Let's set the midpoint of the rod as x=0. If we draw E vectors from -x and x at the point, we see that the vector components in y cancel and the components in x add. We can figure out the Ex from adding up the dEx from the dq along the line for -2≤x≤0 and double that to find the contribution from both parts of line charge.
The Ex component wil be Ecosθ for the triangle from the -x position on the line to the point (vertical position 1.45 m) The cos of the angle will be x/sqrt(x2 + 1.452)
It is also convenient to express dq as λdx where λ = 6.4 nC/2 m = 3.2 nC/m = 3.2 x 10-9 C/m
Recall that dE = (1/4πε0)dq/r2
The integral becomes (1/4πε0) integral from x = -2 to 0 of (λdx/(x2+1.452)(x/(x2+1.452))
This reduces to (3.2 x 10-9)/4πε0) integral from -2 to 0 of xdx/(x2+1.452)2 which is integrable by u sub.
Please consider a tutor. Take care (Remember to integral by 2 to obtain contribution from both parts of the line charge)