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The weight of a king's solid crown is w. When the crown is suspended by a light rope and completely immersed in water, the tension in the rope (the crown's apparent weight) is \(f w .\) (a) Prove that the crown's relative density (specific gravity) is \(1 /(1-f) .\) Discuss the meaning of the limits as \(f\) approaches 0 and \(1 .\) (b) If the crown is solid gold and weighs 129 \(\mathrm{N}\) in air, what is its apparent weight when completely immersed in water? (c) Repeat part (b) if the crown is solid lead with a very thin gold plating, but still has a weight in air of 12.9 \(\mathrm{N}\) .

Short Answer

Expert verified
(a) Relative density = \(1/(1-f)\). (b) 122.3 N. (c) 11.8 N.

Step by step solution

01

Understand Buoyancy and Tension

When an object is immersed in a fluid, it experiences a buoyant force equal to the weight of the fluid displaced by the object (Archimedes' Principle). If the crown weighs \(w\) and its tension in water is \(fw\), then the buoyant force \(B\) is given by \(B = w - fw\).
02

Calculate Buoyant Force in Terms of Density

Let \(\rho\) be the density of the crown and \(\rho_w\) be the density of water. The buoyant force can also be expressed as \(B = V \rho_w g\), where \(V\) is the volume of the crown. Since \(B = w - fw\), combining these gives \(V \rho_w g = w - fw\). Simultaneously, we know that \(w = V \rho g\).
03

Solve for Relative Density

Divide \(w - fw = V \rho_w g\) by \(w = V \rho g\) to get relative density: \(\frac{\rho}{\rho_w} = \frac{w}{w - fw} = \frac{1}{1-f}\). This shows that the crown's relative density (specific gravity) is \(1/(1-f)\). As \(f\to 0\), the density approaches that of the crown's actual material. As \(f\to 1\), the density approaches infinity, meaning the crown becomes near weightless in water (like cork).
04

Calculate Apparent Weight for Gold Crown

For part (b), a solid gold crown has a density of approximately 19,300 kg/m³. With a weight of 129 N in air (\(w = 129\) N), its relative density in water is \(\rho/\rho_w = 19.3\), so \(f = 1 - 1/19.3\). The apparent weight \(f w = (1-1/19.3) \times 129\) N. Calculate \(f \approx 0.948\), giving an apparent weight of \(0.948 \times 129 \approx 122.3\) N.
05

Apparent Weight for Lead Crown

For part (c), a lead crown with a thin gold plating weighs 12.9 N. Lead has a density of around 11,340 kg/m³, so its relative density in water is \(11.34\). Then, \(f = 1 - 1/11.34\). Calculate \(f \approx 0.912\), leading to an apparent weight of \(0.912 \times 12.9 \approx 11.8\) N.

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Key Concepts

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

Relative Density
Relative density, also known as specific gravity, is a measure of the density of a substance compared to the density of a reference substance, typically water. It's a dimensionless quantity that helps in determining whether an object will float or sink in a fluid.

When we talk about the relative density of the king's crown, it involves comparing the crown's density to that of water. The formula derived from the exercise is \(\frac{1}{1-f}\), where \(f\) is the fraction of the crown's weight supported by the fluid or the factor by which its buoyancy affects apparent weight. This formula helps us understand the relationship between the true weight of the crown and its apparent weight when submerged.

As \(f\) approaches 0, it suggests that the crown's relative density is nearly equal to its actual density, meaning it is almost as dense as water itself. On the other hand, as \(f\) approaches 1, the relative density becomes infinitely large, indicating the crown is much denser than the water, akin to it being almost "weightless" or displacing a large amount of water relative to its weight.

This understanding allows us to perceive how different materials compare to water, helping in the identification and characterization of substances based on their buoyancy. It also provides a way to quantify the submerged fraction of a floating object relative to its total volume.
Buoyant Force
The buoyant force is a key concept in understanding how objects behave when submerged in fluids. According to Archimedes' Principle, an object immersed in a fluid experiences an upward force known as buoyancy. This force is equal to the weight of the fluid displaced by the object.

In the case of the king's crown, the buoyant force can be calculated by subtracting the apparent weight of the crown in the fluid (\(fw\)) from its actual weight (\(w\)). Thus, the buoyant force formula becomes \(B = w - fw\). This indicates how much of the crown's weight is countered by the fluid's support.

The buoyancy can also be expressed in terms of volume and density: \(B = V \rho_w g\). By equating this to \(w - fw\), we deduce how much liquid is displaced by the volume of the crown. This displacement not only helps determine the buoyant force but also reveals the extent to which the crown is supported by the water, reducing its apparent heaviness.

Understanding buoyant force is crucial for predicting whether an object will sink or float and is widely used in industries involving fluids, such as naval engineering and fluid dynamics.
Specific Gravity
Specific gravity is another term for relative density and is used to compare the density of a substance to a reference substance, usually water. It gives intuitive insights into whether an object will float in a particular fluid.

In practical terms, specific gravity can be determined by dividing the density of the object by the density of the reference fluid, most often water (density \(\rho_w\)). In this exercise, the specific gravity formula \(\frac{1}{1-f}\) reveals the proportionate relationship between the object's density (crown in this case) and water.

Having specific gravity aids in characterizing materials without the need for weight measurements in new situations. For example, gold has a higher specific gravity than lead, confirming its denser nature as seen in the exercise with a typical density value for gold around 19.3 times that of water. Using specific gravity eases material identification and allows for predictions about an object's buoyancy without immersion.

The concept importantly serves in various applications, such as battery acid testing, urinary analyzers, and more, delivering a quick assessment tool for material and fluid characteristics. By understanding specific gravity, one can gain practical knowledge in material selection and buoyancy effects in various contexts.

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Most popular questions from this chapter

A sealed tank containing seawater to a height of 11.0 \(\mathrm{m}\) also contains air above the water at a gauge pressure of 3.00 atm. Water flows out from the bottom through a small hole. How fast is this water moving?

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