Some people use U for the potential, others use V. Let it be V.
The force required to move the charge is opposite to the electric force. When you integrate the electric force from zero to 1.25 m, it is the same as integrating the opposite force from 1,25 to 0.
The potential at a point A is defined as the negative work done by the electric field when a unit positive charge moves from the reference point P0,where the potential is zero, to A.
V(A)=-\int_{P_0}^A{\vec{E} d\vec{r}}
In case of a point charge we choose the potential zero at infinity. The same holds for a ring of charge: The potential along the axis is V(x)=kQ/(x^2+a^2)^0.5, and it is zero at the limit when x tends to infinity.
If the zero of the potential is at infinity
V(A)=\int_A^\infty{\vec{E} d\vec{r}}.
As the integration is additive,
V(A)=\int_A^B{\vec{E} d\vec{r}}+\int_B^\infty{\vec{E} d\vec{r}},
\int_A^B{\vec{E} d\vec{r}}=V(A)-V(B)=-\Delta V
The work done by the electric field when a charge q moves
from point A to B is equal to the integral of the electric force, qE :
W(AB)=q\int_A^B{\vec{E} d\vec{r}}=q[V(A)-V(B)]=-q\Delta V,
the same as the negative potential difference multiplied by q.
The work required to move the charge from A to B, done some external force against the electric field, is just the opposite, q[V(B)-V(A)].
Your potential is kQ/(x^2+a^2)^0.5, and the work required to move the charge q from x=1.25 m to x=0 is
W=kqQ(\frac{1}{a}-\frac{1}{\sqrt{1.25^2+a^2}}).