That reminds me… must download the test prep HW.

Slides:



Advertisements
Similar presentations
An insulating sphere of radius b has a spherical cavity of radius a located within its volume and centered a distance R from the center of the sphere.
Advertisements

Chapter 22: The Electric Field II: Continuous Charge Distributions
A rod is bent into an eighth of a circle of radius a, as shown. The rod carries a total positive charge +Q uniformly distributed over its length. What.
Physics 1502: Lecture 4 Today’s Agenda Announcements: –Lectures posted on: –HW assignments, solutions.
Slide 1 Electric Field Lines 10/29/08. Slide 2Fig 25-21, p.778 Field lines at a conductor.
Today’s agenda: Announcements. Gauss’ Law Examples. You must be able to use Gauss’ Law to calculate the electric field of a high-symmetry charge distribution.
Physics 1502: Lecture 3 Today’s Agenda Announcements: –Lectures posted on: –HW assignments, solutions.
a b c Gauss’ Law … made easy To solve the above equation for E, you have to be able to CHOOSE A CLOSED SURFACE such that the integral is TRIVIAL. (1)
III.A 3, Gauss’ Law.
Electricity and Magnetism Review 1: Units 1-6
Electric Flux and Gauss Law
Chapter 22 Gauss’s Law Chapter 22 opener. Gauss’s law is an elegant relation between electric charge and electric field. It is more general than Coulomb’s.
Physics 2112 Unit 4: Gauss’ Law
Physics 2135 Exam adapted from (nz118.jpg) That reminds me… must pick up test prep HW Exam?
Announcements: Physics department has arranged for Physics 121 tutoring by Natasha Parikh on Thursdays from 12:00 Noon to 4:00 PM in the Physics Conference.
Physics 2135 Exam adapted from (nz118.jpg) That reminds me… must pick up test prep HW Exam?
Tue. Feb. 3 – Physics Lecture #26 Gauss’s Law II: Gauss’s Law, Symmetry, and Conductors 1. Electric Field Vectors and Electric Field Lines 2. Electric.
 We learned about charge and got a conceptual feel for what it is.  We identified charge with the fundamental building clocks of atoms.  We studies.
Chapter 23 Electric Potential & Electric Potential Energy.
Example: calculate the electric field for 0
24.2 Gauss’s Law.
Exam 1 Exam 1 is on Tuesday, February 14, from 5:00-6:00 PM.
Physics 2102 Lecture 10r: WED04FEB
Exam 1: Tuesday, Feb 14, 5:00-6:00 PM
Final Exam and End Material Test
Electric potential of a charge distribution. Equipotentials.
Conductors and Gauss’s Law
Exam 1: Tuesday, Feb 14, 5:00-6:00 PM
Cultural enlightenment time. Conductors in electrostatic equilibrium.
θ dθ Q R Clicker Question
Physics 212 Lecture 4 Gauss’ Law.
Exam 2: Tuesday, March 21, 5:00-6:00 PM
Exam 2: Tuesday, March 21, 5:00-6:00 PM
Final Exam and End Material Test
Exam 3: Tuesday, April 18, 5:00-6:00 PM
Exam 2: Tuesday, March 21, 5:00-6:00 PM
Exam 2: Tuesday, March 21, 5:00-6:00 PM
Exam 3: Tuesday, April 18, 5:00-6:00 PM
Physics 2113 Jonathan Dowling Physics 2113 Lecture 13 EXAM I: REVIEW.
Lecture 5 : Conductors and Dipoles
Copyright © 2014 John Wiley & Sons, Inc. All rights reserved.
Flux Capacitor (Operational)
TOPIC 3 Gauss’s Law.
Final Exam and End Material Test
That reminds me… must download the test prep HW.
Exam 1: Tuesday, Sept 19, 5:00-6:00 PM
A ring with radius R has a uniform charge density 
Exam 2: Tuesday, Oct 17, 5:00-6:00 PM
Flux Capacitor (Schematic)
An insulating spherical shell has an inner radius b and outer radius c
E. not enough information given to decide Gaussian surface #1
C. less, but not zero. D. zero.
Electricity and Magnetism
Exam 2: Tuesday, March 21, 5:00-6:00 PM
1/2/2019.
Exam 3: Tuesday, Nov 14, 5:00-6:00 PM
That reminds me… must download the test prep HW.
Question for the day Can the magnitude of the electric charge be calculated from the strength of the electric field it creates?
Announcements Final exam day events (Friday, May 12, 10:00am to 12:00pm) 50-point multiple choice end-material test (covering material from chapters 33-36).
A rod is bent into an eighth of a circle of radius a, as shown
Three charges +Q, +Q, and –Q, are located at the corners of an equilateral triangle with sides of length a. What is the force on the charge located at.
Quiz 1 (lecture 4) Ea
Wednesday (Day 4).
Electricity and Magnetism
Exam 3: Tuesday, Nov 14, 5:00-6:00 PM
Exam 3: Tuesday, April 18, 5:00-6:00 PM
Exam 1: Tuesday, Feb 14, 5:00-6:00 PM
Gauss’s law This lecture was given mostly on the board so these slides are only a guide to what was done.
Electricity and Magnetism
PHYS 1444 – Section 02 Lecture #7
Presentation transcript:

