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Ideal Gas Equation | 理想气体方程

2026-08-29 12:43 · 本文部分内容由AI辅助创作

📚 Ideal Gas Equation | 理想气体方程

pV = NkT, convert units correctly, and explain the assumptions behind the ideal gas model.

理想气体方程是A-Level热物理的核心关系之一。它将理想气体的压强、体积、物质的量和热力学温度联系在一个方程中。在CIE考纲中,你需要使用pV = nRT和pV = NkT,正确换算单位,并能解释理想气体模型背后的假设。


1. From Gas Laws to the Ideal Gas Equation | 从气体定律到理想气体方程

re p, volume V and absolute temperature T behave when one variable is held constant. Boyle's law gives pV = constant for fixed mass and temperature; Charles' fixed mass and pressure; the pressure law gives p/T = constant for fixed mass and volume.

实验气体定律描述了在没有物质交换且某个变量保持不变时,压强p、体积V和绝对温度T之间的关系。波义耳定律给出pV为常数;查理定律给出V/T为常数;压强定律给出p/T为常数。

Avogadro's law adds that at the same pressure and temperature, equal volumes of all ideal gases contain the same number of molecules. Combining these laws introduces the amount of substance n and leads to the ideal gas equation.

阿伏伽德罗定律补充指出,在相同压强和温度下,相同体积的所有理想气体含有相同的分子数。将这些定律综合起来,引入物质的量n,就得到理想气体方程。


2. The Equation pV = nRT | 方程 pV = nRT

The most common form of the ideal gas equation is:

理想气体方程最常用的形式是:

pV = nRT

Here p is pressure in pascals, V is volume in cubic metres, n is amount in moles, R is the molar gas constant, and T is absolute temperature in kelvin.

其中p是压强(单位帕斯卡),V是体积(单位立方米),n是物质的量(单位摩尔),R是摩尔气体常数,T是热力学温度(单位开尔文)。

The equation is called an equation of state because it relates the state variables of the gas. For a fixed mass, if any three quantities are known, the fourth can be calculated.

该方程被称为状态方程,因为它联系了气体的状态参量。对于一定质量的气体,只要已知其中三个量,就能求出第四个量。


3. Amount of Substance and the Mole | 物质的量与摩尔

mole contains exactly 6.02 × 10²³ elementary entities, known as the Avogadro constant Nₐ.

摩尔是物质的量的国际单位。1摩尔恰好包含6.02 × 10²³个基本单元,这个数称为阿伏伽德罗常数Nₐ。

deal gas calculations, molar mass must be expressed in kg mol⁻¹ if the other units are SI.

如果气体质量为m,摩尔质量为M,则摩尔数 n = m / M。在理想气体计算中,如果其他量采用SI单位,摩尔质量必须用kg mol⁻¹表示。

n = m / M


4. Gas Constant R and Boltzmann Constant k | 气体常数R与玻尔兹曼常数k

R = 8.31 J K⁻¹ mol⁻¹ is the molar gas constant. It is the same for all ideal gases.

R = 8.31 J K⁻¹ mol⁻¹ 是摩尔气体常数,对所有理想气体都相同。

Boltzmann' stant k relates R to the Avogadro constant by k = R / Nₐ. Its value is 1.38 × 10⁻²³ J K⁻¹.

玻尔兹曼常数k通过 k = R / Nₐ 与阿伏伽德罗常数相联系,其值为1.38 × 10⁻²³ J K⁻¹。

ConstantValueUse
R8.31 J K⁻¹ mol⁻¹pV = nRT
k1.38 × 10⁻²³ J K⁻¹pV = NkT
Nₐ6.02 × 10²³ mol⁻¹n = N / Nₐ

5. Alternative Form pV = NkT | 替代形式 pV = NkT

contains N molecules, then n = N / Nₐ. Substituting into pV = nRT gives the particle form:

如果气体含有N个分子,则 n = N / Nₐ。代入 pV = nRT 得到粒子形式:

pV = NkT

This form is especially useful in kinetic theory and particle physics because it counts individual molecules rather than moles.

