One of the Theorems relating work and energy is $$W_{C,A \to B} = - \Delta U,$$ where $W_{C, A \to B}$ represents the work done by the conservative forces between two points $A$ and $B$ and $\Delta U$ represents the change in the potential energy.
The work done by a force between two points $A$ and $B$ is defined as $$W_{A \to B} = \int_A^B \vec{F} \cdot \text{d}\vec{s}.$$
Since every force related to a potential (by the formula $\vec{F} = - \nabla U$) is a conservative force, it comes easily that:
$$\vec{F} = - \nabla U$$
$$\int_A^B \vec{F} \cdot \text{d}\vec{s} = - \int_A^B \nabla U \cdot \text{d}\vec{s}$$
$$ W_{C, A \to B} = - \left[ U(B) - U(A) \right]$$
$$ \therefore W_{C,A \to B} = - \Delta U$$
Since, when close to the ground, $U(h) = mgh$, you just have to calculate $U(A) - U(B) = mg \cdot h(A) - mg \cdot h(B)$.
$$W = 50 \cdot g \cdot 0 - 50 \cdot g \cdot 1.5 = - 75 \cdot g$$
$$ \therefore W = -750 \text{ J}$$
As you can see, the work is negative, since the weight force points downwards and the displacement points upwards.