That reminds me… must download the test prep HW. Physics 2135 Exam adapted from http://www.nearingzero.net (nz118.jpg)

Exam 1: Tuesday, Feb 14, 5:00-6:00 PM Test rooms: Instructor Sections Room Dr. Hale F, H 104 Physics Dr. Kurter B, N 125 BCH Dr. Madison K, M 199 Toomey Dr. Parris J, L St Pat’s Ballroom* Mr. Upshaw A, C, E, G G-3 Schrenk Dr. Waddill D 120 BCH Special Accommodations Testing Center *exam 1 only If at 5:00 on test day you are lost, go to 104 Physics and check the exam room schedule, then go to the appropriate room and take the exam there.

Exam Reminders 5 multiple choice questions, 4 worked problems bring a calculator (any calculator that does not communicate with the outside world is OK) no external communications, any use of a cell phone, tablet, smartwatch etc. will be considered cheating no headphones be on time, you will not be admitted after 5:15pm

Exam Reminders grade spreadsheets will be posted the day after the exam you will need your PIN to find your grade (PINs were emailed by the recitation instructors) test preparation homework 1 is posted on course website, will be discussed in recitation tomorrow problems on the test preparation home work are NOT guaranteed to cover all topics on the exam!!! LEAD review session Monday from 7 to 9 pm in BCH 120

Exam 1 topics Electric charge and electric force, Coulomb’s Law Electric field (calculating electric fields, motion of a charged particle in an electric field, dipoles) Gauss’ Law (electric flux, calculating electric fields via Gaussian surfaces, fields and surface charges of conductors) Electric potential and potential energy (calculating work, potential energy and potential, calculating fields from potentials, equipotentials, potentials of conductors) Capacitors (calculating capacitance, equivalent capacitance of capacitor network, charges and voltages in capacitor network)

Exam 1 topics don’t forget the Physics 1135 concepts look at old tests (2014 to 2016 tests are on course website) exam problems may come from topics not covered in test preparation homework or test review lecture

Three charges +Q, +Q, and –Q, are located at the corners of an equilateral triangle with sides of length a. What is the force on the charge located at point P (see diagram)? y F1 P  +Q  F2 a =60 +Q -Q x Note: if there is not a problem like this on Exam 1, there will be one on the Final!

Three charges +Q, +Q, and –Q, are located at the corners of an equilateral triangle with sides of length a. What is the force on the charge located at point P (see diagram)? y F1 P  +Q  F2 a +Q -Q x I could have stated that Fy=0 and Fx=2F1x by symmetry, but I decided to do the full calculation here.

Three charges +Q, +Q, and –Q, are located at the corners of an equilateral triangle with sides of length a. What is the force on the charge located at point P (see diagram)? y F1 P  +Q  F F2 a +Q -Q x

You can “repeat” the above calculation, What is the electric field at P due to the two charges at the base of the triangle? You can “repeat” the above calculation, replacing F by E (and using Coulomb’s Law). y Or you can be smart… P a This is the charge which had been at point P, “feeling” the force . +Q -Q x Caution: never write . Why?

A rod is bent into an eighth of a circle of radius a, as shown A rod is bent into an eighth of a circle of radius a, as shown. The rod carries a total positive charge +Q uniformly distributed over its length. What is the electric field at the origin? y x a

A rod is bent into an eighth of a circle of radius a, as shown A rod is bent into an eighth of a circle of radius a, as shown. The rod carries a total positive charge +Q uniformly distributed over its length. What is the electric field at the origin? y dq   x a dE

A rod is bent into an eighth of a circle of radius a, as shown A rod is bent into an eighth of a circle of radius a, as shown. The rod carries a total positive charge +Q uniformly distributed over its length. What is the electric field at the origin? y d ds  x a dE

A rod is bent into an eighth of a circle of radius a, as shown A rod is bent into an eighth of a circle of radius a, as shown. The rod carries a total positive charge +Q uniformly distributed over its length. What is the electric field at the origin? y dq   x a dE

A rod is bent into an eighth of a circle of radius a, as shown A rod is bent into an eighth of a circle of radius a, as shown. The rod carries a total positive charge +Q uniformly distributed over its length. What is the electric field at the origin?

A rod is bent into an eighth of a circle of radius a, as shown A rod is bent into an eighth of a circle of radius a, as shown. The rod carries a total positive charge +Q uniformly distributed over its length. What is the electric field at the origin?

