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Course Number: MASTERING PHYS, Spring 2009

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MasteringPhysics: Assignment Print View http://session.masteringphysics.com/myct/assignmentPrint?assig... [ Assignment View ] Elisfri 2, vor 2007 22. Gauss' Law Assignment is due at 2:00am on Wednesday, January 31, 2007 Credit for problems submitted late will decrease to 0% after the deadline has passed. The wrong answer penalty is 2% per part. Multiple choice questions are penalized as described in the online...

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Assignment MasteringPhysics: Print View http://session.masteringphysics.com/myct/assignmentPrint?assig... [ Assignment View ] Elisfri 2, vor 2007 22. Gauss' Law Assignment is due at 2:00am on Wednesday, January 31, 2007 Credit for problems submitted late will decrease to 0% after the deadline has passed. The wrong answer penalty is 2% per part. Multiple choice questions are penalized as described in the online help. The unopened hint bonus is 2% per part. You are allowed 4 attempts per answer. [ Gauss' Law Gauss's Law Learning Goal: To understand the meaning of the variables in Gauss's law, and the conditions under which the law is applicable. Gauss's law is usually written where Part A is the permittivity of vacuum. How should the integral in Gauss's law be evaluated? ANSWER: Answer n ot d isplayed Part B Part n ot d isplayed Gauss's Law in 3, 2, and 1 Dimension Gauss's law relates the electric flux through a closed surface to the total charge . You can use Gauss's law to determine the charge enclosed inside a closed surface on which the electric field is known. However, Gauss's law is most frequently used to determine the electric field from a symmetric charge distribution. The simplest case in which Gauss's law can be used to determine the electric field is that in which the charge is localized at a point, a line, or a plane. When the charge is localized at a point, so that the electric field radiates in three-dimensional space, the Gaussian surface is a sphere, and computations can be done in spherical coordinates. Now consider extending all elements of the problem (charge, Gaussian surface, boundary conditions) infinitely along some direction, say along the z axis. In this case, the point has been extended to a line, namely, the z axis, and the resulting electric field has cylindrical symmetry. Consequently, the problem reduces to two dimensions, since the field varies only with x and y, or with and in cylindrical coordinates. A one-dimensional problem may be achieved by extending the problem uniformly in two directions. In this case, the point is extended to a plane, and consequently, it has planar symmetry. Three d imensions Consider a point charge in three-dimensional space. Symmetry requires the electric field to point directly away from the charge in all directions. To find , the magnitude of the field at distance from the charge, the logical enclosed by the surface: 1 of 13 17/4/07 14:59 MasteringPhysics: Assignment Print View http://session.masteringphysics.com/myct/assignmentPrint?assig... Gaussian surface is a sphere centered at the charge. The electric field is normal to this surface, so the dot product of the electric field and an infinitesimal surface element involves . The flux integral is therefore reduced to , where is the magnitude of the electric field on the Gaussian surface, and is the area of the surface. Part A Determine the magnitude by applying Gauss's law. Part A .1 Find the area of the surface Part n ot d isplayed Express ANSWER: in terms of some or all of the variables/constants , , and . = T wo d imensions Now consider the case that the charge has been extended along the z axis. This is generally called a line charge. The usual variable for a line charge density (charge per unit length) is , and it has units (in the SI system) of coulombs per meter. Part B By symmetry, the electric field must point radially outward from the wire at each point; that is, the field lines lie in planes perpendicular to the wire. In solving for the magnitude of the radial electric field produced by a line charge with charge density , one should use a cylindrical Gaussian surface whose axis is the line charge. The length of the cylindrical surface should cancel out of the expression for . Apply Gauss's law to this situation to find an expression for . P art B .1 Find the surface area of a Gaussian cylinder Part n ot d isplayed Part B .2 Find the enclosed charge Part n ot d isplayed Express in terms of some or all of the variables , , and any needed constants. 