EBK PHYSICS FOR SCIENTISTS AND ENGINEER
EBK PHYSICS FOR SCIENTISTS AND ENGINEER
6th Edition
ISBN: 9781319321710
Author: Mosca
Publisher: VST
bartleby

Videos

Question
Book Icon
Chapter 25, Problem 102P

(a)

To determine

The battery current just after closing switch S.

(a)

Expert Solution
Check Mark

Answer to Problem 102P

The battery current just after closing the switch S is 3.42A .

Explanation of Solution

Given:

The value of emf is ε=50.0V .

The value of capacitances are C1=10.0μF and C2=5.0μF .

Formula used:

Apply Kirchhoff’s rule in circuit just after switch is closed,

  εI0(10.0Ω)I0Req=0 ..... (1)

Here, I0 is initial current in battery just after closing the switch.

Calculation:

The equivalent resistance of parallel resistors 15.0Ω,12.0Ω and 15.0Ω is calculated as,

  1R eq=115.0Ω+112.0Ω+115.0Ω1R eq=4+5+460Req=6013Req=4.615Ω

From equation (1), the battery current just after closing switch S is calculated as,

  (50.0V)I0(10.0Ω)I0(4.615Ω)=0I0(14.615Ω)=50.0VI0=3.42A

Conclusion:

Therefore, the battery current just after closing the switch S is 3.42A .

(b)

To determine

The battery current a long time after closing the switch S.

(b)

Expert Solution
Check Mark

Answer to Problem 102P

The battery current a long time after closing the switch S is 0.962A .

Explanation of Solution

Formula used:

Apply Kirchhoff’s rule in circuit a long time after switch is closed,

  εI(10.0Ω)IReq=0 ..... (2)

Here, I is initial current in battery a long time after closing the switch.

Calculation:

The equivalent resistance of series resistors 15.0Ω,12.0Ω and 15.0Ω is calculated as,

  Req=(15.0Ω)+(12.0Ω)+(15.0Ω)=42.0Ω

From equation (2), the battery current a long time after closing switch S is calculated as,

  (50.0V)I(10.0Ω)I(42.0Ω)=0I(52.0Ω)=50.0VI=0.962A

Conclusion:

Therefore, the battery current a long time after closing the switch S is 0.962A .

(c)

To determine

The charges on capacitors plates a long time after closing the switch S.

(c)

Expert Solution
Check Mark

Answer to Problem 102P

The charges on capacitors plates a long time after closing the switch S are 260μC and 130μC respectively.

Explanation of Solution

Formula used:

Apply Kirchhoff’s rule in circuit containing resistors 15.0Ω , 12.0Ω and capacitors 10.0μF ,

  V10.0μFI(15.0Ω)I(12.0Ω)=0 ..... (3)

Apply Kirchhoff’s rule in circuit containing resistors 15.0Ω , 12.0Ω and capacitors 5.00μF ,

  V5.00μFI(15.0Ω)I(12.0Ω)=0 ..... (4)

The expression for charge on capacitor 10.0μF is,

  Q10.0μF=C1V10.0μF

The expression for charge on capacitor 5.00μF is,

  Q5.00μF=C2V5.00μF

Calculation:

From equation (3), the potential difference V10.0μF is calculated as,

  V10.0μF(0.962A)(15.0Ω)(0.962A)(12.0Ω)=0V10.0μF=(27.0A)(0.962A)V10.0μF=25.974V

From equation (4), the potential difference V5.00μF is calculated as,

  V5.00μF(0.962A)(15.0Ω)(0.962A)(12.0Ω)=0V5.00μF=(27.0A)(0.962A)V5.00μF=25.974V

The charge on charge on capacitor 10.0μF is calculated as,

  Q10.0μF=(10.0μF)(25.974V)=259.74μC260μC

The charge on charge on capacitor 5.00μF is calculated as,

  Q5.00μF=(5.00μF)(25.974V)=129.87μC130μC

Conclusion:

Therefore, the charges on capacitors plates a long time after closing the switch S are 260μC and 130μC respectively.

(d)

To determine

The charges on capacitors plates a long time after reopening the switch S.

