Step 1: Resolve the first force into components.
The force \(\vec{F_1}\) has magnitude \(4\;N\) and acts at an angle \(30^\circ\) above the positive \(x\)-axis.
Its \(x\)-component is
\[
F_{1x}=4\cos30^\circ
\]
\[
=4\left(\frac{\sqrt{3}}{2}\right)
\]
\[
=2\sqrt{3}\;N
\]
Its \(y\)-component is
\[
F_{1y}=4\sin30^\circ
\]
\[
=4\left(\frac12\right)
\]
\[
=2\;N
\]
Step 2: Write the components of the second force.
The second force \(\vec{F_2}\) acts along the positive \(y\)-axis with magnitude \(4\;N\).
Therefore,
\[
F_{2x}=0
\]
and
\[
F_{2y}=4\;N
\]
Step 3: Find the resultant force.
Total \(x\)-component of force:
\[
F_x=2\sqrt{3}
\]
Total \(y\)-component of force:
\[
F_y=2+4
\]
\[
=6
\]
Magnitude of resultant force:
\[
F=\sqrt{F_x^2+F_y^2}
\]
\[
=\sqrt{(2\sqrt{3})^2+6^2}
\]
\[
=\sqrt{12+36}
\]
\[
=\sqrt{48}
\]
\[
=4\sqrt{3}\;N
\]
\[
\approx 6.93\;N
\]
Step 4: Use Newton's second law.
Given mass,
\[
m=1\;kg
\]
Acceleration is
\[
a=\frac{F}{m}
\]
\[
=\frac{4\sqrt{3}}{1}
\]
\[
=4\sqrt{3}\;\text{m s}^{-2}
\]
\[
\approx 6.9\;\text{m s}^{-2}
\]
Step 5: Final conclusion.
Hence, the magnitude of acceleration is
\[
\boxed{6.9\;\text{m s}^{-2}}
\]