2 of 13 17/4/07 14:59 MasteringPhysics: Assignment Print View http://session.masteringphysics.com/myct/assignmentPrint?assig... ANSWER: O ne d imension = Now consider the case with one effective direction. In order to make a problem effectively one-dimensional, it is necessary to extend a charge to infinity along two orthogonal axes, conventionally taken to be x and y. When the charge is extended to infinity in the xy plane (so that by symmetry, the electric field will be directed in the z direction and depend only on z), the charge distribution is sometimes called a sheet charge. The symbol usually used for two-dimensional charge density is either , or . In this problem we will use . has units of coulombs per meter squared. Part C In solving for the magnitude of the electric field produced by a sheet charge with charge density , use the planar symmetry since the charge distribution doesn't change if you slide it in any direction of xy plane parallel to the sheet. Therefore at each point, the electric field is perpendicular to the sheet and must have the same magnitude at any given distance on either side of the sheet. To take advantage of these symmetry properties, use a Gaussian surface in the shape of a cylinder with its axis perpendicular to the sheet of charge, with ends of area which will cancel out of the expression for in the end. The result of applying Gauss's law to this situation then gives an expression for for both and . P art C .1 Find the total electric flux out of the cylinder Part n ot d isplayed Part C .2 Find the charge within the Gaussian surface Part n ot d isplayed Express ANSWER: for = in terms of some or all of the variables/constants , , and . In this problem, the electric field from a distribution of charge in 3, 2, and 1 dimension has been found using Gauss's law. The most noteworthy feature of the three solutions is that in each case, there is a different relation of the field strength to the distance from the source of charge. In each case, the field strength varies inversely as an integral power of the distance from the charge. In the case of a point charge (spherical symmetry, field in three dimensions), the field strength varies as . In the case of a line charge (cylindrical symmetry, field in two dimensions), the field strength varies as . Finally, in the case of a sheet charge (planar symmetry, field in one dimension), the field varies as ; that is, the strength of the field is independent of the distance from the sheet! If you visualize the electric field using field lines, this result shows that as the number of directions in which the electric field can point is reduced, the field lines have one dimension fewer in which to to spread out, and the field therefore falls off less rapidly with distance. In a one-dimensional problem (sheet charge), the extension of the charge in the xy plane means that all field lines are parallel to the z axis, and so the field strength does not change with distance. Such a situation, of course, is impossible in the real world: In reality, 3 of 13 17/4/07 14:59 MasteringPhysics: Assignment Print View http://session.masteringphysics.com/myct/assignmentPrint?assig... the planar charge is not infinite, so the field will in fact fall off over long distances. The Electric Field and Surface Charge at a Conductor Learning Goal: To understand the behavior of the electric field at the surface of a conductor, and its relationship to surface charge on the conductor. A conductor is placed in an external electrostatic field. The external field is uniform before the conductor is placed within it. The conductor is completely isolated from any source of current or charge. Part A Which of the following describes the electric field inside this conductor? ANSWER: It is in the same direction as the original external field. It is in the opposite direction from that of the original external field. It has a direction determined entirely by the charge on its surface. It is always zero. The net electric field inside a conductor is always zero. If the net electric field were not zero, a current would flow inside the conductor. This would build up charge on the exterior of the conductor. This charge would oppose the field, ultimately (in a few nanoseconds for a metal) canceling the field to zero. Part B The