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Harnessing green hydrogen production from natural Red Sea water offers an innovative solution to address energy challenges. A one-pot fabrication method is used to create novel nanocomposite thin films with open-spherical shapes, utilizing copper sulfide/poly-O-amino benzenethiol decorated on copper oxide as a promising photocathode. After thorough analysis, a unique morphology characterized by open spherical shapes is projected, which contributes to improved optical absorption. The bandgap of the nanocomposite is 1.17 eV, enabling efficient absorption of light across the entire optical spectrum, extending up to 950 nm. Utilizing Red Sea water as an electrolyte, the generated J ph serves as an indicator of H2 gas production. The substantial J ph value of −0.82 mA cm−2 is achieved at −0.85 V under light illumination. Furthermore, J ph values exhibit variability, starting at −0.58 mA cm−2 (at 730 nm) and increasing to −0.75 mA cm−2 at a wavelength of 340 nm. The estimated hydrogen gas production rate reaches 1.5 µmole h−1 cm−2, translating to an impressive 15 µmole h−1 for every 10 cm². This remarkable rate underscores the effectiveness of the photocathode, especially given its fabrication through a single-step process that is suitable for mass production. In addition, its cost-effectiveness further enhances its appeal as a viable solution for renewable energy production for hydrogen gas generation from seawater.

Utilizing an innovative and highly light-absorbing photocathode, the direct conversion of hydrogen gas from Red Sea water is achieved. This involves creating a new nanocomposite thin film through a one-pot synthesis method, combining poly(O-chloroaniline) with trichalcogenides (MoS3) and MoO3 (MoS3–molebednium oxide/poly(o-chloroaniline)). This nanocomposite has remarkable morphological and optical properties with potential as a photocathode for hydrogen generation by harnessing the power of Red Sea water. This nanocomposite exhibits a unique semi-spherical architecture, with an average size of around 150 nm. These semi-spherical particles are surrounded by a dense network of fibers, forming a complex structure that provides ample space for trapping photons when exposed to light. The distinctive morphology significantly influences the optical properties of this nanocomposite, showing strong absorbance across a wide range of optical wavelengths up to ∼700 nm, with a promising bandgap of 1.75 eV. The hydrogen generation is quantified by measuring the generated photocurrent density (J ph) as a function of the light incidence frequency using various optical filters at a fixed potential of −0.8 V. The highest J ph values are recorded at −0.558 and −0.553 mA·cm−2 for wavelengths of 340 and 440 nm, respectively; the value reaches its maximum at the white light with a wavelength of −0.63 mA·cm−2. Elevating the temperature from 30°C to 50°C results in a substantial enhancement of the J ph values, increasing from −0.63 to −0.71 mA·cm−2, respectively. This temperature increase leads to a noteworthy improvement in incidnce photon to current conversion from 1.85% to 2.22%. This photoelectrode demonstrates not only cost-effectiveness but also eco-friendliness, making it an attractive choice for H2 generation by Red Sea water as a natural, environmentally friendly, and economically viable hydrogen source. Consequently, this study holds significant promise for industrial applications due to its economic and eco-friendly characteristics.

A one-pot synthesis approach was employed to create a composite nanorod structure (Mn2O3–MnO2–poly(m-methylaniline) or Mn2O3–MnO2–PmMA) on a polypyrrole (Ppy) film. Optoelectronic and solar cell thin film devices were constructed using n- and p-type layers of Mn2O3–MnO2–PmMA and Ppy, respectively. The optical characteristics of the n-layer, coupled with the morphological behavior of its nanorods, enhance optical absorbance efficiency, reducing the bandgap value to 2.48 eV. The behavior of the optoelectronic device is chiefly determined by the significantly higher current density (J ph) value of 0.017 mA/cm2 compared to the dark current density (J o) value of 0.002 mA/cm2. Additionally, the linear dynamic range is 85 dB, and the noise ratio is 12%. The optimized values for the photosensitivity (R) and detectivity (D) at 340 nm are 0.22 mA W−1 and 0.47 × 10⁸ Jones, respectively. Even at 540 nm, these values decrease to 0.08 and 0.2 × 10⁸ Jones, respectively. For solar cell behavior, the short-circuit current (J SC) and open-circuit voltage (V OC) at 540 nm are determined, yielding values of 0.001 mA/cm2 and 0.98 V, respectively. The outstanding performance of this optoelectronic device, coupled with its solar cell behavior, positions the thin film material for a dual role in various industrial applications.

