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Question

A plane is going in circles around an airport. The plane takes 3 minutes to complete one round. The angle of elevation of the plane from a point P on the ground at time t seconds is equal to that at time (t + 30) seconds. At time (t + x) seconds, the plane flies vertically above the point P. What is x equal to?

This question was previously asked in
CDS I 2019 Elementary Mathematics Previous Year Paper (03-Feb-2019)
The correct answer is

105 seconds

Understanding the Plane's Circular Motion

The problem describes a plane executing circular motion around an airport. We are given the time it takes to complete one full circle and information about its angle of elevation from a specific point P on the ground.

  • Time Period: The plane completes one round in 3 minutes. We convert this to seconds: \(T = 3 \text{ minutes} \times 60 \text{ seconds/minute} = 180 \text{ seconds}\).
  • Angular Speed: Since the plane completes a full circle (\(360^\circ\)) in 180 seconds, its angular speed (\(\omega\)) is constant. $\( \omega = \frac{360^\circ}{180 \text{ s}} = 2^\circ/\text{s} $\) This means the plane covers 2 degrees of its circular path every second.

Analyzing the Angle of Elevation Condition

We are told that the angle of elevation (\(\alpha\)) from point P at time \(t\) is the same as at time \(t + 30\) seconds. Mathematically, this condition is \(\alpha(t) = \alpha(t+30)\).

Let's consider the plane's angular position, denoted by \(\theta(t)\), measured in degrees from a reference direction. Assuming P is at the center of the horizontal projection of the circular path, the angle of elevation might be constant. However, the condition \(\alpha(t) = \alpha(t+30)\) suggests there's a dependency or symmetry involved. The angular position of the plane at time \(t\) is:

$\( \theta(t) = (\omega \times t) \pmod{360} = (2t) \pmod{360} $\)

The time difference given is 30 seconds. The angle covered during this time is:

$\( \Delta\theta = \omega \times 30 \text{ s} = (2^\circ/\text{s}) \times 30 \text{ s} = 60^\circ $\)

So, the plane's angular position changes by \(60^\circ\) between time \(t\) and time \(t+30\). The condition \(\alpha(t) = \alpha(t+30)\) often implies a symmetry in the setup. For instance, if the angle of elevation depends on the angular position \(\theta\) as \(f(\theta)\), the condition \(f(\theta(t)) = f(\theta(t+30))\) means \(f(\theta) = f(\theta + 60^\circ)\). This implies the function \(f\) is periodic with a \(60^\circ\) period. A common interpretation leading to a solvable problem is that the positions \(\theta\) and \(\theta+60^\circ\) are related such that the elevation angle is the same. This can happen if \(\theta = -(\theta + 60^\circ) \pmod{360}\), which simplifies to \(2\theta = -60^\circ \pmod{360}\), or \(2\theta = 300^\circ \pmod{360}\). Solving for \(\theta\) gives:

$\( \theta(t) \equiv 150^\circ \pmod{180} $\)

This means the condition \(\alpha(t) = \alpha(t+30)\) holds true when the plane's angular position is \(150^\circ\) or \(330^\circ\) within its 180-second cycle.

Calculating the Specific Time

We can now calculate the specific times (\(t\)) when these angular positions occur during the flight cycle:

  • For \(\theta(t) = 150^\circ\): $\( t_1 = \frac{150^\circ}{\omega} = \frac{150^\circ}{2^\circ/\text{s}} = 75 \text{ seconds} $\)
  • For \(\theta(t) = 330^\circ\): $\( t_2 = \frac{330^\circ}{\omega} = \frac{330^\circ}{2^\circ/\text{s}} = 165 \text{ seconds} $\)

The problem asks for the value of \(x\), where \(t+x\) is the time when the plane flies vertically above point P. The statement "vertically above the point P" implies that point P is directly below the center of the circular path. Let's define the position \(\theta = 0^\circ\) as the moment the plane is vertically above P. The cycle completes at \(t=180\) seconds, which is the next time the plane is vertically above P.

The question implies we should consider a time \(t\) that satisfies the angle condition \(\alpha(t) = \alpha(t+30)\), and then find how much additional time (\(x\)) passes until the plane is vertically above P. If there are multiple such times \(t\), we typically consider the earliest one. The first time the condition holds is \(t_1 = 75\) seconds.

So, we start at \(t = 75\) seconds. We need to find \(x\) such that the plane is vertically above P at time \(t+x = 75+x\). The next time the plane is vertically above P is at the end of the cycle, \(t_{overhead} = 180\) seconds.

Setting up the equation:

$\( 75 \text{ s} + x = 180 \text{ s} $\)

Solving for \(x\):

$\( x = 180 \text{ s} - 75 \text{ s} $\) $\( x = 105 \text{ seconds} $\)

Conclusion

By analyzing the plane's circular motion and the given condition on the angle of elevation, we find that the condition is met at \(t=75\) seconds (and \(t=165\) seconds). Starting from \(t=75\) seconds, the time it takes for the plane to reach the position vertically above point P (at \(t=180\) seconds) is \(x=105\) seconds.

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