charge density inside the conductor is: ANSWER: 0 non-zero; but uniform non-zero; non-uniform infinite You already know that there is a zero net electric field inside a conductor; therefore, if you surround any internal point with a Gaussian surface, there will be no flux at any point on this surface, and hence the surface will enclose zero net charge. This surface can be imagined around any point inside the conductor with the same result, so the charge density must be zero everywhere inside the conductor. This argument breaks down at the surface of the conductor, because in that case, part of the Gaussian surface must lie outside the conducting object, where there is an electric field. Part C Assume that at some point just outside the surface of the conductor, the electric field has magnitude and is directed toward the surface of the conductor. What is the charge density on the surface of the conductor at that point? Part C .1 How to approach the problem Which of the following is the best way to solve this problem? ANSWER: Answer n ot d isplayed Part C .2 Calculate the flux through the top of the cylinder Part n ot d isplayed Part C .3 Calculate the flux through the bottom of the box Part n ot d isplayed Part C .4 What is the charge inside the Gaussian surface? 4 of 13 17/4/07 14:59 MasteringPhysics: Assignment Print View http://session.masteringphysics.com/myct/assignmentPrint?assig... Part n ot d isplayed Hint C .5 Apply G auss's l aw Hint n ot d isplayed Express your answer in terms of ANSWER: = and . The Electric Field inside and outside a Charged Insulator A slab of insulating material of uniform thickness , lying between to along the x axis, extends infinitely in the y and z directions, as shown in the figure. The slab has a uniform charge density . The electric field is zero in the middle of the slab, at . Part A Which of the following statements is true of the electric field ANSWER: Answer n ot d isplayed Part B Part n ot d isplayed Part C Part n ot d isplayed Part D Part n ot d isplayed Concept and Exercises on Electric Flux at the surface of one side of the slab? Calculating Electric Flux through a Disk Suppose a disk with area is placed in a uniform electric field of magnitude . The disk is oriented so that the vector normal to its surface, , makes an angle with the electric field, as shown in the figure. Part A 5 of 13 17/4/07 14:59 MasteringPhysics: Assignment Print View http://session.masteringphysics.com/myct/assignmentPrint?assig... Calculating Flux for Hemispheres of Different Radii Learning Goal: To understand the definition of electric flux, and how to calculate it. Flux is the amount of a vector field that "flows" through a surface. We now discuss the electric flux through a surface (a quantity needed in Gauss's law): , where is the flux through a surface with differential area element , and is the electric field in which the surface lies. There are several important points to consider in this expression: 1. It is an integral over a surface, involving the electric field at the surface. 2. is a vector with magnitude equal to the area of an infinitesmal surface element and pointing in a direction normal (and usually outward) to the infinitesmal surface element. 3. The scalar (dot) product implies that only the component of integral. That is, , where is the angle between normal to the surface contributes to the and . When you compute flux, try to pick a surface that is either parallel or perpendicular to , so that the dot product is easy to compute. Two hemispherical surfaces, 1 and 2, of respective radii and , are centered at a point charge and are facing each other so that their edges define an annular ring (surface 3), as shown. The field at position due the to point charge is: where is a constant proportional to the charge, vector in the radial direction. Part A What is the electric flux , and is the unit through the annular ring, surface 3? Hint A .1 Apply t he d efinition o f e lectric f lux Hint n ot d isplayed Express your answer in terms of ANSWER: Part B What is the electric flux through surface 1? , , , a nd a ny c onstants. = Answer n ot d isplayed Hint B .1 Apply t he d efinition o f e lectric f lux Hint n ot d isplayed Part B .2 Find the area of surface 1 Part n ot d isplayed Express ANSWER: Part C in terms of , , , and any needed constants. = Answer n ot d isplayed 6 of 13 17/4/07 14:59 MasteringPhysics: Assignment Print View http://session.masteringphysics.com/myct/assignmentPrint?assig... What