Projectile Horizontal Range: Debunking the Intuition

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Discussion Overview

The discussion revolves around the horizontal range of a projectile, specifically addressing the counterintuitive nature of the relationship between launch angle and distance traveled. Participants explore the equations governing projectile motion, the implications of different launch angles, and the conditions affecting the range, including time of flight and horizontal distance.

Discussion Character

  • Exploratory
  • Technical explanation
  • Debate/contested
  • Mathematical reasoning

Main Points Raised

  • Some participants express confusion about the relationship between launch angle and horizontal range, noting that while the range is maximized at 45 degrees, the horizontal distance appears to be maximized at 0 degrees due to the equation x = v0 cos(θ) t.
  • Others clarify that while cos(θ) is maximum at θ = 0, the time of flight (t) is not constant and is influenced by the vertical motion of the projectile.
  • One participant points out that if θ = 0, the time of flight becomes zero, leading to a horizontal range of zero, which contradicts the idea of maximum horizontal distance.
  • Another participant introduces the concept that friction with the ground would halt a horizontally fired projectile immediately, suggesting that the range formula needs modification if the launch height is above ground level.
  • Participants discuss the differences between the equations for horizontal distance and range, particularly at θ = 0 degrees, and how these differences manifest in the context of projectile motion.

Areas of Agreement / Disagreement

Participants generally agree that the range is maximized at 45 degrees, but there is disagreement and confusion regarding the implications of launching at 0 degrees and how it affects horizontal distance and time of flight. The discussion remains unresolved regarding the interpretation of these relationships.

Contextual Notes

Limitations include assumptions about the absence of air resistance and friction, as well as the dependence on the initial height of the projectile. The discussion also highlights the need for clarity in distinguishing between horizontal distance and range under different launch conditions.

yitriana
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The equation describing the horizontal range of a projectile is

<br /> R = \frac{v_0^2}{g} \sin{2\theta}<br />

The previous equation states that the projectile wouldn't travel any distance if launched at 0 degrees. Further, the range of a projectile decreases from 45 to 0 degrees, but it seems counterintuitive, since the horizontal distance traveled is described by,

<br /> x = v_0 \cos{\theta_0}t<br />

Therefore, an angle of 0 would yield maximum x value.

I'm rather confused.
 
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Hi yitriana! :smile:

(have a theta: θ and a degree: º :wink:)
yitriana said:
… Further, the range of a projectile decreases from 45 to 0 degrees, but it seems counterintuitive, since the maximum distance traveled is when,

<br /> x = v_0 \cos{\theta_0}t<br />

Therefore, an angle of 0 would yield maximum x value.

Yes, the range is v0cosθ times t,

and cosθ is maximum when θ = 0,

but t is the time in the air, and it isn't constant.

sin2θ is maximum when 2θ = 90º, ie θ = 45º. :wink:
 
Write out the equations of motion for both vx and vy at time t=0 for initial velocity v0.

vx0 = v0 cosθ
vy0 = v0 sinθ

The maximum height of the projectile is given by
mgh = (1/2)mvy02; solve for h
the time the projectile is in the air is given by
t=2 sqrt(2 h/g)
The range is
R=vx0 t

α β γ δ ε ζ η θ ι κ λ μ ν ξ ο π ρ ς σ τ υ φ χ ψ ω
 
tiny-tim said:
Yes, the range is v0cosθ times t,

and cosθ is maximum when θ = 0,

but t is the time in the air, and it isn't constant.

sin2θ is maximum when 2θ = 90º, ie θ = 45º. :wink:

Yes, I see that R is maximized at θ = 45º

However, if we were to find the x distance of the projectile, wouldn't the distance be maximized when θ= 0, since vx0 = v0 cosθ is greatest?

How are the x distance and range different when θ = 0º?

I know they are different when θ != 0º

It seems logical that if the projectile goes in a straight line with constant velocity, it will travel farther than if the projectile goes in a curved path (at an angle) at constant x velocity.

So how do the two equations differ when launching a projectile at 0º??
 
The assumption is that friction with the ground will halt the horizontally fired projectile immediately. In other words, R = 0 when theta is zero, no matter what the initial velocity is. If your cannon is actually some vertical distance above the ground when it fires, then the formula for range needs some modification. Geometrically, you're looking for the intersection of a line (the ground) and a parabola (the trajectory).
 
yitriana said:
The equation describing the horizontal range of a projectile is

<br /> R = \frac{v_0^2}{g} \sin{2\theta}<br />

The previous equation states that the projectile wouldn't travel any distance if launched at 0 degrees. Further, the range of a projectile decreases from 45 to 0 degrees, but it seems counterintuitive, since the horizontal distance traveled is described by,

<br /> x = v_0 \cos{\theta_0}t<br />

Therefore, an angle of 0 would yield maximum x value.

I'm rather confused.

Another way to think about it is if \theta = 0 then

t = \frac{vsin\theta}{g} = \frac{vsin(0)}{g} = 0

since the time of flight is 0, then the distance x is 0.

Btw t = \frac{vsin\theta}{g} comes from doing v_f = v_0 + gt for the y direction, from t = 0, to t = t/2 (aka halfway through). This means v_f = 0 since the ball stops moving in the y direction at that point before starting to come down.
 
Thanks for all your replies!
 

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