Problem 80
Question
The increase in internal energy of the system is 100 \(\mathrm{J}\) when \(300 \mathrm{~J}\) of heat is supplied to it. What is the amount of work done by the system (a) \(-200 \mathrm{~J}\) (b) \(+200 \mathrm{~J}\) (c) \(-300 \mathrm{~J}\) (d) \(-400 \mathrm{~J}\)
Step-by-Step Solution
Verified Answer
(b) +200 J
1Step 1: Understand the Problem
We need to find the amount of work done by the system when the internal energy change and the heat supplied to the system are given.
2Step 2: Know the Formula
The formula used to find the work done by the system when heat is added is the First Law of Thermodynamics: \( \Delta U = Q - W \), where \( \Delta U \) is the change in internal energy, \( Q \) is the heat added to the system, and \( W \) is the work done by the system.
3Step 3: Substitute the Values
Given that \( \Delta U = 100 \, \mathrm{J} \) and \( Q = 300 \, \mathrm{J} \), substitute these into the formula: \[ 100 = 300 - W \].
4Step 4: Solve for Work Done
Rearrange the equation to solve for \( W \): \[ W = 300 - 100 \] \[ W = 200 \, \mathrm{J} \].
5Step 5: Consider the Sign of Work
The calculated work is \( 200 \, \mathrm{J} \). Since energy is used to do work, it must be counted as positive work done by the system. Therefore, the answer is \(+200 \, \mathrm{J}\).
Key Concepts
Change in Internal EnergyHeat SuppliedWork Done by the System
Change in Internal Energy
When studying thermodynamics, one key concept is the change in internal energy, denoted as \( \Delta U \). Internal energy refers to the total energy contained within a system, arising from the kinetic and potential energies of its particles.
Internal energy can change in response to energy added or removed from the system. This is governed by the First Law of Thermodynamics, which is expressed as \( \Delta U = Q - W \). Here, \( Q \) is the heat supplied to the system, and \( W \) is the work done by the system.
The change in internal energy can be:
Internal energy can change in response to energy added or removed from the system. This is governed by the First Law of Thermodynamics, which is expressed as \( \Delta U = Q - W \). Here, \( Q \) is the heat supplied to the system, and \( W \) is the work done by the system.
The change in internal energy can be:
- Positive when the system gains energy.
- Negative when the system loses energy.
Heat Supplied
Heat is energy transferred due to a temperature difference between a system and its surroundings. In thermodynamics, it is a key factor affecting a system's energy balance.
When heat is supplied to a system, it can cause changes in both the internal energy and the work done. This relationship is captured by the First Law of Thermodynamics. For example, when heat is added to a system,
When heat is supplied to a system, it can cause changes in both the internal energy and the work done. This relationship is captured by the First Law of Thermodynamics. For example, when heat is added to a system,
- some of it increases the internal energy, which might raise the system's temperature.
- some might do work, such as expanding a gas.
Work Done by the System
In thermodynamics, work done by the system is the energy transferred from the system to its surroundings, often involving a force causing movement. It is denoted as \( W \) in equations.
When a system does work, it uses its internal energy. For example, imagine a gas expanding in a piston; the gas does work by pushing the piston outward, which decreases its internal energy. The formula \( \Delta U = Q - W \) shows that work done is subtracted from the heat supplied.
In this exercise:
When a system does work, it uses its internal energy. For example, imagine a gas expanding in a piston; the gas does work by pushing the piston outward, which decreases its internal energy. The formula \( \Delta U = Q - W \) shows that work done is subtracted from the heat supplied.
In this exercise:
- The change in internal energy was 100 J after 300 J of heat was supplied.
- The work done by the system was calculated as 200 J, meaning energy was used positively to perform work.
Other exercises in this chapter
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