is the electric flux passing outward through surface 2? Hint C .1 Apply t he d efinition o f e lectric f lux Hint n ot d isplayed Part C .2 Find the area of surface 2 Part n ot d isplayed Express ANSWER: in terms of , , , and any constants or other known quantities. = Answer n ot d isplayed Flux through a Cube A cube has one corner at the origin and the opposite corner at the point . The sides of the cube are parallel to the coordinate planes. The electric field in and around the cube is given by . Part A Find the total electric flux through the surface of the cube. Hint A .1 Definition o f f lux Hint n ot d isplayed Part A .2 Flux through the face Part n ot d isplayed Part A .3 Flux through the face Part n ot d isplayed Part A .4 Flux through the face Part n ot d isplayed Part A .5 Flux through the face Part n ot d isplayed Hint A .6 Putting i t t ogether Hint n ot d isplayed Express your answer in terms of , , , and . ANSWER: Part B Part n ot d isplayed Part C = Answer n ot d isplayed 7 of 13 17/4/07 14:59 MasteringPhysics: Assignment Print View http://session.masteringphysics.com/myct/assignmentPrint?assig... What is the net charge inside the cube? Hint C .1 Gauss's l aw Hint n ot d isplayed Express your answer in terms of , , , ANSWER: = Answer n ot d isplayed , and . The Charge Inside a Conductor A spherical cavity is hollowed out of the interior of a neutral conducting sphere. At the center of the cavity is a point charge, of positive charge . Part A What is the total surface charge on the interior surface of the conductor (i.e., on the wall of the cavity)? Hint n ot d isplayed ANSWER: Part B What is the total surface charge on the exterior surface of the conductor? Hint n ot d isplayed ANSWER: = Hint B .1 Properties o f t he c onductor = Hint A .1 Gauss's law and properties of conductors Part C What is the magnitude of the electric field inside the cavity as a function of the distance from the point charge? Let , as usual, denote . Hint C .1 How to approach the problem The net electric field inside the conductor has three contributions: 1. from the charge ; 2. from the charge on the cavity's walls ; 3. from the charge on the outer surface of the spherical conductor . and be distributed for this to However, the net electric field inside the conductor must be zero. How must happen? Here's a clue: the first two contributions above cancel each other out, outside the cavity. Then the electric field produced by inside the spherical conductor must separately be zero also. How must be distributed for this to happen? 8 of 13 17/4/07 14:59 MasteringPhysics: Assignment Print View http://session.masteringphysics.com/myct/assignmentPrint?assig... After you have figured out how and are distributed, it will be easy to find the field in the cavity, either by adding field contributions from all charges, or using Gauss's Law. Part C .2 Charge d istributions a nd f inding t he e lectric f ield and are both uniformly distributed. Unfortunately there is no easy way to determine this, that is why a clue was given in the last hint. You might hit upon it by assuming the simplest possible distribution (i.e., uniform) or by trial and error, and check that it works (gives no net electric field inside the conductor). If is distributed uniformly over the surface of the conducting sphere, it will not produce a net electric field inside the sphere. What are the characteristics of the field produces inside the cavity? ANSWER: zero the same as the field produced by a point charge located at the center of the sphere the same as the field produced by a point charge located at the position of the charge in the cavity ANSWER: Part D 0 What is the electric field outside the conductor? Hint D .1 How to approach the problem The net electric field inside the conductor has three contributions: 1. from the charge ; 2. from the charge on the cavity's walls ; 3. from the charge on the outer surface of the spherical conductor . and be distributed for this to However, the net electric field inside the conductor must be zero. How must happen? Here's a helpful clue: the first two contributions above cancel each other out, outside the cavity. Then the electric field produced by inside the spherical conductor must be separately be zero also. How must be distributed for this to happen? What sort of field would such a distribution produce outside the conductor? Hint D .2 The d istribution o f If is distributed uniformly over the surface of