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2010-2011学年春季《热学》习题3(答案)

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2010-2011学年春季《热学》习题3(答案)2010-2011春 《热学》习题 第二章 分子动理学理论的平衡态理论 习题三: 质量为10Kg的氮气,当压强为1.0atm,体积为7700cm3 时,其分子的平均平动能是多少? 解: ∵ 而 ∴ 求常温下质量为m1=3.00g的水蒸气与m2=3.00g的氢气组成的混合理想气体的定体摩尔热容. 设:水蒸汽的定容比热为 ,氢气的定容比热为 ,则混合气体的定容比热可由 量热学 即 ,得 ,定容摩尔热容量 , 对混合气体,其平均摩尔质量满足关系: (注:(3)式可由理想气体...

2010-2011学年春季《热学》习题3(答案)
2010-2011春 《热学》习题 第二章 分子动理学理论的平衡态理论 习题三: 质量为10Kg的氮气,当压强为1.0atm,体积为7700cm3 时,其分子的平均平动能是多少? 解: ∵ 而 ∴ 求常温下质量为m1=3.00g的水蒸气与m2=3.00g的氢气组成的混合理想气体的定体摩尔热容. 设:水蒸汽的定容比热为 ,氢气的定容比热为 ,则混合气体的定容比热可由 量热学 即 ,得 ,定容摩尔热容量 , 对混合气体,其平均摩尔质量满足关系: (注:(3)式可由理想气体状态方程及道尔顿分压定律得出。) 综合上述三式,其中 ,可得 , 令:水蒸汽和氢气的定容摩尔热容量分别为 、 ,则上式变为 , 对水蒸汽, 对氢气, ,故有 在等温大气模式中,设气温为5oC,同时测得海平面的大气压和山顶的气压分别为 和 ,试问山顶的海拔为多少? 解:根据玻尔兹曼分布律,可得等温高度公式,代入数据,得 。 当液体与其饱和蒸气共存时,气化率与凝结率相等。设所有碰到液面上的蒸气分子都能凝结为液体,并假定当把液面上的蒸气迅速抽去时,液体的气化率与存在饱和蒸气时的气化率相同。已知水银在0oC时的饱和蒸气压为 ,问每秒通过每平方厘米液面有多少克水银向真空中气化。 解:以饱和蒸汽为研究对象,设所有碰到液面的蒸汽分子都凝结为液体,则 内碰到 液面的气体质量为: 代入数据: 得 。 按题意,假设凝结率等于汽化率,则该结果也就是每秒通过每平方厘米液面逸出的水银分子的质量。 某种气体的分子由四个原子组成,它们分别处在正四面体的四个顶点上。(1)求这种分子的平动、转动和振动自由度数;(2)根据能量均分定理求这种气体的定容摩尔热容。 解: (1)因n个原子组成的分子最多有3n个自由度。其中3个平动自由度,3个转动自由度, 3n-6个是振动自由度,这里n=4, ,故有12个自由度。 (2)作刚性近似,自由度数 , A sealed cubical container 20.0 cm on a side contains three times Avogadro’s number of molecules at a temperature of 20.0℃. Find the force exerted by the gas on one of the walls of the container. [Answer] Now , , the mole of the gas , the side length of the container One-sided area of the container The volume of the container Assuming the gas is ideal, according to the Equation of State for an ideal gas, So Then, the force exerted by the gas on one of the walls of the container In a period of 1.00 s, 5.00×1023 nitrogen molecules strike a wall with an area of 8.00 cm2. If the molecules move with a speed of 300 m/s and strike the wall head on in perfectly elastic collisions, what is the pressure exerted on the wall? (The mass of one N2 molecule is 4.68×10-26 kg.) [Answer] the mole of nitrogen molecules The total mass of nitrogen molecules Assuming the velocity attitude of nitrogen molecules before collision is the positive direction, so the speeds of nitrogen molecules before collision and after collision are and , respectively. According to the Momentum theorem, the impulse of single nitrogen molecule caused by the wall is The minus sign represents the direction of the impulse of nitrogen molecule is opposite to that of the velocity. The total impulse of all nitrogen molecules is The force of the nitrogen molecules caused by wall is According to The Newton third law, the force exerted by the nitrogen molecules on the wall is Since the area of the wall strike by nitrogen molecules The pressure exerted on the wall In a constant-volume process, 209J of energy is transferred by heat to 1.00mol of an ideal monatomic gas initially at 300K. Find (1) the increase in internal energy of the gas. (2) The work it does. (3) Its final temperature. [Answer] (1) In the constant-volume process, the energy was transformed into internal energy, so the increase of the internal energy is 209J. In the constant-volume process, the system does not do work, so the work it does is 0J. So, So the final temperature is 316.77K One mole of an ideal diatomic gas with occupies a volume at a pressure . The gas undergoes a process in which the pressure is proportional to the volume. At the end of the process, it is found that of the gas molecules has doubled from its initial value. Determine the amount of energy transferred to the gas by heat. [Answer] According to the equation of state for an ideal gas, So The dimensions of a room are 4.20m×3.00m×2.50m. (1) Find the number of molecules of air in it at atmospheric pressure and 20.0℃. (2) Find the mass of this air, assuming that the air consists of diatomic molecules with a molar mass of 28.9g/mol. (3) Find the average kinetic energy of a molecule. (4) Find the root-mean-square molecular speed. (5) On the assumption that the specific heat is a constant independent of temperature, we have . Find the internal energy in the air. (6) Find the internal energy of the air in the room at 25.0℃. [Answer] According to the equation of state for an ideal gas, So, According to the equation of state for an ideal gas, So, , 4 邢玉梅2011-05-01 _1234567921.unknown _1234567937.unknown _1234567945.unknown _1234567953.unknown _1234567957.unknown _1234567961.unknown _1234567963.unknown _1234567965.unknown _1234567966.unknown _1234567967.unknown _1234567964.unknown _1234567962.unknown _1234567959.unknown _1234567960.unknown _1234567958.unknown _1234567955.unknown _1234567956.unknown _1234567954.unknown _1234567949.unknown _1234567951.unknown _1234567952.unknown _1234567950.unknown _1234567947.unknown _1234567948.unknown _1234567946.unknown _1234567941.unknown _1234567943.unknown _1234567944.unknown _1234567942.unknown _1234567939.unknown _1234567940.unknown _1234567938.unknown _1234567929.unknown _1234567933.unknown _1234567935.unknown _1234567936.unknown _1234567934.unknown _1234567931.unknown _1234567932.unknown _1234567930.unknown _1234567925.unknown _1234567927.unknown _1234567928.unknown _1234567926.unknown _1234567923.unknown _1234567924.unknown _1234567922.unknown _1234567905.unknown _1234567913.unknown _1234567917.unknown _1234567919.unknown _1234567920.unknown _1234567918.unknown _1234567915.unknown _1234567916.unknown _1234567914.unknown _1234567909.unknown _1234567911.unknown _1234567912.unknown _1234567910.unknown _1234567907.unknown _1234567908.unknown _1234567906.unknown _1234567897.unknown _1234567901.unknown _1234567903.unknown _1234567904.unknown _1234567902.unknown _1234567899.unknown _1234567900.unknown _1234567898.unknown _1234567893.unknown _1234567895.unknown _1234567896.unknown _1234567894.unknown _1234567891.unknown _1234567892.unknown _1234567890.unknown
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