(d)

Expert Solution
Check Mark

Answer to Problem 102P

The charges on capacitors plates a long time after reopening the switch S is zero.

Explanation of Solution

Calculation:

If the switch S is reopened, then after long time there will not be any flow of current in the circuit. Thus,

  I=0

The potential difference across 10.0μF and 5.00μF capacitors will be zero,

  V10.0μF=V5.00μF=0

The charges on 10.0μF and 5.00μF capacitors will be zero,

  Q10.0μF=Q5.00μF=0

Conclusion:

Therefore, the charges on capacitors plates a long time after reopening the switch S is zero.

Want to see more full solutions like this?

Subscribe now to access step-by-step solutions to millions of textbook problems written by subject matter experts!
Students have asked these similar questions
A cylinder with a piston contains 0.153 mol of nitrogen at a pressure of 1.83×105 Pa and a temperature of 290 K. The nitrogen may be treated as an ideal gas. The gas is first compressed isobarically to half its original volume. It then expands adiabatically back to its original volume, and finally it is heated isochorically to its original pressure. Part A Compute the temperature at the beginning of the adiabatic expansion. Express your answer in kelvins. ΕΠΙ ΑΣΦ T₁ = ? K Submit Request Answer Part B Compute the temperature at the end of the adiabatic expansion. Express your answer in kelvins. Π ΑΣΦ T₂ = Submit Request Answer Part C Compute the minimum pressure. Express your answer in pascals. ΕΠΙ ΑΣΦ P = Submit Request Answer ? ? K Pa
Learning Goal: To understand the meaning and the basic applications of pV diagrams for an ideal gas. As you know, the parameters of an ideal gas are described by the equation pV = nRT, where p is the pressure of the gas, V is the volume of the gas, n is the number of moles, R is the universal gas constant, and T is the absolute temperature of the gas. It follows that, for a portion of an ideal gas, pV = constant. Τ One can see that, if the amount of gas remains constant, it is impossible to change just one parameter of the gas: At least one more parameter would also change. For instance, if the pressure of the gas is changed, we can be sure that either the volume or the temperature of the gas (or, maybe, both!) would also change. To explore these changes, it is often convenient to draw a graph showing one parameter as a function of the other. Although there are many choices of axes, the most common one is a plot of pressure as a function of volume: a pV diagram. In this problem, you…
Learning Goal: To understand the meaning and the basic applications of pV diagrams for an ideal gas. As you know, the parameters of an ideal gas are described by the equation pV = nRT, where p is the pressure of the gas, V is the volume of the gas, n is the number of moles, R is the universal gas constant, and T is the absolute temperature of the gas. It follows that, for a portion of an ideal gas, pV = constant. T One can see that, if the amount of gas remains constant, it is impossible to change just one parameter of the gas: At least one more parameter would also change. For instance, if the pressure of the gas is changed, we can be sure that either the volume or the temperature of the gas (or, maybe, both!) would also change. To explore these changes, it is often convenient to draw a graph showing one parameter as a function of the other. Although there are many choices of axes, the most common one is a plot of pressure as a function of volume: a pV diagram. In this problem, you…

