The mass undergoes a change in kinetic energy of
∆K = 1/2 (12 kg) [(26 m/s)² - (11 m/s)²] = 3330 J
By the work-energy theorem, the total work W performed on the mass is equal to ∆K. Assuming no friction, only the horizontal component of the applied force performs work on the mass.
Let F be the magnitude of this force, so that its horizontal component has mag. F cos(30.0°) = √3/2 F. It acts over a displacement of 22 m and performs 3330 J of work in the process, so that
3330 J = (√3/2 F) (22 m) ⇒ F = 1110√3/11 N ≈ 175 N