtained from the DSC results for the samples and the pure media.