Where can the water jet spray?

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Discussion Overview

The discussion revolves around the problem of determining the boundary of a water jet spray from ground level on flat ground, considering various angles and initial velocity while ignoring drag. The focus is on deriving an equation that describes the reach of the water jet.

Discussion Character

  • Exploratory, Homework-related, Mathematical reasoning

Main Points Raised

  • One participant describes the scenario of a water jet spraying from ground level at any angle between $0$ and $\pi$ with an initial velocity $v_0$.
  • Another participant requests hints on how to begin solving the problem, indicating a need for guidance on the mathematical approach.
  • A third participant offers a hint in response to the request for help, suggesting a collaborative exploration of the problem.

Areas of Agreement / Disagreement

The discussion does not present any consensus or resolution, as participants are still in the initial stages of exploring the problem and seeking guidance.

MarkFL
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Consider a water jet that sprays from ground level on flat ground. The jet can spray at any angle $0<\theta<\pi$ along some horizontal axis, that is in one vertical plane. The jet sprays water at a velocity of $v_0$. Ignoring drag, find an equation that describes the boundary between where water can reach and where it cannot.
 
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Hi MarkFL,

I'm hoping to get some hint on how to at least start to work on the problem...:o
 
anemone said:
Hi MarkFL,

I'm hoping to get some hint on how to at least start to work on the problem...:o

Well, since you asked so nicely...sure no problem! (Sun)

Hint:

I would begin with the parametric equations of motion:

$$\tag{1}x=v_0\cos(\theta)t$$

$$\tag{2}y=-\frac{g}{2}t^2+v_0\sin(\theta)t$$

To eliminate the parameter $t$, we solve (1) for $t$ and substitute into (2) to get:

$$\tag{3}y=\tan(\theta)x-\frac{g}{2v_0^2\cos^2(\theta)}x^2$$

Using $$\frac{1}{ \cos^2(\theta)}= \sec^2(\theta)= \tan^2(\theta)+1$$ (3) becomes:

$$\tag{4}y=\tan(\theta)x-\frac{g}{2v_0^2}\left(\tan^2(\theta)+1 \right)x^2$$

Now, using the substitution:

$$u=\tan(\theta)$$

we get the parametrization:

$$\tag{5}y=ux-\frac{g}{2v_0^2}\left(u^2+1 \right)x^2$$

Now, let the boundary we seek be denoted by $$f(x)$$. What can we say about the intersection of $y$ and $f(x)$?
 
Solution:

Continuing from the hint I gave above, we will equate $y=f(x)$ and obtain the quadratic in $u$ in standard form:

$$u^2-\frac{2v_0^2}{gx}u+\left(1+\frac{2v_0^2f(x)}{gx^2} \right)=0$$

Because $y$ will only ever be tangent to $f(x)$ as it is the boundary, we know therefore that the discriminant must be zero, giving us:

$$\left(-\frac{2v_0^2}{gx} \right)^2-4\left(1+\frac{2v_0^2f(x)}{gx^2} \right)=0$$

$$\left(\frac{v_0^2}{gx} \right)^2=1+\frac{2v_0^2f(x)}{gx^2}$$

And then solving for $f(x)$, we find:

$$f(x)=-\frac{g}{2v_0^2}x^2+\frac{v_0^2}{2g}$$
 

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