  The Newtonian Euler-Poisson equations with attractive forces are the
classical models for the evolution of gaseous stars and galaxies in
astrophysics. In this paper, we use the integration method to study the blowup
problem of the $N$-dimensional system with adiabatic exponent $\gamma>1$, in
radial symmetry. We could show that the $C^{1}$ non-trivial classical solutions
$(\rho,V)$, with compact support in $[0,R]$, where $R>0$ is a positive constant
with $\rho(t,r)=0$ and $V(t,r)=0$ for $r\geq R$, under the initial condition
\begin{equation}
H_{0}=\int_{0}^{R}r^{n}V_{0}dr>\sqrt{\frac{2R^{2n-N+4}M}{n(n+1)(n-N+2)}}%
\end{equation} with an arbitrary constant $n>\max(N-2,0),$\newline blow up
before a finite time $T$ for pressureless fluids or $\gamma>1.$ Our results
could fill some gaps about the blowup phenomena to the classical $C^{1}$
solutions of that attractive system with pressure under the first boundary
condition.\newline In addition, the corresponding result for the repulsive
systems is also provided. Here our result fully covers the previous case for
$n=1$ in "M.W. Yuen, \textit{Blowup for the Euler and Euler-Poisson Equations
with Repulsive Forces}, Nonlinear Analysis Series A: Theory, Methods &
Applications 74 (2011), 1465--1470".
