I am in a course currently studying this topic, and this is how I understand and solved the problem:
Electric field due to a continuous charge distribution:
E (as a vector) = [tex]\int[/tex]kdq / r^2 (in r vector direction)
So, dE = kdq / r^2 = k[tex]\lambda[/tex]dx / r^2
The E field has both x and y component, but if you draw the diagram as I see it, there is point p in the middle and directly above the uniformly charged line (ie along a line of symmetry). In that case, the x component will be 0 and there will just be the y.
Also, since this point is directly in the middle it cuts the charged line half, and so we let it's length (L) be L/2 until the intersection point and L/2 past the intersection point. This makes two right triangles with [tex]\Theta[/tex](1) representing the top angle for the first, and [tex]\Theta[/tex](2) representing the top angle for the second. It is difficult to explain this without a drawing...
So, we just need to find the y component of the E field:
E(y component) = dEcos[tex]\Theta[/tex] = (k[tex]\lambda[/tex]dx / r^2) (y / r) = k[tex]\lambda[/tex]ydx/r^3
You can use trig substitution to solve this integral or use some relationships in the graph to simplify it. Notice cos[tex]\Theta[/tex](2) = y / r. So, 1/r = cos[tex]\Theta[/tex](2) / y.
Also, tan[tex]\Theta[/tex] = x / y. So, x = ytan[tex]\Theta[/tex] and dx = ysec^2[tex]\Theta[/tex] d[tex]\Theta[/tex].
Plugging this stuff in we get dE(y) = k[tex]\lambda[/tex]yysec^2[tex]\Theta[/tex]d[tex]\Theta[/tex]cos^3[tex]\Theta[/tex](2) / y^3
Simplifying should get k[tex]\lambda[/tex]cos[tex]\Theta[/tex]d[tex]\Theta[/tex] / y
E(y) = k[tex]\lambda[/tex] / y [tex]\int[/tex]cos[tex]\Theta[/tex]d[tex]\Theta[/tex]
Solving this integral gives k[tex]\lambda[/tex] / y (sin[tex]\Theta[/tex](2) - sin[tex]\Theta[/tex](1))
Since [tex]\Theta[/tex](2) = -[tex]\Theta[/tex](1) in the graph, the sines can be written as (sin[tex]\Theta[/tex] - sin(-[tex]\Theta[/tex])) = 2sin[tex]\Theta[/tex]
Thus, E(y) = (2k[tex]\lambda[/tex] / y) sin[tex]\Theta[/tex]
Notice from the graph that sin[tex]\Theta[/tex] = x/r = (1/2L)/([tex]\sqrt{(1/2L)^2 + y^2}[/tex]
So, E(y) = (2k[tex]\lambda[/tex]/y) ((1/2L)/([tex]\sqrt{(1/2L)^2 + y^2}[/tex])
The expression [tex]\lambda[/tex]L can be rewritten as Q, since it is the charge per unit length. So, on top, the 2 and (1/2) cancel leaving you with just kQ in the numerator.
Plugging in the numbers gives (8.99x10^9)(7x10^-6) / ((.69) * ([tex]\sqrt{1/2(.25)^2 + (.69)^2}[/tex]))
The resulting calculation is 128042.6956 N/C