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In 1892 George W. G. Ferris designed a carnival ride in the shape of a large wheel. This Ferris wheel had a diameter of \(76 \mathrm{~m}\) and rotated one revolution every \(20 \mathrm{~min}\). What was the magnitude of the acceleration that riders experienced? SSM

Short Answer

Expert verified
The magnitude of the acceleration that riders experienced on the Ferris wheel is obtained by dividing the square of the speed by the radius of the Ferris wheel.

Step by step solution

01

Conversion of Units

Convert the time of one revolution to seconds as acceleration is usually measured in m/s^2. This can be done by multiplying the given value by the equivalent in seconds: \(20 \ \mathrm{min} = 20 \times 60 = 1200 \ \mathrm{s}\)
02

Calculating the Speed

Compute the speed using the formula \(speed = \frac{distance}{time}\). Here, the distance is the circumference of the Ferris wheel, which is \(diameter \times \pi = 76 \ \mathrm{m} \times \pi\), and the time is the time for one revolution, which we have calculated in the previous step. Thus, \(speed = \frac{76 \ \mathrm{m} \times \pi}{1200} \ \mathrm{s}\)
03

Calculating the Radius

Compute the radius of the Ferris wheel to be used in the acceleration formula. The radius is half the diameter, so in this case, \(radius = \frac{76 \ \mathrm{m}}{2} = 38 \ \mathrm{m}\)
04

Calculating the Acceleration

Compute the acceleration using the equation for acceleration in circular motion: \(acceleration = \frac{speed^2}{radius}\). Substitute the calculated values of speed and radius into that equation to get the desired acceleration.

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Key Concepts

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

Centripetal Acceleration
When objects move in a circle, even at a constant speed, they experience a type of acceleration known as centripetal acceleration. This is because the object's direction is constantly changing, which is a form of acceleration, even if its speed remains constant. In circular motion, the acceleration always points towards the center of the circle, hence the term "centripetal," which means "center-seeking."
The formula for centripetal acceleration is given by:\[ a = \frac{v^2}{r} \]Here, \( a \) is the centripetal acceleration, \( v \) is the linear velocity or speed of the object, and \( r \) is the radius of the circular path.
  • The larger the velocity, the greater the centripetal acceleration.
  • The smaller the radius, the greater the centripetal acceleration for the same speed.
Understanding this concept helps explain why riders on a Ferris wheel feel pushed towards the outer edge as the wheel rotates, even though the motion seems gentle.
Circumference Calculations
Calculating the circumference of a circular object is pivotal in solving problems related to circular motion. The circumference provides the distance an object covers in one full revolution. For a circle, like a Ferris wheel, the circumference is calculated using the formula:\[ C = \pi \cdot d \]Where \( C \) is the circumference and \( d \) is the diameter of the circle. In our Ferris wheel problem, the diameter was given as \(76 \ \mathrm{m}\), so:\[ C = \pi \cdot 76 \ \mathrm{m} \]This calculation provides the total distance traveled around the circle in one full rotation. It's essential for computing the speed of riders, especially since this plays a direct role in determining the centripetal acceleration they experience.
  • Accurate circumference calculations are critical, as any error can propagate through the speed and acceleration calculations.
Unit Conversions
Unit conversions may seem like a small detail but are crucial for solving physics problems correctly. In the context of circular motion, it's often necessary to convert time units to ensure that all components in an equation are compatible. For example, in acceleration calculations, which are expressed in \( \mathrm{m/s}^2 \), time must be in seconds for the units to work out correctly.
In the case of the Ferris wheel:
  • We converted the time for one revolution from minutes to seconds: \( 20 \ \mathrm{min} = 20 \times 60 = 1200 \ \mathrm{s} \).
  • Ensuring units are consistent prevents errors and makes complex equations solvable.
Always remember to double-check unit conversions as errors in this area are often the root cause of incorrect physics calculations. Effective problem-solving in physics depends on meticulous attention to these details.

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Most popular questions from this chapter

\- A washing machine drum \(80.0 \mathrm{~cm}\) in diameter starts from rest and achieves \(1200 \mathrm{rev} / \mathrm{min}\) in \(22 \mathrm{~s}\). Assuming the acceleration of the drum is constant, calculate the net acceleration (magnitude and direction) of a point on the drum after \(1.00 \mathrm{~s}\) has elapsed.

An object undergoing parabolic motion travels \(100 \mathrm{~m}\) in the horizontal direction before returning to its initial height. If the object is thrown initially at a \(30^{\circ}\) angle, determine the \(x\) component and the \(y\) component of the initial velocity. (Neglect any effects due to air resistance.)

Sports In 1998, Jason Elam kicked a record field goal. The football started on the ground \(63.0\) yards from the base of the goal posts and just barely cleared the 10 -ft-high bar. If the initial trajectory of the football was \(40.0^{\circ}\) above the horizontal, (a) what was its initial speed and (b) how long after the ball was struck did it pass through the goal posts? (Neglect any effects due to air resistance.)

\- You toss a ball into the air at initial angle \(40^{\circ}\) from the horizontal. At what point in the ball's trajectory does the ball have the smallest speed? (Neglect any effects due to air resistance.) A. just after it is tossed B. at the highest point in its flight C. just before it hits the ground D. halfway between the ground and the highest point on the rise portion of the trajectory E. halfway between the ground and the highest point on the fall portion of the trajectory

\- An object experiences a constant acceleration of \(2.0 \mathrm{~m} / \mathrm{s}^{2}\) along the \(-x\) axis for \(2.7 \mathrm{~s}\), attaining a velocity of \(16 \mathrm{~m} / \mathrm{s}\) in a direction \(45^{\circ}\) from the \(+x\) axis. Find the initial velocity vector of the object.

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