/*! This file is auto-generated */ .wp-block-button__link{color:#fff;background-color:#32373c;border-radius:9999px;box-shadow:none;text-decoration:none;padding:calc(.667em + 2px) calc(1.333em + 2px);font-size:1.125em}.wp-block-file__button{background:#32373c;color:#fff;text-decoration:none} Problem 52 (a) A 5.0-kg rock at a temperatu... [FREE SOLUTION] | 91Ó°ÊÓ

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(a) A 5.0-kg rock at a temperature of \(20^{\circ} \mathrm{C}\) is dropped into a shallow lake also at \(20^{\circ} \mathrm{C}\) from a height of \(1.0 \times 10^{3} \mathrm{m} .\) What is the resulting change in entropy of the universe? (b) If the temperature of the rock is \(100^{\circ} \mathrm{C}\) when it is dropped, what is the change of entropy of the universe? Assume that air friction is negligible (not a good assumption) and that \(c=860 \mathrm{J} / \mathrm{kg} \cdot \mathrm{K}\) is the specific heat of the rock.

Short Answer

Expert verified
(a) For case (a), the change in entropy of the universe due to the change in potential energy is: ΔS = (5 * 9.81 * 1000) / 293.15 ≈ 166.93 J/K (b) For case (b), the heat exchanged between the rock and the lake is: Q = 5 * 860 * 80 = 344000 J The entropy changes due to the change in potential energy and the heat exchange are: ΔS1 = (5 * 9.81 * 1000) / 293.15 ≈ 166.93 J/K ΔS2 = 344000 / 293.15 ≈ 1173.99 J/K The total change in entropy for case (b) is: ΔS_total = ΔS1 + ΔS2 ≈ 166.93 + 1173.99 ≈ 1340.92 J/K

Step by step solution

01

Identify variables and constants

For both cases, the mass of the rock, m = 5.0 kg, the specific heat of the rock, c = 860 J/kg K, and the height, h = 1000 m. The gravitational acceleration, g = 9.81 m/s². For case (a), the initial temperature of the rock and the lake, Ti = 20°C. For case (b), the initial temperature of the rock, Ti = 100°C, and the initial temperature of the lake, Tl = 20°C.
02

Calculate the potential energy

First, we need to calculate the potential energy of the rock before it is dropped. The potential energy, PE = m * g * h.
03

Calculate the temperature change for case (a)

Since the rock and the lake are at the same initial temperature, there is no temperature difference, and hence the change in thermal energy due to heat exchange between the rock and the lake is zero.
04

Calculate the entropy change for case (a)

For case (a), the change in entropy of the universe comes from the change in potential energy. The change in entropy ΔS is given by: ΔS = m * g * h / T Where T is the temperature in kelvin. Convert Ti to kelvin: T = Ti + 273.15 = 20 + 273.15 = 293.15 K. ΔS = (5 * 9.81 * 1000) / 293.15 Calculate the change in entropy.
05

Calculate the temperature change for case (b)

For case (b), the temperature difference between the rock and the lake is 100°C - 20°C = 80°C. As the rock's temperature is higher than the lake's, the rock will lose heat, and the lake will gain heat. The heat exchanged, Q, can be found by using the formula: Q = m * c * ΔT where ΔT is the temperature difference. Q = 5 * 860 * 80 Calculate the heat exchanged.
06

Calculate the entropy change for case (b)

For case (b), there are two entropy changes: one due to the change in potential energy and one due to the heat exchange: (a) For the change in potential energy: ΔS1 = m * g * h / T Use the same formula as in Step 4. (b) For the heat exchange: ΔS2 = Q / T Calculate the total change in entropy for case (b) as ΔS_total = ΔS1 + ΔS2.

