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A subway train starts from rest at a station and accelerates at a rate of \(1.60 \mathrm{~m} / \mathrm{s}^{2}\) for \(14.0 \mathrm{~s}\). It runs at constant speed for \(70.0 \mathrm{~s}\) and slows down at a rate of \(3.50 \mathrm{~m} / \mathrm{s}^{2}\) until it stops at the next station. Find the total distance covered.

Short Answer

Expert verified
The total distance covered by the subway train is the sum of the distances covered in the acceleration phase, constant speed phase and deceleration phase.

Step by step solution

01

Compute the Speed after Acceleration

Calculate the speed after acceleration using the formula speed = acceleration x time. Here, acceleration \(a_1\) = 1.60 m/s² and time \(t_1\) = 14.0 s. Than gives us speed = \(a_1 \times t_1\).
02

Calculating Distance Covered in the Acceleration Phase

Compute the distance covered in the acceleration phase using the formula distance = initial speed x time + 0.5 x acceleration x time^2. We already know that initial speed \(u_1\) = 0, time \(t_1\) = 14.0 s and acceleration \(a_1\) = 1.60 m/s². This gives us distance = \(u_1 \times t_1 + 0.5 \times a_1 \times t_1^2\).
03

Calculating Distance Covered in the Constant Speed Phase

Calculate distance covered in the constant speed phase using the formula distance = speed x time. Here, speed is the final speed after acceleration, and time \(t_2\) = 70 s. Hence, distance = speed x \(t_2\).
04

Calculating Distance Covered in the Deceleration Phase

Compute the distance covered in deceleration phase using the formula distance = initial speed x time + 0.5 x deceleration x (time^2). We know that initial speed \(u_2\) equals final speed after acceleration phase, deceleration \(a_2\) = 3.50 m/s² and time \(t_3\) should be determined by dividing speed \(u_2\) by deceleration \(a_2\) as the train comes to rest finally. Then, distance = \(u_2 \times t_3 + 0.5 \times a_2 \times t_3^2\).
05

Calculating the Total Distance Covered

Add up all distances calculated in each stage. The result would be the total distance covered.

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Key Concepts

These are the key concepts you need to understand to accurately answer the question.

Uniformly Accelerated Motion
When an object is accelerating at a constant rate, it is said to be in uniformly accelerated motion. This concept is incredibly useful in physics, as many dynamic systems in both natural and engineered scenarios exhibit this kind of motion. Let's consider a subway train that starts from rest. This means that initially, its speed is zero. However, the train doesn’t just jump to its cruising speed instantaneously; it accelerates over time.
In the case of our subway train, it accelerates at a rate of 1.60 m/s² for 14.0 seconds. The acceleration is uniform or constant, hence the term 'uniformly accelerated motion'. Understanding this concept allows us to predict how an object will behave over time when subjected to a constant force. Additionally, it's the basis for several important physics equations that enable us to calculate variables such as distance, velocity, and time during such motion.
Equations of Motion
The equations of motion are a set of formulas that describe the relationship between velocity, acceleration, distance, and time. They are essential for solving problems in kinetics, like our subway train scenario. There are four primary equations, but in the solution provided, we use two of them:
  • To calculate velocity: \( v = u + at \), where \( v \) is final velocity, \( u \) is initial velocity, \( a \) is acceleration, and \( t \) is time.
  • For the distance: \( s = ut + \frac{1}{2}at^2 \) where \( s \) is distance, and the other variables are as previously defined.
These equations assume uniformly accelerated motion and no other forces acting on the object besides the acceleration (like air resistance). By applying these equations, we can analyse each phase of the train’s journey and calculate distances covered during acceleration, constant velocity, and deceleration.
Distance Calculation in Physics
Calculating the distance an object travels over a period of time is a core part of physics. In our example, we examine a train moving through three distinct phases: acceleration, constant speed, and deceleration. Each phase requires a different approach:
  • During acceleration, the distance is found using \( s = ut + \frac{1}{2}at^2 \), where initial speed \( u \) is zero.
  • At a constant speed, the formula simplifies to \( s = vt \), where \( v \) is the constant speed and \( t \) is the time.
  • The deceleration phase has a similar formula to acceleration, but deceleration is used instead.
By calculating distances for each phase separately and then combining them, we get the total distance traversed by the train during its journey from one station to the next.
Deceleration
Deceleration, often also referred to as negative acceleration, is the rate at which an object slows down. It is the same as acceleration in terms of calculation but with a crucial difference: acceleration increases the velocity of an object, while deceleration decreases it. In the train's case, after running at a constant speed for a period, it needs to slow down to stop at the next station.
To find out how long it takes to stop (time of deceleration), we can use the equation \( t = \frac{v - u}{a} \), considering that final velocity \( v \) will be zero when the train stops, initial velocity \( u \) is the velocity at the end of the constant speed phase, and \( a \) is the deceleration rate. Once we have the time, we use the distance formula \( s = ut + \frac{1}{2}at^2 \) to determine the distance covered during deceleration. This insight is critical for safety in real-world situations such as vehicular traffic, where the ability to slow down efficiently can be lifesaving.

