Provided:
\[ |\vec{F}_1| = F, \quad |\vec{F}_2| = 3F \]
The resultant force \( |\vec{F}_R| \) equals the magnitude of the larger force:
\[ |\vec{F}_R| = 3F \]
The formula for the magnitude of the resultant force is:
\[ |\vec{F}_R|^2 = |\vec{F}_1|^2 + |\vec{F}_2|^2 + 2|\vec{F}_1||\vec{F}_2| \cos \theta \]
With values substituted:
\[ (3F)^2 = F^2 + (3F)^2 + 2 \times F \times 3F \cos \theta \]
After simplification:
\[ 9F^2 = F^2 + 9F^2 + 6F^2 \cos \theta \]
Rearranging the equation:
\[ 0 = 6F^2 \cos \theta \]
\[ \cos \theta = -\frac{1}{6} \]
Conclusion:
\[ \theta = \cos^{-1} \left( -\frac{1}{6} \right) \]
Given the relationship \( \cos \theta = \frac{1}{n} \),
it follows that:
\[ n = -6 \implies |n| = 6 \]