/*! 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 1194 A Carnot engine Converts one six... [FREE SOLUTION] | 91Ó°ÊÓ

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A Carnot engine Converts one sixth of the heat input into work. When the temperature of the sink is reduced by \(62^{\circ} \mathrm{C}\) the efficiency of the engine is doubled. The temperature of the source and sink are (A) \(80^{\circ} \mathrm{C}, 37^{\circ} \mathrm{C}\) (B) \(95^{\circ} \mathrm{C}, 28^{\circ} \mathrm{C}\) (C) \(90^{\circ} \mathrm{C}, 37^{\circ} \mathrm{C}\) (D) \(99^{\circ} \mathrm{C}, 37^{\circ} \mathrm{C}\)

Short Answer

Expert verified
The temperatures of the source and sink are \(99^{\circ}\mathrm{C}\) and \(37^{\circ}\mathrm{C}\), which corresponds to option (D).

Step by step solution

01

Set up the initial efficiency equation

Using the efficiency formula, we have \( \frac{1}{6} = 1 - \frac{T_s}{T_r} \) Where \(T_s\) is the temperature of the sink, and \(T_r\) is the temperature of the source.
02

Set up the efficiency equation after the sink temperature is reduced

When the sink temperature is reduced by 62°C, the efficiency doubles. Let the new sink temperature be marked as \(T_s' = T_s - 62 \). The efficiency equation becomes: \( \frac{1}{3} = 1 - \frac{T_s - 62}{T_r} \)
03

Solve the system of equations

Now, we have a system of two equations: 1. \( \frac{1}{6} = 1 - \frac{T_s}{T_r} \) 2. \( \frac{1}{3} = 1 - \frac{T_s - 62}{T_r} \) To solve this, we can rewrite equation (1): \(T_s = T_r - \frac{T_r}{6} \) Now substitute this in equation (2): \( \frac{1}{3} = 1 - \frac{(T_r - \frac{T_r}{6}) - 62}{T_r} \) Solve for \(T_r\).
04

Calculate the temperature of the source

After solving the equation, we find that the temperature of the source is: \( T_r = 372 K \) We need to convert this to degrees Celsius: \[ T_r^{\circ}C = T_rK - 273 \] \( T_r^{\circ}C = 372 - 273 = 99^{\circ}C \)
05

Calculate the temperature of the sink

Now we can substitute the source temperature back into equation (1) to get the sink temperature: \( T_s = T_r - \frac{T_r}{6} \) \( T_s = 99 - \frac{99}{6} = 310 K \) To convert this to degrees Celsius: \[ T_s^{\circ}C = T_sK - 273 \] \( T_s^{\circ}C = 310 - 273 = 37^{\circ}C \) This matches option (D) \(99^{\circ}\mathrm{C}, 37^{\circ}\mathrm{C}\).

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Key Concepts

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

Heat Input Conversion
In the given exercise, a Carnot engine transforms heat input into work. This relationship is governed by the engine's efficiency. Carnot engines are benchmarked for their ideal efficiency, expressed in a simple mathematical form. In this case, the engine is converting only one-sixth of its heat input into useful work. This fraction, \( \frac{1}{6} \), represents an initial efficiency level. With heat conversion, it's about maximizing the amount of heat input transformed into work. Efficiency then becomes an equation expressing the difference between the heat input and what remains after energy conversion. As the efficiency implies, not all input heat translates to work—some dissipates, maintaining the roles of the source and sink in heat exchange.
Temperature Sink Reduction
Temperatures in thermodynamic systems, like a Carnot engine, play crucial roles in determining efficiency. The temperature of the sink—or the environment where waste heat dissipates—can directly alter an engine's performance. By reducing the temperature of this sink by \(62^{\circ} \mathrm{C}\), as described in the problem, the efficiency of the engine doubles. The sink reduction becomes a pivotal move in minimizing heat waste and increasing the mechanical work produced. Why does this happen? Simply put, a lower temperature sink results in less energy required for heat dissipation, shifting more heat input towards work conversion. Thus, understanding and manipulating temperatures within these systems are key for optimizing engine performance.
System of Equations in Thermodynamics
Equations are backbone elements in understanding and solving for thermodynamic variables like temperature or efficiency. In this exercise, we are faced with a system of equations to find the source and sink temperatures. The first equation comes from the original efficiency setup, \( \frac{1}{6} = 1 - \frac{T_s}{T_r} \), representing the initial state. The second, \( \frac{1}{3} = 1 - \frac{T_s - 62}{T_r} \), accounts for the doubled efficiency after reducing the sink's temperature. Solving these equations involves isolating variables and substituting values. This leads us to solve for the temperatures mathematically, ensuring each step logically follows from thermodynamic principles. Systems of equations are fundamental in predicting changes in systems and iidentifying ideal states of operation.
Temperature Conversion Kelvin to Celsius
In thermodynamics, temperatures are often measured in Kelvin (K), but practical daily use and problem-solving sometimes require results in Celsius (°C). To convert Kelvin to Celsius, use the simple formula: \( T_{\mathrm{C}} = T_{\mathrm{K}} - 273.15 \). In our task, once solved in Kelvin, we need to translate the source and sink temperatures. The source temperature was found to be \(372K\) which converts to \(99^{\circ}C\) and the sink temperature was \(310K\), corresponding to \(37^{\circ}C\). Keeping this conversion handy allows us to easily interpret thermodynamic values in everyday contexts.

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Most popular questions from this chapter

Instructions:Read the assertion and reason carefully to mask the correct option out of the options given below. (A) If both assertion and reason are true and the reason is the correct explanation of the assertion. (B) If both assertion and reason are true but reason is not be correct explanation of assertion. (C) If assertion is true but reason is false. (D) If the assertion and reason both are false. Assertion: The carnot is useful in understanding the performance of heat engine Reason: The carnot cycle provides a way of determining the maximum possible efficiency achievable with reservoirs of given temperatures. (A) \(\mathrm{A}\) (B) B (C) \(\mathrm{C}\) (D) \(\mathrm{D}\)

The efficiency of Carnot's engine operating between reservoirs, maintained at temperature \(27^{\circ} \mathrm{C}\) and \(-123^{\circ} \mathrm{C}\) is (A) \(0.5\) (B) \(0.4\) (C) \(0.6\) (D) \(0.25\)

Two cylinders \(\mathrm{A}\) and \(\mathrm{B}\) fitted with piston contain equal amounts of an ideal diatomic gas at \(300 \mathrm{k}\). The piston of \(\mathrm{A}\) is free to move, While that of \(\mathrm{B}\) is held fixed. The same amount of heat is given to the gas in each cylinders. If the rise in temperature of the gas in \(\mathrm{A}\) is \(30 \mathrm{~K}\), then the rise in temperature of the gas in \(\mathrm{B}\) is. (A) \(30 \mathrm{~K}\) (B) \(42 \mathrm{~K}\) (C) \(18 \mathrm{~K}\) (D) \(50 \mathrm{~K}\)

The efficiency of heat engine is \(30 \%\) If it gives \(30 \mathrm{KJ}\) heat to the heat sink, than it should have absorbed ....... KJ heat from heat source. (A) \(42.8\) (B) 39 (C) 29 (D) 9

If for a gas \(\left(\mathrm{C}_{\mathrm{p}} / \mathrm{C}_{\mathrm{v}}\right)=1.67\), this gas is made up to molecules which are (A) diatomic (B) Polytomic (C) monoatomic (D) mixnese of diatomic and polytomic molecules

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