To solve the problem, we start by considering a vector \(\vec{v}\) represented in a three-dimensional space. The vector \(\vec{v}\) is inclined at certain angles to the coordinate axes and lies in the first octant. Let's denote the direction cosines of this vector as \(\text{cos}(\alpha)\), \(\text{cos}(\beta)\), and \(\text{cos}(\gamma)\) corresponding to the x, y, and z axes, respectively.
Given that:
We can calculate the direction cosines using the given angles:
Since the sum of the squares of the direction cosines is 1, we have:
\(\text{cos}^2(\alpha) + \text{cos}^2(\beta) + \text{cos}^2(\gamma) = 1\)
Substitute the known values:
\(\left(\frac{1}{2}\right)^2 + \left(\frac{1}{\sqrt{2}}\right)^2 + \text{cos}^2(\gamma) = 1\)
Solve for \(\text{cos}^2(\gamma)\):
\(\frac{1}{4} + \frac{1}{2} + \text{cos}^2(\gamma) = 1\)
\(\text{cos}^2(\gamma) = 1 - \frac{3}{4} = \frac{1}{4}\)
Thus, \(\text{cos}(\gamma) = \frac{1}{2}\) or \(-\frac{1}{2}\). Since the angle with the z-axis is acute, \(\text{cos}(\gamma) = \frac{1}{2}\).
The direction ratios of the line representing the vector \(\vec{v}\) are proportional to the direction cosines: \((1/2, 1/\sqrt{2}, 1/2)\). Hence, the direction ratios can be taken as \((1, \sqrt{2}, 1)\).
Now, for the plane passing through the points \((\sqrt{2},-1,1)\) and \((a, b, c)\) which is normal to \(\vec{v}\), we use the plane equation formed using the direction ratios as the normal vector:
The equation of the plane is \(1(x - \sqrt{2}) + \sqrt{2}(y + 1) + 1(z - 1) = 0\), which simplifies to:
\(x + \sqrt{2}y + z = \sqrt{2} - \sqrt{2} + 1 = 1\).
Thus, the correct answer, where the equation holds, is: \(a+\sqrt{2} b+c=1\).