The horizontal direction is usually represented by the x-axis.
So, we need to find the angle that the force vector \( \vec{F} = 4\hat{i} + 3\hat{j} - 5\hat{k} \) makes with the unit vector along the x-axis, which is \( \hat{i} \).
The magnitude of the force vector \( \vec{F} \) is:
$$ |\vec{F}| = \sqrt{(4)^2 + (3)^2 + (-5)^2} = \sqrt{16 + 9 + 25} = \sqrt{50} = 5\sqrt{2} $$
The dot product of the force vector \( \vec{F} \) and the unit vector along the horizontal \( \hat{i} \) is:
$$ \vec{F} \cdot \hat{i} = (4\hat{i} + 3\hat{j} - 5\hat{k}) \cdot (1\hat{i} + 0\hat{j} + 0\hat{k}) = 4(1) + 3(0) + (-5)(0) = 4 $$
The dot product of two vectors \( \vec{A} \) and \( \vec{B} \) is also given by \( \vec{A} \cdot \vec{B} = |\vec{A}| |\vec{B}| \cos \theta \), where \( \theta \) is the angle between them.
In our case, \( \vec{A} = \vec{F} \) and \( \vec{B} = \hat{i} \).
The magnitude of \( \hat{i} \) is \( |\hat{i}| = 1 \).
$$ \vec{F} \cdot \hat{i} = |\vec{F}| |\hat{i}| \cos \theta $$
$$ 4 = (5\sqrt{2})(1) \cos \theta $$
$$ \cos \theta = \frac{4}{5\sqrt{2}} $$
To rationalize the denominator:
$$ \cos \theta = \frac{4}{5\sqrt{2}} \times \frac{\sqrt{2}}{\sqrt{2}} = \frac{4\sqrt{2}}{5 \times 2} = \frac{4\sqrt{2}}{10} = \frac{2\sqrt{2}}{5} $$
Therefore, the angle \( \theta \) is:
$$ \theta = \cos^{-1} \left( \frac{2\sqrt{2}}{5} \right) $$