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MAXImum [283]
2 years ago
14

The range is the horizontal distance from the cannon when the pumpkin hits the ground. This distance is given by the product of

the horizontal velocity (which is constant) and the amount of time the pumpkin is in the air (which is determined by the vertical component of the initial velocity, as you just discovered). Set the initial speed to 14 m/s, and fire the pumpkin several times while varying the angle between the cannon and the horizontal. For which angle is the range a maximum (with the initial speed held constant)
Physics
1 answer:
SIZIF [17.4K]2 years ago
6 0

Answer:

x(max) = 20 m

Explanation:

In projectile shoot e have:

V₀y  = V₀*sin θ

V₀ₓ = V₀*cos θ

V₀  initial speed

θ  shotting angle

Vₓ = V₀ₓ = V₀*cos θ     during the trajectory

Vy  = V₀y  - g*t

And when  Vy = 0   h is maximun and the time to reach y maximum is half of the overall time.

According to that

Vy  =  0     V₀y = g*t       t  =  V₀y/g

t = 14* sinθ / 9,8

t = 1,43 *sinθ  s

And    overall time is T = 2* 1,43*sinθ

t = 2,86*sinθ

x = V₀ₓ * t   s

x = 14*cosθ * 2,86* sinθ

x = 40 * cosθ * sinθ

Lets take two very well know sin   cos pairs

for ∡ 30       ∡ 45     ∡60

and 30 and 60 are complementary angles for boths

cosθ * sinθ  is the same  ( 1/2)*(√3/2)

cosθ * sinθ  =  0,433     and

x = 40* 0,433

x = 17,32 m

For ∡ 45    boths   sin45    and  cos45   are equal  √2/2

In this case

x  =  40*(√2/2)*(√2/2)

x  =  40* 2/4

x = 20 m

And that is the maximum range

x(max) = 20 m

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\begin{aligned}\frac{d}{d q_{1}}[F] &= \frac{d}{d q_{1}} \left[\frac{k}{r^{2}}\, (q\, q_{1} - {q_{1}}^{2})\right] \\ &= \frac{k}{r^{2}}\, \left[\frac{d}{d q_{1}} [q\, q_{1}] - \frac{d}{d q_{1}}[{q_{1}}^{2}]\right]\\ &= \frac{k}{r^{2}}\, (q - 2\, q_{1})\end{aligned}.

Second derivative:

\begin{aligned}\frac{d^{2}}{{d q_{1}}^{2}}[F] &= \frac{d}{d q_{1}} \left[\frac{k}{r^{2}}\, (q - 2\, q_{1})\right] \\ &= \frac{(-2)\, k}{r^{2}}\end{aligned}.

The value of the coulomb constant k is greater than 0. Thus, the value of the second derivative of F with respect to q_{1} would be negative for all real r. F\! would be convex over all q_{1}.

By the convexity of \! F with respect to \! q_{1} \!, there would be a unique q_{1} that globally maximizes F. The first derivative of F\! with respect to q_{1}\! should be 0 for that particular \! q_{1}. In other words:

\displaystyle \frac{k}{r^{2}}\, (q - 2\, q_{1}) = 0<em>.</em>

2\, q_{1} = q.

q_{1} = q / 2.

In other words, the force between the two point charges would be maximized when the charge is evenly split:

\begin{aligned} \frac{q}{q_{1}} &= \frac{q}{q / 2} = 2\end{aligned}.

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