the conducting sphere, it will not produce a net electric field inside the sphere. What are the characteristics of the field it produces outside the sphere? ANSWER: zero the same as the field produced by a point charge located at the center of the sphere the same as the field produced by a point charge located at the position of the charge in the cavity Now a second charge, , is brought near the outside of the conductor. Which of the following quantities would change? Part E The total surface charge on the wall of the cavity, : Hint E .1 Canceling the field due to the charge The net electric field inside a conductor is always zero. The charges on the inner conductor cavity will always arrange themselves so that the field lines due to charge do not penetrate into the conductor. 9 of 13 17/4/07 14:59 MasteringPhysics: Assignment Print View http://session.masteringphysics.com/myct/assignmentPrint?assig... ANSWER: Part F would change would not change The total surface charge on the exterior of the conductor, Hint F .1 Canceling the field due to the charge : The net electric field inside a conductor is always zero. The charges on the outer surface of the conductor will rearrange themselves to shield the external field completely. Does this require the net charge on the outer surface to change? ANSWER: Part G The electric field within the cavity, ANSWER: Part H The electric field outside the conductor, ANSWER: : : would change would not change would change would not change would change would not change Finding E-Fields Using Gauss' law The Electric Field of a Ball of Uniform Charge Density A solid ball of radius Part A What is the magnitude of the electric field Hint A .1 Gauss's l aw Hint n ot d isplayed Part A .2 Find P art n ot d isplayed Express your answer in terms of , ANSWER: Part B What is the magnitude of the electric field at a distance from the center of the ball? , , and . at a distance from the center of the ball? has a uniform charge density . = Answer n ot d isplayed Part B .1 How does this situation compare to that of the field outside the ball? Part n ot d isplayed Express your answer in terms of , , ANSWER: Part C , and . = Answer n ot d isplayed 10 of 13 17/4/07 14:59 MasteringPhysics: Assignment Print View http://session.masteringphysics.com/myct/assignmentPrint?assig... Let represent the electric field due to the charged ball throughout all of space. Which of the following statements about the electric field are true? 1. . 2. . 3. . 4. The maximum electric field occurs when 5. The maximum electric field occurs when 6 . The maximum electric field occurs as Hint C .1 Plot t he e lectric f ield Hint n ot d isplayed Enter t (true) or f (false) for each statement. Separate your answers with commas. ANSWER: Answer n ot d isplayed . . A Conducting Shell around a Conducting Rod An infinitely long conducting cylindrical rod with a positive charge per unit length is surrounded by a conducting cylindrical shell (which is also infinitely long) with a charge per unit length of and radius , as shown in the figure. Part A What is , the radial component of the electric field between the rod and cylindrical shell as a function of the distance from the axis of the cylindrical rod? Hint A .1 The i mplications o f s ymmetry Because the cylinder and rod are cylindrically symmetric, the magnitude of the electric field cannot vary as a function of angle around the rod, nor as a function of longitudinal position along the rod (typically represented by the spatial variables and ). By symmetry, the magnitude of the electric field can only depend on the distance from the axis of the rod (the spatial variable ). Hint A .2 Apply G auss' l aw Gauss's law states that , where is the electric flux through a Gaussian surface, and is the total charge coaxial with the rod, enclosed by the surface. Construct a cylindrical Gaussian surface with radius and length with . 