A cage in a mine-shaft descends with 2 ft/s2 units of acceleration. After it has been in motion for 10 seconds a particle is dropped on it from the top of the shaft with 32 ft/s2. What time elapses before the particle hits the cage?
This problem involves analyzing the motion of two separate objects: a descending cage in a mine-shaft and a particle dropped from the top of the shaft. The key is to determine the time it takes for the particle to hit the cage, considering their different initial conditions and acceleration values.
First, let's understand the state of the cage at the moment the particle is dropped. The cage starts from rest and descends with a constant acceleration of \(2 \text{ ft/s}^2\). The particle is dropped after the cage has been in motion for \(10\) seconds.
We can calculate the distance covered by the cage and its velocity at \(t_0 = 10 \text{ seconds}\) using the equations of motion:
1. Displacement of the cage in the first 10 seconds (\(s_{c0}\)):
Using the formula \(s = ut + \frac{1}{2}at^2\):
\(s_{c0} = u_c t_0 + \frac{1}{2}a_c t_0^2\)
\(s_{c0} = (0 \text{ ft/s})(10 \text{ s}) + \frac{1}{2}(2 \text{ ft/s}^2)(10 \text{ s})^2\)
\(s_{c0} = 0 + \frac{1}{2}(2)(100)\)
\(s_{c0} = 100 \text{ ft}\)
2. Velocity of the cage at 10 seconds (\(v_{c0}\)):
Using the formula \(v = u + at\):
\(v_{c0} = u_c + a_c t_0\)
\(v_{c0} = 0 \text{ ft/s} + (2 \text{ ft/s}^2)(10 \text{ s})\)
\(v_{c0} = 20 \text{ ft/s}\)
So, when the particle is dropped, the cage is \(100 \text{ ft}\) below the top of the shaft and moving downwards at \(20 \text{ ft/s}\).
Let's consider the time \(t\) as the duration *after the particle is dropped* until it hits the cage. We will set our reference point (origin) at the top of the shaft, with the downward direction as positive.
The particle is dropped from the top of the shaft, meaning its initial velocity is zero. It accelerates due to gravity.
The displacement of the particle from the top of the shaft after time \(t\) is:
\(s_p(t) = u_p t + \frac{1}{2}a_p t^2\)
\(s_p(t) = (0)t + \frac{1}{2}(32)t^2\)
\(s_p(t) = 16t^2\)
At the moment the particle is dropped (which is \(t=0\) for our new time reference), the cage is already at \(100 \text{ ft}\) from the top and has an initial downward velocity of \(20 \text{ ft/s}\). It continues to accelerate at \(2 \text{ ft/s}^2\).
The displacement of the cage from the top of the shaft after time \(t\) is:
\(s_c(t) = s_{c0} + v_{c0}t + \frac{1}{2}a_c t^2\)
\(s_c(t) = 100 + 20t + \frac{1}{2}(2)t^2\)
\(s_c(t) = 100 + 20t + t^2\)
The particle hits the cage when their displacements from the top of the shaft are equal. So, we set \(s_p(t) = s_c(t)\):
\(16t^2 = 100 + 20t + t^2\)
Rearrange the equation to form a standard quadratic equation (\(At^2 + Bt + C = 0\)):
\(16t^2 - t^2 - 20t - 100 = 0\)
\(15t^2 - 20t - 100 = 0\)
To simplify, divide the entire equation by \(5\):
\(3t^2 - 4t - 20 = 0\)
Now, we use the quadratic formula to solve for \(t\):
\(t = \frac{-B \pm \sqrt{B^2 - 4AC}}{2A}\)
Here, \(A=3\), \(B=-4\), \(C=-20\).
\(t = \frac{-(-4) \pm \sqrt{(-4)^2 - 4(3)(-20)}}{2(3)}\)
\(t = \frac{4 \pm \sqrt{16 + 240}}{6}\)
\(t = \frac{4 \pm \sqrt{256}}{6}\)
\(t = \frac{4 \pm 16}{6}\)
This gives two possible values for \(t\):
Since time cannot be negative, we discard \(t_2 = -2 \text{ seconds}\).
Therefore, the time elapsed before the particle hits the cage is \(t = \frac{10}{3} \text{ seconds}\).
This can also be expressed as a mixed number:
\(t = 3 \frac{1}{3} \text{ seconds}\)
| Parameter | Value |
|---|---|
| Cage acceleration (\(a_c\)) | \(2 \text{ ft/s}^2\) |
| Particle acceleration (\(a_p\)) | \(32 \text{ ft/s}^2\) |
| Time before particle drop | \(10 \text{ s}\) |
| Cage displacement in 10s | \(100 \text{ ft}\) |
| Cage velocity at 10s | \(20 \text{ ft/s}\) |
| Quadratic equation solved | \(3t^2 - 4t - 20 = 0\) |
| Time for particle to hit cage | \(3 \frac{1}{3} \text{ seconds}\) |
The problem is a classic example of relative motion and involves applying equations of motion for objects under constant acceleration. Carefully setting up the initial conditions and displacement equations for both the cage and the particle is crucial for finding the correct time of collision.
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