The force acting on the object is \( F = \alpha + \beta x^2 \). The work done by a variable force is given by:
\[
W = \int_{0}^{x} F \, dx
\]
Substituting \( F = \alpha + \beta x^2 \) into the equation:
\[
W = \int_{0}^{x} (\alpha + \beta x^2) \, dx
\]
We can evaluate the integral:
\[
W = \alpha x + \frac{\beta x^3}{3}
\]
Given that \( W = 5 \, {J} \) when \( x = 1 \, {m} \), we substitute these values:
\[
5 = \alpha \cdot 1 + \frac{\beta \cdot 1^3}{3}
\]
Since \( \alpha = 1 \, {N} \), this simplifies to:
\[
5 = 1 + \frac{\beta}{3}
\]
Solving for \( \beta \):
\[
5 - 1 = \frac{\beta}{3}
\]
\[
4 = \frac{\beta}{3}
\]
\[
\beta = 12 \, {N/m}^2
\]
Thus, the value of \( \beta \) is \( \boxed{12 \, {N/m}^2} \).