MHB Calculating Elevation Angle to Hit Target at 100 m and 10 m

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To calculate the elevation angle needed to hit a target located 100 m away and 10 m high, with an initial velocity of 60 m/s and gravitational acceleration of 10 m/s², the equations of motion for both vertical and horizontal components are used. The time of flight is expressed in terms of the angle of elevation, leading to a quadratic equation in terms of the tangent of the angle. The solutions yield two valid angles for elevation, indicating multiple trajectories can hit the target. The discussion also touches on the derivation of a linear combination identity used in the calculations. The final step involves substituting the known values to find the specific angle of elevation.
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A target is located at the distance 100 m and height 10 m. How much is the elevation angle of the shooter to be able to hit the target if the initial velocity is 60 m/s and g = $$10m/s^2$$?

What I have done:
100 = 60sin$$\alpha$$t and 10 = 60sin$$\alpha$$t - $$\frac{1}{2}(10)t^2$$
$$t=\frac{5cos\alpha}{3}$$ and $$10=t(60sin\alpha)-t)$$
Dunno what to do from here on.
 
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Let's let $\theta$ be the angle of elevation. Let's orient our coordinate axes such that the vertical axis $y$ points up in the positive direction, and the horizontal axis $x$ points in the direction of motion in the positive direction.

For the vertical component of motion, we have:

$$a_y=-g$$

$$v_y=-gt+v_0\sin(\theta)$$

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

For the horizontal component of motion, we have:

$$a_x=0$$

$$v_x=v_0\cos(\theta)$$

$$x=v_0\cos(\theta)t$$

Let's eliminate the parameter $t$, by using $$t=\frac{x}{v_0\cos(\theta)}$$:

And so:

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

Multiply through by $\cos^2(\theta)$:

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

Using double-angle identities, and multiplying through by 2, we may write:

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

Arrange as:

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

Using a linear combination identity, we have:

$$\sqrt{x^2+y^2}\sin\left(2\theta-\arctan\left(\frac{y}{x}\right)\right)=y+\frac{g}{v_0^2}x^2$$

Solving for $\theta$, there results:

$$\theta=\frac{1}{2}\left(\arcsin\left(\frac{v_0^2y+gx^2}{v_0^2\sqrt{x^2+y^2}}\right)+\arctan\left(\frac{y}{x}\right)\right)$$

Now, all that's left is to plug in the given values. :)
 
Monoxdifly said:
A target is located at the distance 100 m and height 10 m. How much is the elevation angle of the shooter to be able to hit the target if the initial velocity is 60 m/s and g = $$10m/s^2$$?

$\Delta x = v_0\cos{\theta_0} \cdot t \implies t = \dfrac{\Delta x}{v_0\cos{\theta_0}} = \dfrac{100}{60\cos{\theta}}$

$\Delta y = v_0\sin{\theta_0} \cdot t - \dfrac{1}{2}gt^2 \implies 10 = 60\sin{\theta} \cdot \dfrac{5}{3\cos{\theta}} - 5\left(\dfrac{5}{3\cos{\theta}}\right)^2 \implies 10 = 100\tan{\theta} - \dfrac{125}{9} \sec^2{\theta}$

using the identity $\sec^2{\theta} = 1 + \tan^2{\theta}$ yields a quadratic equation in $\tan{\theta}$ ...

$0 = -43 + 180\tan{\theta} - 25\tan^2{\theta}$

the quadratic formula yields two valid solutions for $\tan{\theta}$ ...

$\tan{\theta} = \dfrac{18 \pm \sqrt{281}}{5}$
 
Yes, there should be two solutions, and in my post above, I should have included:

$$\sqrt{x^2+y^2}\sin\left(\pi-\left(2\theta-\arctan\left(\frac{y}{x}\right)\right)\right)=y+\frac{g}{v_0^2}x^2$$

As a means of getting the other. :)
 
MarkFL said:
Let's let $\theta$ be the angle of elevation. Let's orient our coordinate axes such that the vertical axis $y$ points up in the positive direction, and the horizontal axis $x$ points in the direction of motion in the positive direction.

For the vertical component of motion, we have:

$$a_y=-g$$

$$v_y=-gt+v_0\sin(\theta)$$

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

For the horizontal component of motion, we have:

$$a_x=0$$

$$v_x=v_0\cos(\theta)$$

$$x=v_0\cos(\theta)t$$

Let's eliminate the parameter $t$, by using $$t=\frac{x}{v_0\cos(\theta)}$$:

And so:

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

Multiply through by $\cos^2(\theta)$:

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

Using double-angle identities, and multiplying through by 2, we may write:

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

Arrange as:

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

Using a linear combination identity, we have:

$$\sqrt{x^2+y^2}\sin\left(2\theta-\arctan\left(\frac{y}{x}\right)\right)=y+\frac{g}{v_0^2}x^2$$

Solving for $\theta$, there results:

$$\theta=\frac{1}{2}\left(\arcsin\left(\frac{v_0^2y+gx^2}{v_0^2\sqrt{x^2+y^2}}\right)+\arctan\left(\frac{y}{x}\right)\right)$$

Now, all that's left is to plug in the given values. :)

Thank you! All comprehensible except the linear combination identity part. What's that and how was it derived?
 
Monoxdifly said:
Thank you! All comprehensible except the linear combination identity part. What's that and how was it derived?

Here's a link that describes the derivation of the identity:

Linear Combination of Sine and Cosine
 
Here is a little puzzle from the book 100 Geometric Games by Pierre Berloquin. The side of a small square is one meter long and the side of a larger square one and a half meters long. One vertex of the large square is at the center of the small square. The side of the large square cuts two sides of the small square into one- third parts and two-thirds parts. What is the area where the squares overlap?

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