ANSWER
191.5 N
Step-by-step explanation
First, let's draw a free-body diagram of the forces acting on the safe,
By Newton's second law, we have that,

We know that the safe is moving to the right at a constant speed, which means that the acceleration is zero,

Solving for the force of friction,

The x-component of the applied force is,

Hence, the force of friction between the floor and the safe is 191.5 N.