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A rock is suspended by a light string. When the rock is in air, the tension in the string is 39.2 \(\mathrm{N}\) . When the rock is totally immersed in water, the tension is 28.4 \(\mathrm{N}\) . When the rock is totally immersed in an unknown liquid, the tension is 18.6 \(\mathrm{N}\) . What is the density of the unknown liquid?

Short Answer

Expert verified
The density of the unknown liquid is approximately 1900 kg/m^3.

Step by step solution

01

Calculate the Weight of the Rock

The weight of the rock when it's in air can be directly determined from the tension in the string. Since this tension is the only force supporting the rock against gravity, it equals the weight of the rock. Thus, the weight of the rock is 39.2 N.
02

Calculate the Buoyant Force in Water

The buoyant force is the difference between the tension in the air and the tension in water. When immersed in water, the tension is 28.4 N. Therefore, the buoyant force is calculated as:\[\text{Buoyant Force in Water} = 39.2 \text{ N} - 28.4 \text{ N} = 10.8 \text{ N}\]
03

Calculate the Volume of the Rock

The buoyant force in water is equal to the weight of the water displaced by the rock, which can be calculated using the formula:\[B = \rho_{water} \cdot V_{rock} \cdot g\]Given that \(B = 10.8\,\text{N}\), \(\rho_{water} = 1000\,\text{kg/m}^3\), and \(g = 9.8\,\text{m/s}^2\), solve for \(V_{rock}\):\[V_{rock} = \frac{B}{\rho_{water} \cdot g} = \frac{10.8}{1000 \times 9.8} \approx 0.001102\,\text{m}^3\]
04

Calculate the Buoyant Force in the Unknown Liquid

The buoyant force when the rock is immersed in the unknown liquid is the difference between the tension in the air and the tension in the unknown liquid:\[\text{Buoyant Force in Unknown Liquid} = 39.2 \text{ N} - 18.6 \text{ N} = 20.6 \text{ N}\]
05

Calculate the Density of the Unknown Liquid

By using the buoyant force formula again, we solve for the density of the unknown liquid (\(\rho_{liquid}\)):\[B = \rho_{liquid} \cdot V_{rock} \cdot g\]\[20.6 = \rho_{liquid} \cdot 0.001102 \cdot 9.8\]\[\rho_{liquid} = \frac{20.6}{0.001102 \times 9.8} \approx 1900\,\text{kg/m}^3 \]

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Key Concepts

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

Buoyant Force
In our everyday experiences, objects appear lighter when submerged in water. This phenomenon is due to the buoyant force. The buoyant force is an upward force exerted by a fluid that opposes the weight of an object immersed in it. According to Archimedes' principle, the magnitude of this force is equal to the weight of the fluid displaced by the object.
To calculate the buoyant force, use:
  • Measure the initial tension in air (e.g., 39.2 N in our example)
  • Measure the tension when the object is submerged (e.g., 18.6 N in an unknown liquid)
The buoyant force is found by subtracting the submerged tension from the air tension. This tells us how much of the object's weight is supported by the fluid. In applied scenarios such as our textbook exercise, determining this force helps us find other properties like density.
Density Calculation
Density calculation is a crucial process in physics as it helps understand how substances interact. Density, denoted as \( \rho \), is the mass contained in a unit volume of a substance and is typically expressed in kilograms per cubic meter (\(\text{kg/m}^3\)). It tells us how compact a substance is. To calculate the density of a fluid based on buoyant force:
  • Determine the buoyant force experienced by the immersed object.
  • Use the volume of the displaced fluid, which is equivalent to the volume of the object itself.
In the given problem, determine the unknown liquid's density using the equation \( B = \rho_{\text{liquid}} \times V_{\text{rock}} \times g \). By knowing the buoyant force and volume obtained from earlier calculations, solve for \( \rho_{\text{liquid}} \). This aids in understanding the substance's interaction or applicability, such as whether it will support certain objects.
Tension in String
Tension in a string is the pulling force transmitted axially by means of a string. This concept plays a vital role in understanding the dynamics of forces acting on suspended objects. When an object is hanging in air without immersion, the only acting force besides gravity is the tension in the string. When submerged, the buoyant force also plays a role, thereby reducing the effective tension in the string. To find the actual weight of the object, look at the tension measurement when it is suspended in air. Then, as the object gets immersed in different fluids, this tension decreases due to the buoyant force. When examining our exercise, note the significant decrease from 39.2 N to 18.6 N in unknown liquid. This change allows us to calculate the buoyant force and, accordingly, the density of the liquid. Thus, understanding tension not only helps in keeping objects stabilized but also in deriving the forces and properties associated with the environment the object is in.