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Key Concepts

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

Potential Energy
Potential energy is the energy stored in an object due to its position relative to a source of gravity. In this exercise, the rock has potential energy because it is at a height above the surface of the lake. The formula used to calculate potential energy is given by:
\( PE = m \cdot g \cdot h \)
where:
  • \( m \) is the mass of the rock in kilograms (kg)
  • \( g \) is the acceleration due to gravity, approximately \( 9.81 \, \text{m/s}^2 \)
  • \( h \) is the height in meters (m)
As the rock falls, its potential energy is converted into kinetic energy. Upon hitting the water, the potential energy the rock had at the height will be transformed and can contribute to changes in thermal and entropy states of the surrounding environment.
Temperature Change
Temperature change refers to the difference in temperature that an object experiences over time or between two separate states. In this problem, the rock originally at different temperatures before and after dropping undergoes different interactions with the lake's water.
For case (a), there is no temperature change when the rock (initially at \(20^{\circ} \text{C}\)) is placed in water also at \(20^{\circ} \text{C}\). Therefore, no net heat exchange directly affects temperature.
In case (b), the temperature initially at \(100^{\circ} \text{C}\) drops due to heat exchange with the lake water (which is at \(20^{\circ} \text{C}\)). The difference \( \Delta T \) is \(80^{\circ} \text{C}\). It plays a crucial role in determining the heat exchange, which subsequently affects entropy.
Specific Heat
Specific heat is a property of a material that measures how much heat energy is needed to change the temperature of a unit mass by one degree. It is essential in determining how a material reacts to temperature changes during heat transfer processes. The formula to calculate the heat energy (\(Q\)) is:
\( Q = m \cdot c \cdot \Delta T \)
where:
  • \( Q \) is the heat energy in joules (J)
  • \( c \) is the specific heat capacity of the material (for the rock, \(860 \, \text{J/kg} \cdot \text{K}\))
  • \( \Delta T \) is the temperature change in degrees Celsius or Kelvin
Using the specific heat, one can determine how the rock's higher initial temperature affects energy transfer, illustrating the concepts of energy conservation and transition between systems.
Heat Exchange
Heat exchange occurs when heat energy transfers between objects or systems. This commonly arises due to difference in temperature, as energy naturally flows from hotter to cooler areas until equilibrium is reached.
In the context of the exercise, once the rock hits the lake, it loses heat to the surrounding water in case (b) because its initial temperature exceeds that of the water. Using the previous sections, we calculate the heat exchange amount:
\( Q = 5 \times 860 \times 80 \)
This equation helps in deriving the alteration in entropy, factoring in both potential energy loss and heat dispersion, affecting the universe's overall entropy. Understanding heat exchange supports concepts of thermodynamics, especially regarding energy dispersion and equilibrium tendencies.

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Most popular questions from this chapter

A heat engine operates between two temperatures such that the working substance of the engine absorbs 5000 J of heat from the high-temperature bath and discharges 3000 J to the low-temperature bath. The rest of the energy is converted into mechanical energy of the turbine. Find (a) the amount of work produced by the engine and (b) the efficiency of the engine.

A Carnot engine employs 1.5 mol of nitrogen gas as a working substance, which is considered as an ideal diatomic gas with \(\gamma=7.5\) at the working temperatures of the engine. The Carnot cycle goes in the cycle \(A B C D A\) with \(A B\) being an isothermal expansion. The volume at points \(A\) and \(C\) of the cycle are \(5.0 \times 10^{-3} \mathrm{m}^{3}\) and 0.15 L, respectively. The engine operates between two themal baths of temperature \(500 \mathrm{K}\) and \(300 \mathrm{K}\). (a) Find the values of volume at \(B\) and \(D\). (b) How much heat is absorbed by the gas in the \(A B\) isothermal expansion? (c) How much work is done by the gas in the \(A B\) isothermal expansion? (d) How much heat is given up by the gas in the \(C D\) isothemal expansion? (e) How much work is done by the gas in the CD isothermal compression? (f) How much work is done by the gas in the \(B C\) adiabatic expansion? (g) How much work is done by the gas in the \(D A\) adiabatic compression? (h) Find the value of efficiency of the engine based on the net work and heat input. Compare this value to the efficiency of a Carnot engine based on the temperatures of the two baths.

An engine absorbs three times as much heat as it discharges. The work done by the engine per cycle is 50 J. Calculate (a) the efficiency of the engine, (b) the heat absorbed per cycle, and (c) the heat discharged per cycle.

Fifty grams of water at \(20^{\circ} \mathrm{C}\) is heated until it becomes vapor at \(100^{\circ} \mathrm{C}\). Calculate the change in entropy of the water in this process.

Two moles of nitrogen gas, with \(\gamma=7 / 5\) for ideal diatomic gases, occupies a volume of \(10^{-2} \mathrm{m}^{3}\) in an insulated cylinder at temperature 300 K. The gas is adiabatically and reversibly compressed to a volume of 5L. The piston of the cylinder is locked in its place, and the insulation around the cylinder is removed. The heatconducting cylinder is then placed in a 300 -K bath. Heat from the compressed gas leaves the gas, and the temperature of the gas becomes \(300 \mathrm{K}\) again. The gas is then slowly expanded at the fixed temperature \(300 \mathrm{K}\) until the volume of the gas becomes \(10^{-2} \mathrm{m}^{3},\) thus making a complete cycle for the gas. For the entire cycle, calculate (a) the work done by the gas, (b) the heat into or out of the gas, (c) the change in the internal energy of the gas, and (d) the change in entropy of the gas.

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