Because the detection in the laboratory takes place so distant from the nucleus, we'll assume the potential at the moment of detection is zero.
As a result, the potential difference is equal to the potential at the nucleus' surface. To get the latter, we'll utilize the traditional approach of calculating the potential as
whereis the nucleus' diameter. We're ignoring the fact that the alpha particle has a nonzero radius; nevertheless, because we don't know what it is, and because of its much lower size, we may fairly assume it is zero.
Rewriting the conservation of energy law, we get speed :
where the charge of the alpha particle is .
Substitute for , and we'll get :
This speed can be calculated numerically to be :
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