11 of 13 17/4/07 14:59 MasteringPhysics: Assignment Print View http://session.masteringphysics.com/myct/assignmentPrint?assig... Part B What is , the surface charge density (charge per unit area) on the inner surface of the conducting shell? Part B .1 Apply G auss's l aw The magnitude of the net force on charges within a conductor is always zero. This implies that the magnitude of the electric field within the conductor is zero. Think about a cylindrical Gaussian surface of length whose radius lies at the middle of the outer cylindrical shell. Since the electric field inside a conductor is zero and the Gaussian surface lies within the conductor, the electric flux across the Gaussian surface must be zero. What, then, must , the total charge inside this Gaussian surface, be? ANSWER: =0 P art B .2 Find the charge contribution from the surface What is surface? , the total charge on the inner surface of the cylindrical shell that is contained within the Gaussian and . Express your answer in terms of ANSWER: = To obtain the charge density per unit area, divide that is contained within the Gaussian surface. ANSWER: Part C = by the area of the inner surface of the conducting shell What is , the surface charge density on the outside of the conducting shell? (Recall from the problem statement that the conducting shell has a total charge per unit length given by .) Part C .1 What is the charge on the cylindrical shell? What is , the total surface charge (the sum of charges on the inner and outer surfaces) of a portion of the shell of length ? ANSWER: = Since the charge on the inner surface of the cylinder is and the total charge on the cylinder is , it is now easy to obtain the charge on the outer surface of the cylinder. Then divide this result by the surface area of the portion of the cylinder that you took to obtain your result. ANSWER: Part D What is the radial component of the electric field, Hint D .1 How to approach the problem Hint n ot d isplayed Part D .2 Find the charge within the Gaussian surface Part n ot d isplayed Part D .3 Find the flux in terms of the electric field Part n ot d isplayed , outside the shell? = 12 of 13 17/4/07 14:59 MasteringPhysics: Assignment Print View http://session.masteringphysics.com/myct/assignmentPrint?assig... ANSWER: = A Charged Sphere with a Cavity An insulating sphere of radius , centered at the origin, has a uniform volume charge density . Part A Find the electric field inside the sphere (for < ) in terms of the position vector . Hint A .1 How to approach the problem Hint n ot d isplayed Part A .2 Determine t he e nclosed c harge Part n ot d isplayed Part A .3 Calculate the integral over the Gaussian surface Part n ot d isplayed Express your answer in terms of ANSWER: Part B Part n ot d isplayed , , and . = Answer n ot d isplayed Summary 4 of 11 problems complete (35.13% avg. score) 19.32 of 20 points 13 of 13 17/4/07 14:59

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Kettering - MASTERING - PHYS
MasteringPhysics: Assignment Print Viewhttp:/session.masteringphysics.com/myct/assignmentPrint?assig.[ Assignment View ]Elisfri 2, vor 200723a. Electric PotentialAssignment is due at 2:00am on Wednesday, January 31, 2007Credit for problems submitted
Kettering - MASTERING - PHYS
MasteringPhysics: Assignment Print Viewhttp:/session.masteringphysics.com/myct/assignmentPrint?assig.[ Assignment View ]Elisfri 2, vor 200723b. Electric PotentialAssignment is due at 2:00am on Wednesday, February 7, 2007Credit for problems submitted
Kettering - MASTERING - PHYS
MasteringPhysics: Assignment Print Viewhttp:/session.masteringphysics.com/myct/assignmentPrint?assig.[ Assignment View ]Elisfri 2, vor 200724. Capacitance and DielectricsAssignment is due at 2:00am on Wednesday, February 7, 2007Credit for problems s
Kettering - MASTERING - PHYS
MasteringPhysics: Assignment Print Viewhttp:/session.masteringphysics.com/myct/assignmentPrint?assig.[ Assignment View ]Elisfri 2, vor 200725. Current, Resistance, and Electromagnetic ForceAssignment is due at 2:00am on Wednesday, February 14, 2007C
Kettering - MASTERING - PHYS
MasteringPhysics: Assignment Print Viewhttp:/session.masteringphysics.com/myct/assignmentPrint?assig.[ Assignment View ]Elisfri 2, vor 200726. DC CircuitsAssignment is due at 2:00am on Wednesday, February 21, 2007Credit for problems submitted late w
Kettering - MASTERING - PHYS
MasteringPhysics: Assignment Print Viewhttp:/session.masteringphysics.com/myct/assignmentPrint?assig.[ Assignment View ]Elisfri 2, vor 200727. Magnetic Field and Magnetic ForcesAssignment is due at 2:00am on Wednesday, February 28, 2007Credit for pr
Kettering - MASTERING - PHYS
MasteringPhysics: Assignment Print View04/19/2007 02:22 PM[ Assignment View ][ PriElisfri 2, vor 200728. Sources of Magnetic FieldAssignment is due at 2:00am on Wednesday, March 7, 2007Credit for problems submitted late will decrease to 0% after th
Kettering - MASTERING - PHYS
