For a useful comparison, we need to ensure each wing has the same lift coefficient $C_L$. As span increases, assuming chord is constant, then the wing area and aspect ratio ($A$) also increases proportionally. Since wingtip vortex strength is related to the induced drag, you may have seen this relationship:
$$C_{D_i}=\frac{C_L^2}{\pi e A}$$
The larger the span, or aspect ratio, the smaller the induced drag (i.e. wingtip vortex) for the same lift coefficient. But why?
From the circulation theory of lift, any change in the circulation along the span will shed trailing vortices. In turn, these trailing vortices will induce downwash on the wing span. At the wingtip, the downwash rolls over and creates the wingtip vortex. Now if the span is short, the change of circulation will be larger, thereby inducing higher downwash all along the span, and the rollover at the tip will be stronger. If the span is longer, the change is circulation is gentler and less downwash/wingtip vortex is induced.
In the limit where the span becomes infinite, assuming the same $C_L$ for the whole wing, the circulation distribution is stretched to a constant value, such that the change in circulation along the span is zero, then no trailing vortex exists and the induced drag becomes zero as well.