Hi Anna A.!
There are several solutions for this answering this question. One way we can think about this is by using the work-energy theorem:
W = Fd = ΔKE
From here, we consider how the electric field strength, electrostatic force and charge are all related:
=> E = Fq*q-1 => Fq = qE
So, we can apply the equation above and substitute it into our work-energy theorem:
W = Fd = ΔKE
=> E = Fq*q-1 => Fq = qE
W = qEd = ΔKE
Now, we just rearrange, plug in and solve:
W = qEd = ΔKE ----> qEd = (1/2)m(vf2 - vo2)
2qEd/m = vf2 - vo2 => vf = √((2qEd/m) + vo2)
<=> √[2*(-1.6x10-19 C)(12x103 N*C-1)(4x10-2m)/(9.1x10-31kg) + (2x107m*s-1)2]
vf = 1.5x107 m*s-1
As we discussed above, there are other solutions to this problem. For instance, we could have obtained the same final equation using potential energy:
ΔUq = q*ΔV
Because the force here is one that is conservative, we can equate the potential energy to the kinetic energy:
ΔUq = q*ΔV = ΔKE
Now, we can substitute for the difference in potential:
ΔV = Ed
If we plug this into our equation, we obtain the same equation as that above:
ΔUq = q*ΔV = ΔKE
=> ΔV = Ed
ΔUq = q*Ed = ΔKE -------> vf = √((2qEd/m) + vo2)
Still, there are more solutions possible. But I think I'll leave it here!
Hope this helps!
Cheers