The shell's horizontal position
and vertical position
are given by
![x=v_0\cos55.0^\circ\,t](https://tex.z-dn.net/?f=x%3Dv_0%5Ccos55.0%5E%5Ccirc%5C%2Ct)
![y=v_0\sin55.0^\circ\,t-\dfrac g2t^2](https://tex.z-dn.net/?f=y%3Dv_0%5Csin55.0%5E%5Ccirc%5C%2Ct-%5Cdfrac%20g2t%5E2)
where
is the given speed of 1.70 x 10^4 m/s, and
is the acceleration due to gravity (taken here to be 9.80 m/s^2).
To find the horizontal range, you can use the range formula,
![x_{\rm max}=\dfrac{{v_0}^2\sin2\theta}g](https://tex.z-dn.net/?f=x_%7B%5Crm%20max%7D%3D%5Cdfrac%7B%7Bv_0%7D%5E2%5Csin2%5Ctheta%7Dg)
with
being the angle at which the shell is fired.
Alternatively, we can work backwards and deal with part (b) first:
(b) The time spent in the air is the time it takes for the shell to reach the ground. To find that, you solve for
in
:
![v_0\sin55.0^\circ\,t-\dfrac g2t^2=0\implies t\approx284\,\rm s](https://tex.z-dn.net/?f=v_0%5Csin55.0%5E%5Ccirc%5C%2Ct-%5Cdfrac%20g2t%5E2%3D0%5Cimplies%20t%5Capprox284%5C%2C%5Crm%20s)
(a) After this time, the shell will have traveled horizontally
![x=v_0\cos55.0^\circ(284\,\rm s)\approx2.77\times10^5\,\rm m](https://tex.z-dn.net/?f=x%3Dv_0%5Ccos55.0%5E%5Ccirc%28284%5C%2C%5Crm%20s%29%5Capprox2.77%5Ctimes10%5E5%5C%2C%5Crm%20m)