Given:
Relationship between work and surface tension:
When a film is removed from the surface, work is done against surface tension. The work done is:
$$W = \gamma_{\text{film}} \times \Delta A - \gamma_{\text{water}} \times \Delta A$$
This represents the work to remove the film and expose water underneath.
However, for a simpler approach, the work to decrease coverage relates directly to the surface tension of the film:
$$W = \gamma_{\text{film}} \times \Delta A$$
Calculation:
$$\gamma_{\text{film}} = \frac{W}{\Delta A}$$
$$\gamma_{\text{film}} = \frac{25.0 \times 10^{-7}}{1 \times 10^{-4}}$$
$$\gamma_{\text{film}} = \frac{25.0 \times 10^{-7}}{10^{-4}}$$
$$\gamma_{\text{film}} = 25.0 \times 10^{-3}$$
$$\gamma_{\text{film}} = 0.025 \text{ N/m}$$
Wait, this gives 0.025, which is outside the range. Let me reconsider.
Alternative interpretation:
The work to decrease coverage by removing the film involves both surfaces (film-air and film-water interfaces):
$$W = (\gamma_{\text{water}} - \gamma_{\text{film}}) \times \Delta A$$
$$25.0 \times 10^{-7} = (0.072 - \gamma_{\text{film}}) \times 1 \times 10^{-4}$$
$$\gamma_{\text{film}} = 0.072 - \frac{25.0 \times 10^{-7}}{1 \times 10^{-4}}$$
$$\gamma_{\text{film}} = 0.072 - 0.025 = 0.047 \text{ N/m}$$
Answer: 0.047 N/m