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Most popular questions from this chapter

An astronaut has left the International Space Station to test a new space scooter. Her partner measures the following velocity changes, each taking place in a \(10 \mathrm{~s}\) interval. What are the magnitude, the algebraic sign, and the direction of the average acceleration in each interval? Assume that the positive direction is to the right. (a) At the beginning of the interval, the astronaut is moving toward the right along the \(x\) -axis at \(15.0 \mathrm{~m} / \mathrm{s}\), and at the end of the interval she is moving toward the right at \(5.0 \mathrm{~m} / \mathrm{s}\). (b) At the beginning she is moving toward the left at \(5.0 \mathrm{~m} / \mathrm{s},\) and at the end she is moving toward the left at \(15.0 \mathrm{~m} / \mathrm{s}\). (c) At the beginning she is moving toward the right at \(15.0 \mathrm{~m} / \mathrm{s}\), and at the end she is moving toward the left at \(15.0 \mathrm{~m} / \mathrm{s}\).

A lunar lander is making its descent to Moon Base I (Fig. E2.40). The lander descends slowly under the retro-thrust of its descent engine. The engine is cut off when the lander is \(5.0 \mathrm{~m}\) above the surface and has a downward speed of \(0.8 \mathrm{~m} / \mathrm{s}\). With the engine off, the lander is in free fall. What is the speed of the lander just before it touches the surface? The acceleration due to gravity on the moon is \(1.6 \mathrm{~m} / \mathrm{s}^{2}\).

A gazelle is running in a straight line (the \(x\) -axis). The graph in at a rate of \(1.60 \mathrm{~m} / \mathrm{s}^{2}\) for \(14.0 \mathrm{~s}\). It runs at constant speed for \(70.0 \mathrm{~s}\) and slows down at a rate of \(3.50 \mathrm{~m} / \mathrm{s}^{2}\) until it stops at the next station. Find the total distance covered.

A car is stopped at a traffic light. It then travels along a straight road such that its distance from the light is given by \(x(t)=b t^{2}-c t^{3},\) where \(b=2.40 \mathrm{~m} / \mathrm{s}^{2}\) and \(c=0.120 \mathrm{~m} / \mathrm{s}^{3}\). (a) Calculate the average velocity of the car for the time interval \(t=0\) to \(t=10.0 \mathrm{~s}\). (b) Calculate the instantaneous velocity of the car at \(t=0, t=5.0 \mathrm{~s},\) and \(t=10.0 \mathrm{~s} .\) (c) How long after starting from rest is the car again at rest?

An object's velocity is measured to be \(v_{x}(t)=\alpha-\beta t^{2}\), where \(\alpha=4.00 \mathrm{~m} / \mathrm{s}\) and \(\beta=2.00 \mathrm{~m} / \mathrm{s}^{3} .\) At \(t=0\) the object is at \(x=0 .\) (a) Calculate the object's position and acceleration as functions of time. (b) What is the object's maximum positive displacement from the origin?

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