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Stay Dry! You tie a cord to a pail of water and swing the pail in a vertical circle of radius \(0.600 \mathrm{~m}\). What minimum speed must you give the pail at the highest point of the circle to avoid spilling water?

Short Answer

Expert verified
The minimum speed at the highest point of the circle to avoid spilling water is approximately \(2.43 m/s\).

Step by step solution

01

Understand the Forces Involved

In order for the water to remain inside the pail at the top of the circle, the normal force experienced by the water has to be zero. For this to happen, all of the gravitational force has to be used for providing the necessary centripetal force for the circular motion. Hence, we have the following equation: \(F_{gravity} = F_{centripetal}\).
02

Formulate the Equations

We can use the following formulas in our calculation: \(F_{gravity} = m \cdot g\), where m is the mass of water and g is the acceleration due to gravity. Next, \(F_{centripetal} = m \cdot v^{2} / r\). Set them equal to each other, we get \(m \cdot g = m \cdot v^{2} / r\).
03

Solve for the Speed

From the formula, it's clear that the mass \(m\) isn't necessary to figure out our answer, so whether the pail is full of water or just a single drop, the minimum speed needed wouldn't change. By simplifying the equation we get \(v = \sqrt{g \cdot r}\). Plug the given values into the equation. \(v = \sqrt{(9.8 m/s^2) * (0.600 m)}\).
04

Compute the Result

Calculate the above expression to get the value of minimum speed. The final answer comes out to be approximately \(v = 2.43 m/s\). Thus, this is the minimum speed the pail must have at the top to ensure the water does not spill.

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Key Concepts

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

Centripetal Force
Centripetal force is the pivotal concept to understanding why objects move in a circular path instead of continuing in a straight line. Imagine you're swinging a stone tied to a string; the string pulls the stone towards the center of the circular path, which requires a force directed towards that center. That's centripetal force in action.

Mathematically, centripetal force (\( F_{centripetal} \)) is defined as the force that keeps an object moving in a circular path. It is directed towards the center of the circle and is calculated by the equation \( F_{centripetal} = m \cdot v^2 / r \) where \( m \) is the mass of the object, \( v \) is the object's velocity, and \( r \) is the radius of the circle.

In the example of the swinging pail, the pail must maintain a certain minimum speed at the highest point to ensure that the centripetal force is supplied entirely by the gravitational force; otherwise, the water would spill. This is a practical demonstration of how centripetal force is essential for any object traveling in uniform circular motion; without it, the object would simply fly off along a tangential line.
Gravitational Force
Gravitational force is a natural phenomenon by which all things with mass or energy are drawn toward one another. On our planet, this force pulls objects toward the center of the Earth, and it is the reason why we stay grounded.

For any object at the Earth's surface, the gravitational force (\( F_{gravity} \) or weight) is calculated by the product of its mass (\( m \) and the acceleration due to gravity (\( g \) which is approximately \( 9.8 m/s^2 \) near the Earth's surface. This force is what provides the necessary centripetal force for an object in circular motion when acting alone, like the water in the pail at the highest point of its path.

The insight that gravitational force can serve as centripetal force is fundamental; it shows how two seemingly unrelated forces - one pulling an object towards the center of the Earth and another keeping it in a circular motion - are interconnected. If you neglect gravity, even for a moment, in scenarios like astronauts in space, where it is significantly weaker, objects would not behave the same way they do on Earth.
Uniform Circular Motion
Uniform circular motion describes the motion of an object traveling at a constant speed along a circular path. The word 'uniform' refers to the consistent speed - note, however, that it's the speed that's uniform, not the velocity, because velocity is a vector and includes direction.

Since the direction changes continuously in circular motion, the velocity changes too, even if the speed (the magnitude part of the velocity) remains consistent. This change in velocity results in an acceleration, and by Newton's second law of motion (\( F=ma \) a force must be causing this acceleration. That force, as we’ve discussed, is the centripetal force.

An object in uniform circular motion, like our pail of water, is continually accelerating towards the center of the circle, even though its speed is constant. This continuous change of direction is due to the constant inward force - if this force stopped, the object would continue in a straight line due to inertia, as per Newton's first law. Remember, circular motion is all about the balance of forces and requires a perfect centripetal force to maintain the motion without changes in speed.

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Most popular questions from this chapter

Rotating Space Stations. One problem for humans living in outer space is that they are apparently weightless. One way around this problem is to design a space station that spins about its center at a constant rate. This creates "artificial gravity" at the outside rim of the station. (a) If the diameter of the space station is \(800 \mathrm{~m}\), how many revolutions per minute are needed for the "artificial gravity" acceleration to be \(9.80 \mathrm{~m} / \mathrm{s}^{2} ?\) (b) If the space station is a waiting area for travelers going to Mars, it might be desirable to simulate the acceleration due to gravity on the Martian surface \(\left(3.70 \mathrm{~m} / \mathrm{s}^{2}\right) .\) How many revolutions per minute are needed in this case?

A horizontal wire holds a solid uniform ball of mass \(m\) in place on a tilted ramp that rises \(35.0^{\circ}\) above the horizontal. The surface of this ramp is perfectly smooth, and the wire is directed away from the center of the ball (Fig. P5.64). (a) Draw a free-body diagram of the ball. (b) How hard does the surface of the ramp push on the ball? (c) What is the tension in the wire?

A stone with mass \(0.80 \mathrm{~kg}\) is attached to one end of a string \(0.90 \mathrm{~m}\) long. The string will break if its tension exceeds \(60.0 \mathrm{~N}\). The stone is whirled in a horizontal circle on a frictionless tabletop; the other end of the string remains fixed. (a) Draw a free-body diagram of the stone. (b) Find the maximum speed the stone can attain without the string breaking.

An \(8.00 \mathrm{~kg}\) box sits on a ramp that is inclined at \(33.0^{\circ}\) above the horizontal. The coefficient of kinetic friction between the box and the surface of the ramp is \(\mu_{\mathrm{k}}=0.300 .\) A constant horizontal force \(F=26.0 \mathrm{~N}\) is applied to the box (Fig. \(\mathbf{P} 5.73),\) and the box moves down the ramp. If the box is initially at rest, what is its speed \(2.00 \mathrm{~s}\) after the force is applied?

A block with mass \(m_{1}\) is placed on an inclined plane with slope angle \(\alpha\) and is connected to a hanging block with mass \(m_{2}\) by a cord passing over a small, friction less pulley (Fig. P5.74). The coefficient of static friction is \(\mu_{\mathrm{s}}\), and the coefficient of kinetic friction is \(\mu_{\mathrm{k}}\). (a) Find the value of \(m_{2}\) for which the block of mass \(m_{1}\) moves up the plane at constant speed once it is set in motion. (b) Find the value of \(m_{2}\) for which the block of mass \(m_{1}\) moves down the plane at constant speed once it is set in motion. (c) For what range of values of \(m_{2}\) will the blocks remain at rest if they are released from rest?

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