这种形式在分子动理论和粒子物理中特别有用,因为它直接计数分子数,而不是摩尔数。


6. Molar Volume at Standard Conditions | 标准状况下的摩尔体积

ssure, taken as 273 K and 1.01 × 10⁵ Pa, one mole of an ideal gas occupies about 22.4 dm³.

在标准温度与压强下,即273 K和1.01 × 10⁵ Pa,1摩尔理想气体的体积约为22.4 dm³。

perature and pressure, about 298 K and 1.01 × 10⁵ Pa, the molar volume is close to 24 dm³.

摩尔体积可由 Vₘ = RT / p 求出。在室温常压下,约298 K和1.01 × 10⁵ Pa时,摩尔体积接近24 dm³。

You must remember that 1 m³ = 1000 dm³ = 1000 L, and 1 dm³ = 1 × 10⁻³ m³.

你必须记住 1 m³ = 1000 dm³ = 1000 L,而 1 dm³ = 1 × 10⁻³ m³。


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7. Units and Conversions in Ideal Gas Calculations | 理想气体计算中的单位与换算

K⁻¹ mol⁻¹, p must be in Pa, V in m³, and T in K. Convert kPa and cm³ before substituting.

使用 R = 8.31 J K⁻¹ mol⁻¹ 时,p必须用Pa,V必须用m³,T必须用K。代入前要换算kPa和cm³。

+ 273.15. In exam numerical work, 273 is often accepted unless high precision is required.

摄氏温度必须用 T(K) = θ(°C) + 273.15 换算。在考试计算中,除非要求高精度,通常使用273即可。


8. Assumptions of the Ideal Gas Model | 理想气体模型的假设

The ideal gas model assumes that gas particles occupy negligible volume, move randomly, exert no intermolecular forces except during elastic collisions, and collide elastically with the container walls.

理想气体模型假设:气体粒子自身体积可以忽略,粒子随机运动,除弹性碰撞外粒子间无分子力,粒子与容器壁的碰撞是弹性的。

These assumptions break down at high pressure and low temperature, where particle volume and attractive forces become important. Real gases approach ideal behaviour at low pressure and high temperature.

这些假设在高压和低温下失效,因为粒子体积和吸引力变得重要。真实气体在低压和高温下接近理想行为。


9. Linking to Boyle's, Charles's and Pressure Laws | 与波义耳定律、查理定律和压强定律的联系

For a fixed amount of gas at constant temperature, pV is constant, which is Boyle's law. At constant pressure, V/T is constant, which is Charles's law. At constant volume, p/T is constant, which is the pressure law.

对于一定量的气体,在温度不变时 pV 为常数,这就是波义耳定律;在压强不变时 V/T 为常数,这就是查理定律;在体积不变时 p/T 为常数,这就是压强定律。

Therefore the ideal gas equation does not replace these laws; it combines them and extends them to processes where none of p, V or T is constant, provided the amount of gas is known.

因此理想气体方程并不取代这些定律,而是将它们综合起来,并推广到p、V、T都不恒定的过程,只要气体的物质的量已知。


10. Worked Example: Moles from Pressure and Volume | 例题:由压强和体积求物质的量

volume 0.030 m³ contains nitrogen at 2.0 × 10⁵ Pa and 27 °C. Calculate the amount of gas.

一个体积为0.030 m³的气缸内装有压强为2.0 × 10⁵ Pa、温度为27 °C的氮气。计算气体的物质的量。

Convert the temperature: T = 27 + 273 = 300 K. Then use n = pV / RT:

换算温度:T = 27 + 273 = 300 K。然后使用 n = pV / RT:

n = (2.0 × 10⁵ Pa × 0.030 m³) / (8.31 J K⁻¹ mol⁻¹ × 300 K) ≈ 2.41 mol


11. Worked Example: Temperature from Mass and Pressure | 例题:由质量和压强求温度

as molar mass 0.032 kg mol⁻¹. It occupies 0.060 m³ at 1.50 × 10⁵ Pa. Find its temperature.

一个0.100 kg的氧气样品,摩尔质量为0.032 kg mol⁻¹。它在1.50 × 10⁵ Pa压强下占据0.060 m³的体积。求其温度。

First find n = m / M = 0.100 / 0.032 = 3.125 mol. Then T = pV / nR:

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