English
Karnataka Board PUCPUC Science Class 11

The Ratio of the Molar Heat Capacities of an Ideal Gas is Cp/Cv = 7/6.

Advertisements
Advertisements

Question

The ratio of the molar heat capacities of an ideal gas is Cp/Cv = 7/6. Calculate the change in internal energy of 1.0 mole of the gas when its temperature is raised by 50 K (a) keeping the pressure constant (b) keeping the volume constant and (c) adiaba

Answer in Brief
Advertisements

Solution

Given:

`(("C""p")/("C""v")) = 7/6`

Number of moles of the gas, n = 1 mol
Change in temperature of the gas, ∆T = 50 K   
(a) Keeping the pressure constant:
Using the first law of thermodynamics,

dQ= dU+dW

`triangle"T" = 50 "K" and gamma  = 7/6`

dQ =dU +dW

work done , dW =PdV

As pressure is kept constant, work done = P(Δ V)

Using the ideal gas equation PV =nRT,

P(ΔV) =nR(ΔT)

⇒ dW =nR(ΔT)

At constant pressure, dQ=nCpdT

Substituting these values in the first law of thermodynamics, we get

nCp dT = dU + RdT
⇒ dU = nCp dT − RdT

Using `"C"^"p"/("C""v") = gamma and "C"_"p" -"C"_"v" = "R", we get`

`"d""U" = 1 xx ("R"gamma)/((gamma -1)) xx "d""T" -"R""d""T"`

 = 7 RdT − RdT
   = 7 RdT − RdT = 6 RdT
   = 6 × 8.3 × 50 = 2490 J

(b) Keeping volume constant:
Work done = 0
Using the first law of thermodynamics,
dU  = dQ
dU = nCv dT

`= 1 xx "R"/(gamma-1) xx "d""T"`

`= 1 xx (8.3/(7/6 - 1)) xx 50`

= 8.3 × 50 × 6 = 2490 J

(c) Adiabatically, dQ = 0
Using the first law of thermodynamics, we get
dU = − dW

=`[("n" xx "R")/(gamma - 1) ("T"_1-"T"_2)]`

= `(1 xx 8.3)/(7/6 -1) = ("T"_2 -"T"_1)`

= 8.3 × 6 ×  50 =2490 J

shaalaa.com
Interpretation of Temperature in Kinetic Theory - Introduction of Kinetic Theory of an Ideal Gas
  Is there an error in this question or solution?
Chapter 27: Specific Heat Capacities of Gases - Exercises [Page 77]

APPEARS IN

HC Verma Concepts of Physics Volume 1 and 2 [English]
Chapter 27 Specific Heat Capacities of Gases
Exercises | Q 5 | Page 77

RELATED QUESTIONS

Keeping the number of moles, volume and temperature the same, which of the following are the same for all ideal gases?


The average momentum of a molecule in a sample of an ideal gas depends on


Consider the quantity \[\frac{MkT}{pV}\] of an ideal gas where M is the mass of the gas. It depends on the


Calculate the volume of 1 mole of an ideal gas at STP.


Find the number of molecules in 1 cm3 of an ideal gas at 0°C and at a pressure of 10−5mm of mercury.

Use R = 8.31 J K-1 mol-1


Let Q and W denote the amount of heat given to an ideal gas and the work done by it in an isothermal process.


A vessel containing one mole of a monatomic ideal gas (molecular weight = 20 g mol−1) is moving on a floor at a speed of 50 m s−1. The vessel is stopped suddenly. Assuming that the mechanical energy lost has gone into the internal energy of the gas, find the rise in its temperature.


An amount Q of heat is added to a monatomic ideal gas in a process in which the gas performs a work Q/2 on its surrounding. Find the molar heat capacity for the process


Two ideal gases have the same value of Cp / Cv = γ. What will be the value of this ratio for a mixture of the two gases in the ratio 1 : 2?


The volume of an ideal gas (γ = 1.5) is changed adiabatically from 4.00 litres to 3.00 litres. Find the ratio of (a) the final pressure to the initial pressure and (b) the final temperature to the initial temperature.


Consider a given sample of an ideal gas (Cp/Cv = γ) having initial pressure p0 and volume V0. (a) The gas is  isothermally taken to a pressure p0/2 and from there, adiabatically to a pressure p0/4. Find the final volume. (b) The gas is brought back to its initial state. It is adiabatically taken to a pressure p0/2 and from there, isothermally to a pressure p0/4. Find the final volume.


Two samples A and B, of the same gas have equal volumes and pressures. The gas in sample A is expanded isothermally to double its volume and the gas in B is expanded adiabatically to double its volume. If the work done by the gas is the same for the two cases, show that γ satisfies the equation 1 − 21−γ = (γ − 1) ln2.


1 litre of an ideal gas (γ = 1.5) at 300 K is suddenly compressed to half its original volume. (a) Find the ratio of the final pressure to the initial pressure. (b) If the original pressure is 100 kPa, find the work done by the gas in the process. (c) What is the change in internal energy? (d) What is the final temperature? (e) The gas is now cooled to 300 K keeping its pressure constant. Calculate the work done during the process. (f) The gas is now expanded isothermally to achieve its original volume of 1 litre. Calculate the work done by the gas. (g) Calculate the total work done in the cycle.


The figure shows an adiabatic cylindrical tube of volume V0 divided in two parts by a frictionless adiabatic separator. Initially, the separator is kept in the middle, an ideal gas at pressure p1 and temperature T1 is injected into the left part and another ideal gas at pressure p2 and temperature T2 is injected into the right part. Cp/Cv = γ is the same for both the gases. The separator is slid slowly and is released at a position where it can stay in equilibrium. Find (a) the volumes of the two parts (b) the heat given to the gas in the left part and (c) the final common pressure of the gases.


Diatomic molecules like hydrogen have energies due to both translational as well as rotational motion. From the equation in kinetic theory `pV = 2/3` E, E is ______.

  1. the total energy per unit volume.
  2. only the translational part of energy because rotational energy is very small compared to the translational energy.
  3. only the translational part of the energy because during collisions with the wall pressure relates to change in linear momentum.
  4. the translational part of the energy because rotational energies of molecules can be of either sign and its average over all the molecules is zero.

We have 0.5 g of hydrogen gas in a cubic chamber of size 3 cm kept at NTP. The gas in the chamber is compressed keeping the temperature constant till a final pressure of 100 atm. Is one justified in assuming the ideal gas law, in the final state?

(Hydrogen molecules can be consider as spheres of radius 1 Å).


Share
Notifications

Englishहिंदीमराठी


      Forgot password?
Use app×