Chapter 25 Solutions

EBK PHYSICS FOR SCIENTISTS AND ENGINEER

Ch. 25 - Prob. 11PCh. 25 - Prob. 12PCh. 25 - Prob. 13PCh. 25 - Prob. 14PCh. 25 - Prob. 15PCh. 25 - Prob. 16PCh. 25 - Prob. 17PCh. 25 - Prob. 18PCh. 25 - Prob. 19PCh. 25 - Prob. 20PCh. 25 - Prob. 21PCh. 25 - Prob. 22PCh. 25 - Prob. 23PCh. 25 - Prob. 24PCh. 25 - Prob. 25PCh. 25 - Prob. 26PCh. 25 - Prob. 27PCh. 25 - Prob. 28PCh. 25 - Prob. 29PCh. 25 - Prob. 30PCh. 25 - Prob. 31PCh. 25 - Prob. 32PCh. 25 - Prob. 33PCh. 25 - Prob. 34PCh. 25 - Prob. 35PCh. 25 - Prob. 36PCh. 25 - Prob. 37PCh. 25 - Prob. 38PCh. 25 - Prob. 39PCh. 25 - Prob. 40PCh. 25 - Prob. 41PCh. 25 - Prob. 42PCh. 25 - Prob. 43PCh. 25 - Prob. 44PCh. 25 - Prob. 45PCh. 25 - Prob. 46PCh. 25 - Prob. 47PCh. 25 - Prob. 48PCh. 25 - Prob. 49PCh. 25 - Prob. 50PCh. 25 - Prob. 51PCh. 25 - Prob. 52PCh. 25 - Prob. 53PCh. 25 - Prob. 54PCh. 25 - Prob. 55PCh. 25 - Prob. 56PCh. 25 - Prob. 57PCh. 25 - Prob. 58PCh. 25 - Prob. 59PCh. 25 - Prob. 60PCh. 25 - Prob. 61PCh. 25 - Prob. 62PCh. 25 - Prob. 63PCh. 25 - Prob. 64PCh. 25 - Prob. 65PCh. 25 - Prob. 66PCh. 25 - Prob. 67PCh. 25 - Prob. 68PCh. 25 - Prob. 69PCh. 25 - Prob. 70PCh. 25 - Prob. 71PCh. 25 - Prob. 72PCh. 25 - Prob. 73PCh. 25 - Prob. 74PCh. 25 - Prob. 75PCh. 25 - Prob. 76PCh. 25 - Prob. 77PCh. 25 - Prob. 78PCh. 25 - Prob. 79PCh. 25 - Prob. 80PCh. 25 - Prob. 81PCh. 25 - Prob. 82PCh. 25 - Prob. 83PCh. 25 - Prob. 84PCh. 25 - Prob. 85PCh. 25 - Prob. 86PCh. 25 - Prob. 87PCh. 25 - Prob. 88PCh. 25 - Prob. 89PCh. 25 - Prob. 90PCh. 25 - Prob. 91PCh. 25 - Prob. 92PCh. 25 - Prob. 93PCh. 25 - Prob. 94PCh. 25 - Prob. 95PCh. 25 - Prob. 96PCh. 25 - Prob. 97PCh. 25 - Prob. 98PCh. 25 - Prob. 99PCh. 25 - Prob. 100PCh. 25 - Prob. 101PCh. 25 - Prob. 102PCh. 25 - Prob. 103PCh. 25 - Prob. 104PCh. 25 - Prob. 105PCh. 25 - Prob. 106PCh. 25 - Prob. 107PCh. 25 - Prob. 108PCh. 25 - Prob. 109PCh. 25 - Prob. 110PCh. 25 - Prob. 111PCh. 25 - Prob. 112PCh. 25 - Prob. 113PCh. 25 - Prob. 114PCh. 25 - Prob. 115PCh. 25 - Prob. 116PCh. 25 - Prob. 117PCh. 25 - Prob. 118PCh. 25 - Prob. 119PCh. 25 - Prob. 120P
Knowledge Booster
Background pattern image
Physics
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.
Similar questions
SEE MORE QUESTIONS
Recommended textbooks for you
Text book image
College Physics
Physics
ISBN:9781938168000
Author:Paul Peter Urone, Roger Hinrichs
Publisher:OpenStax College
Text book image
Physics for Scientists and Engineers: Foundations...
Physics
ISBN:9781133939146
Author:Katz, Debora M.
Publisher:Cengage Learning
Text book image
Physics for Scientists and Engineers, Technology ...
Physics
ISBN:9781305116399
Author:Raymond A. Serway, John W. Jewett
Publisher:Cengage Learning
Text book image
Principles of Physics: A Calculus-Based Text
Physics
ISBN:9781133104261
Author:Raymond A. Serway, John W. Jewett
Publisher:Cengage Learning
Text book image
College Physics
Physics
ISBN:9781285737027
Author:Raymond A. Serway, Chris Vuille
Publisher:Cengage Learning
Text book image
University Physics Volume 2
Physics
ISBN:9781938168161
Author:OpenStax
Publisher:OpenStax
DC Series circuits explained - The basics working principle; Author: The Engineering Mindset;https://www.youtube.com/watch?v=VV6tZ3Aqfuc;License: Standard YouTube License, CC-BY