  In this paper the global mode structures of linear ion-temperature-gradient
(ITG) modes in tokamak plasmas are obtained by combining results from the local
gyrokinetic code GS2 with analytical theory. Local gyrokinetic calculations,
using GS2, are performed for a range of radial flux surfaces, ${x}$, and
ballooning phase angles, ${p}$, to map out the local complex mode frequency,
${\Omega_{0}(x,p)=\omega_{0}(x,p)+i\gamma_{0}(x,p)}$ for a single toroidal mode
number, ${n}$. Taylor expanding ${\Omega_{0}}$ about ${x=0}$, and employing the
Fourier-ballooning representation leads to a second order ODE for the amplitude
envelope, ${A\left(p\right)}$ , which describes how the local results are
combined to form the global mode. We employ the so-called CYCLONE base case for
circular Miller equilibrium model. Assuming radially varying profiles of
${a/L_{T}}$ and ${a/L_{n}}$, peaked at ${x=0}$, and with all other equilibrium
profiles held constant, ${\Omega_{0}(x,p)}$ is found to have a stationary
point. The reconstructed global mode sits at the outboard mid-plane of the
tokamak, with global growth rate, ${\gamma\sim}$Max${\left[\gamma_{0}\right]}$.
Including the radial variation of other equilibrium profiles like safety factor
and magnetic shear, leads to a mode that peaks away from the outboard
mid-plane, with a reduced global growth rate. Finally, the influence of
toroidal flow shear has also been investigated through the introduction of a
Doppler shift, ${\omega_{0} \rightarrow \omega_{0} - n\Omega_{\phi}^{\prime}
x}$, where ${\Omega_{\phi}}$ is the equilibrium toroidal flow, and a prime
denotes the radial derivative. The equilibrium profile variations introduce an
asymmetry into the global growth rate spectrum with respect to the sign of
${\Omega_{\phi}^{\prime}}$, such that the maximum growth rate is achieved with
non-zero shearing, consistent with recent global gyrokinetic calculations.
