Figure 3: Flight of an arrow without air resistance
When an arrow encounters no air resistance, the laws of projectile motion from high-school physics apply. Using x for the distance when it is x units away, and θ for the initial angle, we have this model for the trajectory of an arrow without air resistance:
12fx = tan(θ)x - 16
When the acceleration on the arrow is proportional to its velocity, the proportion factor is given by:
32gx = tan(θ) + log(200cos(θ)) - e
The range of flight is the time that y = 0. When y = 0, the definition of both gx and fx should be satisfied.
First, we investigate an arrow's flight without wind resistance. Exercise 6 in x. Rewrite f(x) so that the coefficients are careful with the scientific notation.
1. Let e = 4.
2. Look carefully at f(x), it is a quadratic polynomial.
3. Rewrite f(x) as f(x) = ax^2 + bx + c.
Enter a short answer.