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(a) The mass and the radius of the sun are, respectively, \(1.99 \times 10^{30} \mathrm{kg}\) and \(6.96 \times 10^{8} \mathrm{m}\) . What is its density? (b) If a solid object is made from a material that has the same density as the sun, would it sink or float in water? Why? (c) Would a solid object sink or float in water if were made from a material whose density was the same as that of the planet Saturn (mass \(=5.7 \times 10^{26} \mathrm{kg},\) radius \(=6.0 \times 10^{7} \mathrm{m} ) ?\) Provide a reason for your answer.

Short Answer

Expert verified
(a) Sun's density: 1410 kg/m³. (b) It would sink, it's denser than water. (c) It would float, Saturn's density is less than water.

Step by step solution

01

Calculate the Volume of the Sun

The volume of a sphere is given by the formula \( V = \frac{4}{3} \pi r^3 \), where \( r \) is the radius. Here, the radius \( r = 6.96 \times 10^8 \) m. Thus, the volume of the Sun is \( V = \frac{4}{3} \pi (6.96 \times 10^8)^3 \approx 1.41 \times 10^{27} \) m³.
02

Determine the Density of the Sun

Density is calculated using the formula \( \text{Density} = \frac{\text{Mass}}{\text{Volume}} \). For the Sun, with mass \(1.99 \times 10^{30} \) kg and volume \(1.41 \times 10^{27} \) m³, the density is \( \frac{1.99 \times 10^{30}}{1.41 \times 10^{27}} \approx 1410 \) kg/m³.
03

Compare Sun's Density with Water

The density of water is \(1000\) kg/m³. Since the Sun's density (1410 kg/m³) is greater than water, a solid object with the Sun's density would sink in water.
04

Calculate the Volume of Saturn

Using the same formula for the volume of a sphere, with Saturn's radius \( r = 6.0 \times 10^7 \) m, the volume is \( V = \frac{4}{3} \pi (6.0 \times 10^7)^3 \approx 9.04 \times 10^{24} \) m³.
05

Determine the Density of Saturn

The density of Saturn is calculated by \( \text{Density} = \frac{\text{Mass}}{\text{Volume}} \). With mass \(5.7 \times 10^{26} \) kg and volume \(9.04 \times 10^{24} \) m³, the density is \( \frac{5.7 \times 10^{26}}{9.04 \times 10^{24}} \approx 630 \) kg/m³.
06

Compare Saturn's Density with Water

Since Saturn's density (630 kg/m³) is less than that of water (1000 kg/m³), a solid object with Saturn's density would float in water.

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Key Concepts

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

Volume of a Sphere
In order to find the density of celestial bodies like the Sun or Saturn, calculating the volume is crucial. For spherical objects, the volume can be found using the formula \( V = \frac{4}{3} \pi r^3 \), where \( r \) is the radius of the sphere.
  • The radius is simply half the diameter of the sphere, which is often provided in problems like these.
  • Don't forget that the radius needs to be in meters for standard measurements.
For example, if you take the radius of the Sun, \( r = 6.96 \times 10^8 \) meters, you plug it into the formula:
\[ V = \frac{4}{3} \pi (6.96 \times 10^8)^3 \approx 1.41 \times 10^{27} \text{ m}^3 \].
This gives you a glimpse of the Sun's vast size compared to Earth. Remember, calculating the volume is the first step in determining density!
Density Comparison
Once you have the volume, you can move on to calculating density. Density gives insight into the compactness of a body, calculated as \( \text{Density} = \frac{\text{Mass}}{\text{Volume}} \).
  • The mass should be in kilograms and the volume in cubic meters for consistency.
For instance, the density of the Sun is determined using its mass \((1.99 \times 10^{30} \text{ kg})\) and its calculated volume \((1.41 \times 10^{27} \text{ m}^3)\):
\[ \text{Density} = \frac{1.99 \times 10^{30}}{1.41 \times 10^{27}} \approx 1410 \text{ kg/m}^3 \].
When comparing this to water's density, which is \(1000\) \(\text{kg/m}^3\), any object with the Sun's density would sink because it is denser than water. Conversely, for Saturn, with calculated density \(630 \text{ kg/m}^3\), it is less dense compared to water, meaning it would float if it were submerged.
Mass and Radius Calculations
Understanding the relationship between mass and radius provides insights into a celestial body's density. By knowing these, you can derive the density, which tells you about the object’s overall composition.
  • The mass involves all the particles that make up the celestial body, and knowing this helps determine how gravity might act.
  • Radius gives an indication of size and helps when comparing the object's size to other celestial bodies.
Let's look at Saturn: the mass is \(5.7 \times 10^{26} \text{ kg}\) and the radius is \(6.0 \times 10^7 \text{ m}\). Its volume is calculated as:
\[ V = \frac{4}{3} \pi (6.0 \times 10^7)^3 \approx 9.04 \times 10^{24} \text{ m}^3 \].
Then its density is:
\[ \text{Density} = \frac{5.7 \times 10^{26}}{9.04 \times 10^{24}} \approx 630 \text{ kg/m}^3 \].
This simplification process allows us to predict behavior, such as whether it will float or sink in a given medium, such as water.

