Results of measurements on the thermoelectric power of 45 nm diameter interconnected nanowire networks consisting of pure Fe, dilute FeCu and FeCr alloys and Fe/Cu multilayers are presented. The thermopower values of Fe nanowires are very close to those found in bulk materials, at all temperatures studied between 70 and 320 K. For pure Fe, the diffusion thermopower at room temperature, estimated to be around − 15\documentclass[12pt]{minimal}
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				\begin{document}$$\upmu$$\end{document}μV/K from our data, is largely supplanted by the estimated positive magnon-drag contribution, close to 30\documentclass[12pt]{minimal}
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				\begin{document}$$\upmu$$\end{document}μV/K. In dilute FeCu and FeCr alloys, the magnon-drag thermopower is found to decrease with increasing impurity concentration to about 10\documentclass[12pt]{minimal}
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				\begin{document}$$\upmu$$\end{document}μV/K at 10\documentclass[12pt]{minimal}
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				\begin{document}$$\%$$\end{document}%impurity content. While the diffusion thermopower is almost unchanged in FeCu nanowire networks compared to pure Fe, it is strongly reduced in FeCr nanowires due to pronounced changes in the density of states of the majority spin electrons. Measurements performed on Fe(7 nm)/Cu(10 nm) multilayer nanowires indicate a dominant contribution of charge carrier diffusion to the thermopower, as previously found in other magnetic multilayers, and a cancellation of the magnon-drag effect. The magneto-resistance and magneto-Seebeck effects measured on Fe/Cu multilayer nanowires allow the estimation of the spin-dependent Seebeck coefficient in Fe, which is about − 7.6\documentclass[12pt]{minimal}
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				\begin{document}$$\upmu$$\end{document}μV/K at ambient temperature.