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Question 3
A particle is projected from a point P with speed 60 m s-1 at an angle of 30° to the horizontal. At the same time a second particle is projected from a point Q with ... show full transcript
Step 1
Answer
To find sin β, we start by analyzing the vertical components of the velocities. For the particle from point P:
The vertical velocity is given by:
Now considering the time of flight until the two particles collide (let's denote this time as t):
For the particle from point Q, the vertical distance covered can be described using the equation of motion: where (u_y = 50 \sin \beta).
Setting equal the vertical components:
On rearranging and cancelling t (as t > 0):
For simplicity, assuming standard gravity g = 9.81 m/s², we can deduce:
At the horizontal level, we have |PQ|=100m, so we can obtain more relations between the two angles. Eventually, solving simultaneously leads us to:
After simplifications:
Step 2
Answer
Using the projectiles, we resolve both into horizontal and vertical components:
For particle P:
For particle Q:
From our earlier calculations of t, substitute back to calculate |PR|:
Using the equations for both horizontal and vertical motions, and equating gives us:
Gain the total:
Upon computing with values substituted:
Step 3
Answer
For the particle projected up the inclined plane:
The time of flight t for the first particle is derived from: This results in:
Similarly, for the second particle:
The ratio of their times becomes:
Step 4
Answer
Applying the range formula, with θ as 45°:
The range R becomes: = \frac{u^2}{g}, = \frac{u^2{}{sin² θ}}{g \cos θ}$$
For θ as 45°:
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