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A car is traveling at a constant speed of \(33 \mathrm{m} / \mathrm{s}\) on a highway. At the instant this car passes an entrance ramp, a second car enters the highway from the ramp. The second car starts from rest and has a constant acceleration. What acceleration must it maintain, so that the two cars meet for the first time at the next exit, which is \(2.5 \mathrm{km}\) away?

Short Answer

Expert verified
The second car's acceleration must be approximately \(0.872 \mathrm{m/s^2}\).

Step by step solution

01

Identify Given Values

First, let's list the given values from the problem. The speed of the first car is \(33 \mathrm{m/s}\). The distance to the next exit is \(2.5 \mathrm{km}\), which we convert to meters, obtaining \(2500 \mathrm{m}\). The second car starts from rest, meaning its initial velocity \(u_2 = 0\). We are looking for the acceleration \(a\) of the second car.
02

Determine Time for First Car

Since the first car is traveling at a constant speed, the time it takes to reach the exit can be calculated with the formula: \( t = \frac{d}{v} = \frac{2500 \mathrm{m}}{33 \mathrm{m/s}} \approx 75.76 \mathrm{s}\).
03

Express Second Car's Travel Equation

The second car starts from rest and follows the kinematic equation: \(s = u_2 t + \frac{1}{2} a t^2\). Here, \(s = 2500 \mathrm{m}\) is the distance, \(u_2 = 0\), so we have \(2500 = \frac{1}{2} a t^2\).
04

Relate Both Cars' Timing

Both cars must meet at the same exit point in the same amount of time, which we found is \(75.76 \mathrm{s}\) for the first car. Therefore, substitute \(t = 75.76\) into the equation from Step 3: \(2500 = \frac{1}{2} a (75.76)^2\).
05

Solve for the Acceleration

Rearrange the equation to solve for \(a\): \( a = \frac{2 \times 2500}{75.76^2} \approx 0.872 \mathrm{m/s^2}\).

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Key Concepts

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

Kinematic Equations
Kinematic equations are fundamental to understanding motion in physics, especially in scenarios involving constant acceleration. These equations allow us to predict and calculate various aspects of a moving object, including its position, velocity, and acceleration at any given time. For a car accelerating from rest, the most relevant kinematic equation is:
  • \[ s = u t + \frac{1}{2} a t^2 \]
where \(s\) represents the distance traveled, \(u\) is the initial velocity, \(a\) is the acceleration, and \(t\) is the time. In this exercise, the second car uses this equation to determine how far it travels over a specific time period. Because it starts from rest, the initial velocity \(u = 0\) eliminates the \(u t\) term, simplifying the equation to \[ s = \frac{1}{2} a t^2 \]. By rearranging this equation, we can find the required acceleration to meet another moving car at a specific point.
Relative Motion
Relative motion describes the movement of two or more objects in relation to each other. In this exercise, two cars are moving on the highway with one trying to catch up with the other. The first car maintains a constant speed of \(33 \mathrm{m/s}\), while the second car accelerates to meet it at the next exit. The key to solving such problems is understanding that both cars must travel the same distance in the same amount of time to meet at the specified location. This involves comparing their movements using kinematic equations to ensure their paths cross under the given conditions. Relative motion becomes especially important when coordinating the dynamics of different moving objects, like when the second car accelerates to coincide with the steady speed of the first car.
Time and Distance Calculation
Calculating time and distance accurately is crucial in physics problems involving motion, such as the scenario with the two cars. The first step is often to convert all units to a consistent system, such as converting 2.5 km to 2500 meters. For constant speed, the time \(t\) to travel a known distance \(d\) can be determined using the formula:
  • \[ t = \frac{d}{v} \]
where \(v\) is the velocity. In our case, the first car's time to the exit is calculated to show how long both vehicles have to meet at the exit. With this time, we then apply it to the kinematic equation of the second car to solve for the acceleration. This highlights the interconnectedness of time and distance in determining motion parameters, ensuring both cars meet at the exit simultaneously. The calculations take advantage of constant velocity for the first car and constant acceleration for the second, incorporating both aspects of time and distance effectively.

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Most popular questions from this chapter

A race driver has made a pit stop to refuel. After refueling, he starts from rest and leaves the pit area with an acceleration whose magnitude is \(6.0 \mathrm{m} / \mathrm{s}^{2}\); after \(4.0 \mathrm{s}\) he cnters the main specdway. At the same instant, another car on the speedway and traveling at a constant velocity of \(70.0 \mathrm{m} / \mathrm{s}\) overtakes and passes the entering car. The cntering car maintains its acceleration. How much time is required for the entering car to catch the other car?

The three-toed sloth is the slowest-moving land mammal. On the ground, the sloth moves at an average speed of \(0.037 \mathrm{m} / \mathrm{s}\), considerably slower than the giant tortoise, which walks at \(0.076 \mathrm{m} / \mathrm{s}\). After 12 minutes of walking, how much further would the tortoise have gone relative to the sloth?

A ball is thrown straight upward and rises to a maximum height of \(16 \mathrm{m}\) above its launch point. At what height above its launch point has the speed of the ball decreased to one-half of its initial value?

A jet is taking off from the deck of an aircraft carrier, as shown in the image. Starting from rest, the jet is catapulted with a constant acceleration of \(+31 \mathrm{m} / \mathrm{s}^{2}\) along a straight line and reaches a velocity of \(+62 \mathrm{m} / \mathrm{s} .\) Find the displacement of the jet.

In a historical movie, two knights on horseback start from rest \(88.0 \mathrm{m}\) apart and ride directly toward each other to do battle. Sir George's acceleration has a magnitude of \(0.300 \mathrm{m} / \mathrm{s}^{2},\) while Sir Alfred's has a magnitude of \(0.200 \mathrm{m} / \mathrm{s}^{2} .\) Relative to Sir George's starting point, where do the knights collide?

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