The effective one-loop potential on \(R^{m+1}\times S^N\) spaces for massless tensor fields is evaluated. The Casimir energy is given as a value of \(\zeta-\) function by means of which regularization is made. In even- dimensional spaces the vacuum energy contains divergent terms coming from poles of \(\zeta(s,q)\) at \(s=1\), whereas in odd-dimensional spaces it becomes finite.