This is a terrible question. In an Atwood's Machine, you can not change the total mass, and have the unbalanced forces be unchanged.
Proof:
[tex]a = \frac{M-m}{M+m}g[/tex]
[tex]\implies F_1 = Ma = \frac{M-m}{M+m}Mg ~~~~~~~(1)[/tex]
[tex]and ~F_2 = ma = \frac{M-m}{M+m}mg ~~~~~~~~~(2)[/tex]
Let us change the individual masses, so that [itex]M \longrightarrow M'~,~~m \longrightarrow m'[/itex]. Then again, we can write the equations for the unbalanced forces acting on the two blocks:
[tex]\implies F'_1 = M'a = \frac{M'-m'}{M'+m'}M'g ~~~~~(3)[/tex]
[tex]and ~F'_2 = m'a = \frac{M'-m'}{M'+m'}m'g ~~~~~~~(4)[/tex]
If the unbalanced forces are to remain unchanged, then [itex]F'_1=F_1~,~~F'_2=F_2[/itex]. So that gives us:
[tex]\frac{M-m}{M+m}M=\frac{M'-m'}{M'+m'}M'~~~~~~~~~~~~~(5)[/tex][tex]\frac{M-m}{M+m}m=\frac{M'-m'}{M'+m'}m'~~~~~~~~~~~~~~(6)[/tex]
Dividing (5) by (6) gives:
[tex]\frac{M}{m}=\frac{M'}{m'}~\implies \frac{M}{M}=\frac{m}{m'}[/tex]
Call the latter ratios [itex]\alpha[/itex], so that we have [itex]M' =M \alpha~, ~~m'=m\alpha[/itex].
Making these substitutions in (5) and (6) gives [itex]1=\alpha[/itex].
In other words, if the unbalanced forces are to remain unchanged, the individual masses must also be unchanged.