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During an Olympic bobsled run, a European team takes a turn of radius \(25 \mathrm{ft}\) at a speed of \(60 \mathrm{mi} / \mathrm{h}\). What acceleration do the riders experience \((a)\) in \(\mathrm{ft} / \mathrm{s}^{2}\) and \((b)\) in units of \(g\) ?

Short Answer

Expert verified
The riders experience an acceleration of \(a = 309.76 ft/s^2\) or equivalently \(9.62 g\).

Step by step solution

01

Convert speed from miles/hour to feet/second

First, convert the speed from miles per hour to feet per second. There are 5280 feet in one mile and 3600 seconds in one hour. So, \(v = 60 mi/hr * (5280 ft / 1 mi) * (1 hr / 3600 s) = 88 ft/s\).
02

Substitute values into the acceleration formula

Next, use the equation \(a = v^2/r\) to find the acceleration. Substitute \(v = 88 ft/s\) and \(r = 25 ft\) into the equation to get \(a = (88 ft/s)^2 / 25 ft = 309.76 ft/s^2\) .
03

Convert acceleration from \(ft/s^2\) to \(g\)

Finally, convert the acceleration from \(ft/s^2\) to \(g\). Since \(1 g = 32.2 ft/s^2\), divide 309.76 by 32.2 to get the acceleration in terms of \(g\). So, \(a_g = 309.76 ft/s^2 / 32.2 ft/s^2/g = 9.62 g\).

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Key Concepts

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

Centripetal Acceleration
When an object moves in a circular path, it experiences an acceleration towards the center of the circle. This is called *centripetal acceleration* and is essential for maintaining circular motion. Centripetal acceleration is calculated using the formula \( a = \frac{v^2}{r} \), where \( v \) is the velocity of the object and \( r \) is the radius of the circular path.

In the context of the bobsled problem, this acceleration ensures that the bobsled stays on its curved path as it goes around the turn. The formula tells us that the faster the bobsled goes or the sharper the turn (smaller radius), the greater this centripetal acceleration will be. This acceleration pulls the riders towards the inside of the turn, creating the sensation of being pushed against the outer wall of the bobsled.

Understanding centripetal acceleration is key to interpreting scenarios involving circular motion, such as the motions of vehicles on curved tracks or satellites orbiting planets.
Unit Conversion
Unit conversion is a critical skill in physics, enabling us to express measurements in different units without altering the underlying value. In the bobsled problem, we begin by converting the speed from miles per hour to feet per second. Understanding how to convert units is essential, as it ensures all expressions are consistent and compatible for calculations.

Here's a quick breakdown of the steps for converting miles per hour to feet per second:
  • Recognize that 1 mile equals 5280 feet.
  • Understand there are 3600 seconds in an hour.
  • Use this information to convert 60 miles per hour to feet per second: \( 60 \text{ mi/hr} = 60 \times \frac{5280 \text{ ft}}{1 \text{ mi}} \times \frac{1 \text{ hr}}{3600 \text{ s}} = 88 \text{ ft/s} \).
Unit conversions like these are invaluable tools in physics, providing a foundation for working through problems accurately without being tripped up by mismatched units.
Radius of Curvature
The radius of curvature is a measure that describes how sharply a curve is turning. In the context of circular motion, it defines the radius of the circular path. This concept is crucial because it directly affects the centripetal acceleration an object experiences.

In the bobsled problem, the turn the bobsled takes has a radius of 25 feet. This radius of curvature implies how tightly the turn is. A smaller radius would mean a sharper turn, requiring a greater centripetal acceleration to keep the bobsled on its path. Conversely, a larger radius would mean a gentler curve with a reduced need for acceleration.
  • Radius is directly inversely proportional to centripetal acceleration when speed is constant.
  • In practical scenarios, managing the radius of curvature is important for safety and comfort.
Understanding radius of curvature helps in planning paths for racing tracks, roadways, and in designing fairground rides, ensuring both excitement and safety.

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Most popular questions from this chapter

A lamp hangs vertically from a cord in a descending elevator. The elevator has a deceleration of \(2.4 \mathrm{~m} / \mathrm{s}^{2}\) before coming to a stop. ( \(a\) ) If the tension in the cord is \(89 \mathrm{~N}\), what is the mass of the lamp? (b) What is the tension in the cord when the elevator ascends with an upward acceleration of \(2.4 \mathrm{~m} / \mathrm{s}^{2}\) ?

A 42 -kg slab rests on a frictionless floor. A \(9.7-\mathrm{kg}\) block rests on top of the slab, as in Fig. 5-40. The coefficient of static friction between the block and the slab is \(0.53\), while the coefficient of kinetic friction is \(0.38\). The \(9.7-\mathrm{kg}\) block is acted on by a horizontal force of \(110 \mathrm{~N}\). What are the resulting accelerations of \((a)\) the block and \((b)\) the slab?

A \(2400-\mathrm{lb}(=10.7-\mathrm{kN})\) car traveling at \(30 \mathrm{mi} / \mathrm{h}(=13.4 \mathrm{~m} / \mathrm{s})\) attempts to round an unbanked curve with a radius of \(200 \mathrm{ft}\) \((=61.0 \mathrm{~m}) .(a)\) What force of friction is required to keep the car on its circular path? ( \(b\) ) What minimum coefficient of static friction between the tires and road is required?

In Fig. 5-38, object \(B\) weighs \(94.0 \mathrm{lb}\) and object \(A\) weighs \(29.0 \mathrm{lb} .\) Between object \(B\) and the plane the coefficient of static friction is \(0.56\) and the coefficient of kinetic friction is 0.25. (a) Find the acceleration of the system if \(B\) is initially at rest. (b) Find the acceleration if \(B\) is moving up the plane. ( \(c\) ) What is the acceleration if \(B\) is moving down the plane? The plane is inclined by \(42.0^{\circ}\).

An elevator and its load have a combined mass of \(1600 \mathrm{~kg}\). Find the tension in the supporting cable when the elevator, originally moving downward at \(12.0 \mathrm{~m} / \mathrm{s}\), is brought to rest with constant acceleration in a distance of \(42.0 \mathrm{~m}\).

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