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Most popular questions from this chapter

The densities of air, helium, and hydrogen (at \(p=1.0\) atm and \(T=20^{\circ} \mathrm{C} )\) are \(1.20 \mathrm{kg} / \mathrm{m}^{3}, 0.166 \mathrm{kg} / \mathrm{m}^{3},\) and 0.0899 \(\mathrm{kg} / \mathrm{m}^{3}\) , respectively. (a) What is the volume in cubic meters displaced by a hydrogen-filled airship that has a total "Iift" of 120 \(\mathrm{kN}\) ? (The "lift" is the amount by which the buoyant force exceeds the weight of the gas that fills the airship. \((b)\) What would be the "lift" if helium were used instead of hydrogen? In view of your answer, why is helium used in modern airships like advertising blimps?

Black Smokers. Black smokers are hot volcanic vents that emit smoke deep in the ocean floor. Many of them teem with exotic creatures, and some biologists think that life on earth may have begun around such vents. The vents range in depth from about 1500 \(\mathrm{m}\) to 3200 \(\mathrm{m}\) below the surface. What is the gauge pressure at a \(3200-\mathrm{m}\) deep vent, assuming the density of water does not vary? Express your answer in pascals and atmospheres.

A golf course sprinkler system discharges water from a horizontal pipe at the rate of 7200 \(\mathrm{cm}^{3} / \mathrm{s}\) . At one point in the pipe, where the radius is 4.00 \(\mathrm{cm}\) , the water's absolute pressure is \(2.40 \times 10^{5} \mathrm{Pa}\) . At a second point in the pipe, the water passes through a constriction where the radius is \(2.00 \mathrm{cm} .\) What is the water's absolute pressure as it flows through this constriction?

SHM of a Floating Object. An object with height \(h\) , mass \(M,\) and a uniform cross-sectional area \(A\) floats upright in a liquid with density \(\rho\) . (a) Calculate the vertical distance from the surface of the liquid to the bottom of the floating object at equilibrium. (b) A downward force with magnitude \(F\) is applied to the top of the object. At the new equilibrium position, how much farther below the surface of the liquid is the bottom of the object than it was in part (a)? (Assume that some of the object remains above the surface of the liquid.) (c) Your result in part (b) shows that if the force is suddenly removed, the object will oscillate up and down in SHM. Calculate the period of this motion in terms of the density \(\rho\) of the liquid, the mass \(M,\) and cross-sectional area \(A\) of the object. You can ignore the damping due to fluid friction (see Section \(13.7 ) .\)

A liquid flowing from a vertical pipe has a definite shape as it flows from the pipe. To get the equation for this shape, assume that the liquid is in free fall once it leaves the pipe. Just as it leaves the pipe, the liquid has speed \(v_{0}\) and the radius of the stream of liquid is \(r_{0 .}\) (a) Find an equation for the speed of the liquid as a function of the distance \(y\) it has fallen. Combining this with the equation of continuity, find an expression for the radius of the stream as a function of \(y\) . (b) If water flows out of a vertical pipe at a speed of 1.20 \(\mathrm{m} / \mathrm{s}\) , how far below the outlet will the radius be one-half the original radius of the stream?

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