A rod is bent into an eighth of a circle of radius a, as shown A rod is bent into an eighth of a circle of radius a, as shown. The rod carries a total positive charge +Q uniformly distributed over its length. What is the electric field at the origin? You should provide reasonably simplified answers on exams, but remember, each algebra step is a chance to make a mistake.

What would be different if the charge were negative? What would you do differently if you were asked to calculate the potential rather than the electric field? How would you find the force on a test charge -q at the origin?

An insulating spherical shell has an inner radius b and outer radius c An insulating spherical shell has an inner radius b and outer radius c. The shell has a uniformly distributed total charge +Q. Concentric with the shell is a solid conducting sphere of total charge +2Q and radius a<b. Find the magnitude of the electric field for r<a. Use first and last slide for in-person lecture; delete for video lecture This looks like a test preparation homework problem, but it is different!

For 0<r<a, we are inside the conductor, so E=0. b a An insulating spherical shell has an inner radius b and outer radius c. The shell has a uniformly distributed total charge +Q. Concentric with the shell is a solid conducting sphere of total charge +2Q and radius a<b. Find the magnitude of the electric field for r<a. +Q For 0<r<a, we are inside the conductor, so E=0. b a c If E=0 there is no need to specify a direction (and the problem doesn’t ask for one anyway). +2Q

An insulating spherical shell has an inner radius b and outer radius c An insulating spherical shell has an inner radius b and outer radius c. The shell has a uniformly distributed total charge +Q. Concentric with the shell is a solid conducting sphere of total charge +2Q and radius a<b. Use Gauss’ Law to find the magnitude of the electric field for a<r<b. +Q b a r c +2Q Be able to do this: begin with a statement of Gauss’s Law. Draw an appropriate Gaussian surface on the diagram and label its radius r. Justify the steps leading to your answer.

An insulating spherical shell has an inner radius b and outer radius c An insulating spherical shell has an inner radius b and outer radius c. The shell has a uniformly distributed total charge +Q. Concentric with the shell is a solid conducting sphere of total charge +2Q and radius a<b. Use Gauss’ Law to find the magnitude of the electric field for b<r<c. +Q b a +2Q r c

+Q b a +2Q r c The direction of is shown in the diagram. Solving for the magnitude E (do it!) is “just” math.

+Q b a +2Q r c What would be different if we had concentric cylinders instead of concentric spheres? What would be different if the outer shell were a conductor instead of an insulator?

An insulating spherical shell has an inner radius b and outer radius c An insulating spherical shell has an inner radius b and outer radius c. The shell has a uniformly distributed total charge +Q. Concentric with the shell is a solid conducting sphere of total charge +2Q and radius a<b. Find the magnitude of the electric field for b<r<c. What would be different if we had concentric cylinders instead of concentric spheres? What would be different if the outer shell were a conductor instead of an insulator?

A ring with radius R has a uniform positive charge density  A ring with radius R has a uniform positive charge density . Calculate the potential difference between the point at the center of the ring and a point on the axis of the ring that is a distance of 3R from the center of the ring. R 3R Begin by deriving the equation for the potential along the central axis of a ring of charge. We did this back in part 2 of lecture 6. I am going to be lazy… err, efficient… and just copy the appropriate slides.

Every dq of charge on the ring is the same distance from the point P. x x Q

dq r R P x x Q

A ring with radius R has a uniform positive charge density  A ring with radius R has a uniform positive charge density . Calculate the potential difference between the point at the center of the ring and a point on the axis of the ring that is a distance of 3R from the center of the ring. R x 3R

A ring with radius R has a uniform positive charge density  A ring with radius R has a uniform positive charge density . Calculate the potential difference between the point at the center of the ring and a point on the axis of the ring that is a distance of 3R from the center of the ring. R x 3R

If a proton is released from rest at the center of the ring, how fast will it be at point P?

For the capacitor system shown, C1=6.0 F, C2=2.0 F, and C3=10.0 F. (a) Find the equivalent capacitance. C1=6F V0 C2=2F C3=10F

Don’t expect the equivalent capacitance to always be an integer! For the capacitor system shown, C1=6.0 F, C2=2.0 F, and C3=10.0 F. (a) Find the equivalent capacitance. C1=6F C23=12F V0 Don’t expect the equivalent capacitance to always be an integer!

There are several correct ways to solve this. Shown here is just one. For the capacitor system shown, C1=6.0 F, C2=2.0 F, and C3=10.0 F. (b) The charge on capacitor C3 is found to be 30.0 C. Find V0. C1=6F There are several correct ways to solve this. Shown here is just one. C2=2F C3=10F V0 C3=10F Q3= 30C V3= ?

For the capacitor system shown, C1=6.0 F, C2=2.0 F, and C3=10.0 F. (b) The charge on capacitor C3 is found to be 30.0 C. Find V0. C1=6F C23=12F Q23= ? V23= 3V V0