A gas has a well-defined mean energy E when its volume is V and mean pressure is p. If the volume of the gas is changed quasi-statically, the mean pres- sure p (and energy E) of the gas will then change accordingly. Suppose that the gas is taken very slowly from a to b (see Fig. 5.18) while the gas is kept thermally insulated. In this case p is found to depend on the volume V in accordance with the relation

College Physics
11th Edition
ISBN:9781305952300
Author:Raymond A. Serway, Chris Vuille
Publisher:Raymond A. Serway, Chris Vuille
Chapter1: Units, Trigonometry. And Vectors
Section: Chapter Questions
Problem 1CQ: Estimate the order of magnitude of the length, in meters, of each of the following; (a) a mouse, (b)...
icon
Related questions
Question

Kindly solve 5.4 question urgent need help me thanks

4.5 Proposed method for producing polarized proton targets
In research in nuclear physics and elementary particles, it is, of great
interest to do scattering experiments on targets consisting of protons whose spins
are preferentially polarized in a given direction. Each proton has a spin and
a magnetic moment po=1.4 x 10-23 erg/gauss. Suppose that one tries to
apply the method of the preceding problem by taking a sample of paraffin (which
contains many protons), applying a magnetic field of 50,000 gauss, and cooling
the sample to some very low absolute temperature T. How low would this tem-
perature have to be so that, after equilibrium has been reached, the number of
proton moments pointing parallel to the field is at least 3 times as large as the
number of proton moments pointing in the opposite direction? Express your
answer again in terms of the ratio T/TR where TR is room temperature.
5.4 Work done in an adiabatic process
A gas has a well-defined mean energy E when its volume is V and mean
pressure is p. If the volume of the gas is changed quasi-statically, the mean pres-
sure p (and energy E) of the gas will then change accordingly. Suppose that the
gas is taken very slowly from a to b (see Fig. 5.18) while the gas is kept thermally
insulated. In this case p is found to depend on the volume V in accordance with
the relation
7 x V-5/3.
What is the work done on the gas in this process?
5.5 Work done in alternative processes connecting the same macrostates
The gas of Prob. 5.4 can also be brought quasi-statically from a to b in
various other ways. In particular, consider the following processes and calculate
for each the total work W done on the system and the total heat Q absorbed by
the system when it is brought quasi-statically from a to b. (See Fig. 5.18.)
Process a→→b. The system is compressed from its original to its final
volume, heat being removed to maintain the pressure constant. The volume
is then kept constant and heat is added to increase the mean pressure to 32 × 100
dynes cm 2,
Process adb. The two steps of the preceding process are performed
in the opposite order.
Process ab. The volume is decreased and heat is supplied so that the mean
pressure varies linearly with the volume.
(10° dynes cm²)
32
PV-5/3
8 V
(10³ cm³)
Fig. 5.18 Various processes illustrated on a
diagram of mean pressure p versus volume V.
Transcribed Image Text:4.5 Proposed method for producing polarized proton targets In research in nuclear physics and elementary particles, it is, of great interest to do scattering experiments on targets consisting of protons whose spins are preferentially polarized in a given direction. Each proton has a spin and a magnetic moment po=1.4 x 10-23 erg/gauss. Suppose that one tries to apply the method of the preceding problem by taking a sample of paraffin (which contains many protons), applying a magnetic field of 50,000 gauss, and cooling the sample to some very low absolute temperature T. How low would this tem- perature have to be so that, after equilibrium has been reached, the number of proton moments pointing parallel to the field is at least 3 times as large as the number of proton moments pointing in the opposite direction? Express your answer again in terms of the ratio T/TR where TR is room temperature. 5.4 Work done in an adiabatic process A gas has a well-defined mean energy E when its volume is V and mean pressure is p. If the volume of the gas is changed quasi-statically, the mean pres- sure p (and energy E) of the gas will then change accordingly. Suppose that the gas is taken very slowly from a to b (see Fig. 5.18) while the gas is kept thermally insulated. In this case p is found to depend on the volume V in accordance with the relation 7 x V-5/3. What is the work done on the gas in this process? 5.5 Work done in alternative processes connecting the same macrostates The gas of Prob. 5.4 can also be brought quasi-statically from a to b in various other ways. In particular, consider the following processes and calculate for each the total work W done on the system and the total heat Q absorbed by the system when it is brought quasi-statically from a to b. (See Fig. 5.18.) Process a→→b. The system is compressed from its original to its final volume, heat being removed to maintain the pressure constant. The volume is then kept constant and heat is added to increase the mean pressure to 32 × 100 dynes cm 2, Process adb. The two steps of the preceding process are performed in the opposite order. Process ab. The volume is decreased and heat is supplied so that the mean pressure varies linearly with the volume. (10° dynes cm²) 32 PV-5/3 8 V (10³ cm³) Fig. 5.18 Various processes illustrated on a diagram of mean pressure p versus volume V.
Expert Solution
steps

Step by step

Solved in 3 steps

Blurred answer
Knowledge Booster
Boltzmann Statistics of Ideal gas
Learn more about
Need a deep-dive on the concept behind this application? Look no further. Learn more about this topic, physics and related others by exploring similar questions and additional content below.
Recommended textbooks for you
College Physics
College Physics
Physics
ISBN:
9781305952300
Author:
Raymond A. Serway, Chris Vuille
Publisher:
Cengage Learning
University Physics (14th Edition)
University Physics (14th Edition)
Physics
ISBN:
9780133969290
Author:
Hugh D. Young, Roger A. Freedman
Publisher:
PEARSON
Introduction To Quantum Mechanics
Introduction To Quantum Mechanics
Physics
ISBN:
9781107189638
Author:
Griffiths, David J., Schroeter, Darrell F.
Publisher:
Cambridge University Press
Physics for Scientists and Engineers
Physics for Scientists and Engineers
Physics
ISBN:
9781337553278
Author:
Raymond A. Serway, John W. Jewett
Publisher:
Cengage Learning
Lecture- Tutorials for Introductory Astronomy
Lecture- Tutorials for Introductory Astronomy
Physics
ISBN:
9780321820464
Author:
Edward E. Prather, Tim P. Slater, Jeff P. Adams, Gina Brissenden
Publisher:
Addison-Wesley
College Physics: A Strategic Approach (4th Editio…
College Physics: A Strategic Approach (4th Editio…
Physics
ISBN:
9780134609034
Author:
Randall D. Knight (Professor Emeritus), Brian Jones, Stuart Field
Publisher:
PEARSON