Answer:
a. y = (tanθ)x - 1/2gx²/(v₀cosθ)²
b. Range R = v₀²sin2θ/g
c. Time of flight T = 2v₀sinθ/g
Step-by-step explanation:
a. Show that the path followed by the object is parabolic
Let the vertical component of its velocity be v₁ = v₀sinθ and the horizontal component of its velocity be v₂ = v₀cosθ where v₀ = initial velocity of the projectile.
Now, for its vertical displacement Δy = v₁t - 1/2gt² (1)
Its horizontal displacement Δx = v₂t (2)
From (2) t = Δx/v₂
Substituting t into (1), we have
Δy = v₁(Δx/v₂) - 1/2g(Δx/v₂)²
= (v₁/v₂)Δx - 1/2g(Δx)²/(v₂)² =
= (v₀sinθ/v₀cosθ)Δx - 1/2g(Δx)²/(v₀cosθ)²
If we assume the initial position is at the origin, then Δx = x - 0 = x and Δy = y - 0 = y. So,
y = (tanθ)x - 1/2gx²/(v₀cosθ)² .
This is the required equation and it is a quadratic equation in x. Thus, the path followed by the projectile is parabolic.
b. The Range, R
The range, R is obtained when y = 0
So, 0 = (tanθ)x - 1/2gx²/(v₀cosθ)²
[(tanθ) - 1/2gx/(v₀cosθ)²]x = 0
x = 0 or (tanθ) - 1/2gx/(v₀cosθ)² = 0
x = 0 or (tanθ) = 1/2gx/(v₀cosθ)²
x = 0 or (tanθ)(v₀cosθ)² = 1/2gx
x = 0 or x = 2(sinθ/cosθ)(v₀cosθ)²/g
x = 0 or x = v₀²(2sinθ/cosθ)/g
x = 0 or x = v₀²sin2θ/g [sin2θ = 2sinθ/cosθ]
So its range R = x = v₀²sin2θ/g
c. Time of flight, T
The time of flight, T is obtained from (1) when Δy = 0 and t = T
So, 0 = v₁T - 1/2gT²
(v₁ - 1/2gT)T = 0
T = 0 or (v₁ - 1/2gT) = 0
T = 0 or v₁ = 1/2gT
T = 0 or T = 2v₁/g = 2v₀sinθ/g
So, the time of flight T = 2v₀sinθ/g