Please check this answer for me (Projectile Motion Question)

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Two rocks are launched simultaneously from points A and B with equal speeds but different angles, landing at each other's launch points. The problem involves calculating the minimum distance between the rocks during their flight, expressed in terms of the distance d and the launch angle θ. The equations of motion for both rocks are derived, leading to a quadratic equation for the distance between them. A key point in the discussion is the clarification that the minimum distance does not reach zero, prompting a reevaluation of the calculations. The final expression for the minimum distance incorporates trigonometric functions of the launch angle, indicating the complexity of the projectile motion involved.
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Two points A and B are located on the ground a certain distance d apart. Two rocks are launched simultaneously from points A and B with equal speeds but at different angles. Each rock lands at the launch point of the other. Knowing that one of the rocks is launched at an angle \vartheta> 45 degrees with the horizontal, what is the minimum distance between the rocks during the flight? Express your answer in terms of d and \vartheta

Hm.. this is a very hard problem for me so I hope anyone could help me check this over, as there are lots of rooms for mistakes. Thanks in advance.

4 base equations that I used for solving:
(1) x = V_{0}cos\vartheta t
(2)V_{2x} = V_{0}cos\vartheta
(3)y = V_{0}sin\vartheta t + \frac{1}{2}(-g)(t)^2
(4)V_{2y} = V_{0}sin\vartheta + (-g)(t)

D^2 = (x_{2} - x_{1})^2 + (y_{2} - {y_{1})^2

Rock 1:
x_{1} = V_{0}cos \vartheta t
y_{1} = V_{0}sin \vartheta t - \frac{1}{2}gt^2

Rock 2:
x_{2} = d - V_{0}cos \phi t
y_{2} = V_{0}cos \phi t - \frac{1}{2}gt^2

cos \phi = cos(90 - \vartheta) = sin \vartheta
sin \phi = sin (90 - \vartheta) = cos \vartheta

x_{2} - x_{1} = d - V_{0}(cos \vartheta + sin \vartheta)t
y_{2} - y_{1} = V_{0}(cos \vartheta - sin \vartheta)t

Let A = d, B = -V_{0}(cos \vartheta + sin \vartheta) and c = V_{0}(cos \vartheta + sin \vartheta)

D^2 = (A + Bt)^2 + (Ct)^2
= A^2 + 2ABt + B^2t^2 + C^2t^2
= A^2 + 2ABt + (B^2 + C^2)t

Recall quadratic equation = ax^2 + bx + c
Let a = B^2 + C^2, b = 2AB and c = A^2

Minimum = vertex
x = \frac{-b}{2a}
... y_{min} = a(\frac{-b}{2a})^2 + b(\frac{-b}{2a}) + c
= \frac{ab^2}{4a^2} - \frac{b^2}{2a} + c

... d_{min} = \sqrt\frac{4A^2B^2 - 2(4A^2B^2) + A^2}{4(B+C)}
= \sqrt\frac{-A^2B^2 + A^2(B^2 + C^2)}{B^2 + C^2}
= \sqrt\frac{A^2C^2}{B^2 + C^2}
 
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Substitute for A, B and C

d_{min} = \sqrt\frac{d^2V_{0}^2(cos \vartheta + sin \vartheta)^2}{[-V_{0}(cos \vartheta - sin \vartheta)]^2 + [V_{0}(cos \vartheta - sin \vartheta)]^2}

= \frac{dV_{0}(cos \vartheta + sin \vartheta)}\sqrt { V_{0}^2(1- 2cos \vartheta sin \vartheta) + V_{0}^2(1- 2cos \vartheta sin \vartheta)}
 
sorry for the separate messages.. but the preview keeps showing me my previous equations -_-

= \frac{dV_{0}(cos \vartheta + sin \vartheta)}{V_{0} \sqrt 2 ( 1 - 2 cos <br /> \vartheta sin \vartheta)}

= \frac{d(cos \vartheta + sin \vartheta)}{\sqrt 2 ( 1 - 2 cos <br /> \vartheta sin \vartheta)}
 
With d = 1 m, and \vartheta = 40 degrees, from your equations I get the minimum distance as 66 m, which does seem a bit too big.

In the quadratic equation you've assumed the distance hits zero. This is not the case:
A^2 + 2ABt + (B^2 + C^2)t^2 = D^2 \ne 0

So, your c should be: c = A2 - D2

EDIT:
I got |\mathbf{r}|_{min} = \frac{d}{2}\sqrt{(\sin(2 \theta)-1)^2+(2 \sin ^2 \theta - 1)^2}
But I'm not too convinced :)
 
Last edited:
oh yes 66m does seem unreasonably big.
 
Oh, I suppose there's no use trying to solve t from the quadratic equation (you'd just end up with the same variables).
You should rather figure out a way to compute t when distance is at its minimum.

Hint: There's a mathematical method for this.
 
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