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Most popular questions from this chapter

Two hoses are connected to the same outlet using a Y-connector, as the drawing shows. The hoses A and B have the same length, but hose B has the larger radius. Each is open to the atmosphere at the end where the water exits. Water flows through both hoses as a viscous fluid, and Poiseuille’s law \(\left[Q=\pi R^{4}\left(P_{2}-P_{1}\right) /(8 \eta L)\right]\) applies to each. In this law, \(P_{2}\) is the pressure upstream, \(P_{1}\) is the pressure down- stream, and \(Q\) is the volume flow rate. The ratio of the radius of hose \(B\) to the radius of hose A is \(R_{B} / R_{A}=1.50 .\) Find the ratio of the speed of the water in hose \(\mathrm{B}\) to the speed in hose A.

A pressure difference of \(1.8 \times 10^{3}\) Pa is needed to drive water \(\left(\eta=1.0 \times 10^{-3} \mathrm{Pa} \cdot \mathrm{s}\right)\) through a pipe whose radius is \(5.1 \times 10^{-3} \mathrm{m} .\) The volume flow rate of the water is \(2.8 \times 10^{-4} \mathrm{m}^{3} / \mathrm{s} .\) What is the length of the pipe?

Poiseuille’s law remains valid as long as the fluid flow is laminar. For sufficiently high speed, however, the flow becomes turbulent, even if the fluid is moving through a smooth pipe with no restrictions. It is found experimentally that the flow is laminar as long as the Reynolds number Re is less than about \(2000 : \mathrm{Re}=2 \overline{v} \rho R / \eta .\) Here \(\overline{v},\) \(\rho,\) and \(\eta\) are, respectively, the average speed, density, and viscosity of the fluid, and \(R\) is the radius of the pipe. Calculate the highest average speed that blood \(\left(\rho=1060 \mathrm{kg} / \mathrm{m}^{3}, \eta=4.0 \times 10^{-3} \mathrm{Pa} \cdot \mathrm{s}\right)\) could have and still remain in laminar flow when it flows through the aorta \(\left(R=8.0 \times 10^{-3} \mathrm{m}\right)\)

A ship is floating on a lake. Its hold is the interior space beneath its deck; the hold is empty and is open to the atmosphere. The hull has a hole in it, which is below the water line, so water leaks into the hold. The effective area of the hole is \(8.0 \times 10^{-3} \mathrm{m}^{2}\) and is located 2.0 \(\mathrm{m}\) beneath the surface of the lake. What volume of water per second leaks into the ship?

A fountain sends a stream of water straight up into the air to a maximum height of 5.00 \(\mathrm{m}\) . The effective cross-sectional area of the pipe feeding the fountain is \(5.00 \times 10^{-4} \mathrm{m}^{2}\) . Neglecting air resistance and any viscous effects, determine how many gallons per minute are being used by the fountain. (Note: 1 gal \(=3.79 \times 10^{-3} \mathrm{m}^{3} . )\)

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