The synthesis of rod-shaped Mo(vi) trichalcogenide–Mo(vi) oxide, cleverly adorned on a poly(1-H pyrrole) (P1HP) matrix (MoS3–MoO3/P1HP), is achieved through a one-pot preparation method. This process occurs under the pyrrole oxidation employing the oxidizing agent Na2MoO4. Notably, this oxidation process facilitates the direct incorporation of the inorganic constituents into the polymer matrix. Of particular significance is the material’s bandgap, which is optimally situated at 1.4 eV, rendering it highly suitable for its intended applications. The material assumes a rod-like structure, characterized by an average length of 400 nm and width of 30 nm, further enhancing its desirability. In practice, this thin film serves as an exceptionally promising photoelectrode. It finds its forte in the generation of hydrogen from sewage water, achieving an impressive efficiency rate of 12.66%, specifically at 340 nm. In addition to that, it boasts a remarkable hydrogen generation rate of 1.2 moles·h−1·cm−2. Moreover, the material exhibits remarkable versatility in its response to light. Its sensitivity to monochromatic light across a broad optical spectrum (UV till IR), underscores its potential for hydrogen generation applications for industrial applications.

Herein, the synthesis of a sensor for the determination of lead (Pb2+) ions via the intercalation of iodide ions into the polypyrrole matrix is performed. It demonstrated a Nernstian slope of 31.7 mV/decade, indicating a linear response within the concentration range of 10−5–10−1 M. The detection limit achieved is 9.10−6 M, indicating the sensor’s sensitivity to low concentrations of Pb2+. The effectiveness of the Ppy/I− sensor in Pb2+ sensing is confirmed through cyclic voltammetry, where a peak potential of −0.2 V is observed. The sensitivity of the sensor for Pb2+ detection is measured to be 2 µA/M. Moreover, the Ppy/I− sensor exhibits a negative response to interfering ions, which enhances its selectivity for Pb2+ detection. Furthermore, when tested with natural water samples such as tap or underground water, which are typically free of lead ions, the sensor demonstrates a negative response to normal interfering ions commonly found in such samples. The Ppy/I− sensor offers several advantages, including the ability to detect Pb2+ ions at very low concentrations, a flexible and adaptable design, and a cost-effective preparation technique. These features make it a promising tool for accurate and efficient detection of Pb2+ ions.

The development of a photocathode based on a Pb(ii)-iodide/poly(1H-pyrrole) porous spherical (PbI2/P1HP PS) nanocomposite has been successfully achieved in the efficient production of H2 gas from Red Sea water. The distinguishable spherical and porous shapes of these nanocomposites are characterized by a minimum surface measuring approximately 25 nm. This structural configuration, coupled with the nanocomposite’s substantial light absorbance, results in a modest bandgap of 2.4 eV. This turns the nanocomposite into a highly promising candidate for renewable energy applications, particularly for H2 gas generation from natural sources like Red Sea water. The economic viability of the PbI2/P1HP PS nanocomposite, relying on a glass substrate, mass production, and straightforward fabrication techniques, adds to its promising profile for H2 gas evolution. The photocathode exhibits significant potential for H2 gas production, with a notable current density (J ph) value of 1.0 mA·cm−2 in a three-electrode cell configuration. The IPCE reaches 3.1%, reflecting the successful evolution of 24 µmol·h−1 10 cm2 of the photocathode. Importantly, the use of natural Red Sea water as an electrolyte underscores a key feature for H2 gas production: utilizing freely available natural resources. This aspect holds considerable promise for industrial applications, emphasizing the environmentally sustainable nature of the photocathode.

In this review, the transformative role of polymer nanocomposites in hydrogen production from challenging water sources is explored. Their catalytic efficiency and unique properties are highlighted, making them vital for overcoming complexities in hydrogen generation. Polymer nanocomposites demonstrate exceptional adaptability to various water compositions, including wastewater and saline water, enhancing efficiency, stability, and compatibility. In this review, the significance of these nanomaterials in the sustainable energy landscape is underscored, showcasing their ability to outperform conventional methods. Key breakthroughs in catalytic efficiency and adaptability are emphasized, illustrating their crucial role in clean hydrogen production. Looking forward, in this review, potential applications of polymer nanocomposites in diverse fields, from industrial processes to energy sector advancements, are identified. This synthesis of findings not only enhances the understanding but also sets the stage for the widespread adoption of polymer nanocomposites in meeting the global demand for sustainable hydrogen production. [ABSTRACT FROM AUTHOR]