MasteringPhysics: Assignment Print View04/19/2007 02:22 PM[ Assignment View ][ PriElisfri 2, vor 200729a. Electromagnetic InductionAssignment is due at 2:00am on Wednesday, March 7, 2007Credit for problems submitted late will decrease to 0% after t
Kettering - MASTERING - PHYS
http:/session.masteringphysics.com/myct04/19/2007 05:02 PM[ Assignment View ][ Print ]Elisfri 2, vor 200730. InductanceAssignment is due at 2:00am on Wednesday, March 14, 2007Credit for problems submitted late will decrease to 0% after the deadline
Kettering - MASTERING - PHYS
MasteringPhysics: Assignment Print View04/19/2007 05:03 PM[ Assignment View ][ PriElisfri 2, vor 200731. Alternating Current CircuitsAssignment is due at 2:00am on Wednesday, March 21, 2007Credit for problems submitted late will decrease to 0% afte
Kettering - MASTERING - PHYS
http:/session.masteringphysics.com/myct04/19/2007 05:03 PM[ Assignment View ][ Print ]Elisfri 2, vor 200732. Electromagnetic WavesAssignment is due at 2:00am on Wednesday, March 28, 2007Credit for problems submitted late will decrease to 0% after t
Kettering - MASTERING - PHYS
MasteringPhysics: Assignment Print Viewhttp:/session.masteringphysics.com/myct/assignmentPrint?assig.[ Assignment View ]Elisfri 2, vor 200733. The Nature and Propagation of LightAssignment is due at 2:00am on Wednesday, January 17, 2007Credit for pr
Kettering - MASTERING - PHYS
MasteringPhysics: Assignment Print Viewhttp:/session.masteringphysics.com/myct/assignmentPrint?assig.[ Assignment View ]Elisfri 2, vor 200734. Geometric Optics and Optical InstrumentsAssignment is due at 2:00am on Wednesday, January 17, 2007Credit f
Kettering - MASTERING - PHYS
MasteringPhysics: Assignment Print Viewhttp:/session.masteringphysics.com/myct/assignmentPrint?assig.[ Assignment View ]Elisfri 2, vor 200735. InterferenceAssignment is due at 2:00am on Wednesday, January 17, 2007Credit for problems submitted late w
Kettering - MASTERING - PHYS
MasteringPhysics: Assignment Print Viewhttp:/session.masteringphysics.com/myct/assignmentPrint?assig.[ Assignment View ]Elisfri 2, vor 200736. DiffractionAssignment is due at 2:00am on Wednesday, January 17, 2007Credit for problems submitted late wi
Kettering - MASTERING - PHYS
Chapte 24. Ele r ctric Pote ntial24.1. What is Physics? 24.2. Ele ctric Pote ntial Ene rgy 24.3. Ele ctric Pote ntial 24.4. Equipote ntial S urface s 24.5. C alculating thePote ntial fromtheFie ld 24.6. Pote ntial Dueto a Point C harge 24.7. Pote ntial D
Kettering - MASTERING - PHYS
Electric Potential Electric Potential Energy versus Electric Potential Gravitational Force and Potential Energy First we review the force and potential energy of an object of mass gravitational field that points downward (in the near the earth's surface.
Kettering - MASTERING - PHYS
PHYS-225Homework 225CFall 2009Dr. RussellPart 1: Mean and Uncertainty (6 pts) The data set at right shows a set of data points representing measurements of the electric field at a certain location.1. Enter this data into an Excel spreadsheet. 2. Calc
Kettering - MASTERING - PHYS
23.4. Model: Light rays travel in straight lines. Also, the red and green light bulbs are point sources.Visualize:Solve:The width of the aperture is w = 1 m. From the geometry of the figure for red light,w2 x = x = 2w = 2 (1.0 m ) = 2.0 m 1m 3m + 1mT
Kettering - MASTERING - PHYS
24.40. Model: Assume thin lenses and treat each as a simple magnifier with M = 25cm/f .Visualize: Equation 24.10 gives the magnification of a microscope.M = mobjM eye = L 25cm f obj f eyeSolve: (a) The more powerful lens (4) with the shorter focal len
Kettering - MASTERING - PHYS
22.2. Model: Two closely spaced slits produce a double-slit interference pattern.Visualize: The interference pattern looks like the photograph of Figure 22.3(b). It is symmetrical, with the m = 2 fringes on both sides of and equally distant from the cent
Kettering - MASTERING - PHYS
MasteringPhysics10/19/08 6:50 PMAssignment Display Mode:View Printable Answers[PPhysys 202 Fall08HW4Due at 11:00pm on Wednesday, October 8, 2008View Grading DetailsIntroduction to Electric CurrentDescription: Mostly conceptual questions about el
Kettering - MASTERING - PHYS
26.14. Model: Model the plastic spheres as point charges.Visualize:Solve:(a) The charge q1 = 50.0 nC exerts a force F1 on 2 on q2 = 50.0 nC to the right, and the charge q2 exerts9 2 2 9 9 K q1 q2 ( 9.0 10 N m /C ) ( 50.0 10 C ) ( 50.0 10 C ) = = 0.056
Kettering - MASTERING - PHYS
27.10. Model: The rod is thin, so assume the charge lies along a line. Visualize:Solve: The force on charge q is F = qErod . From Example 27.3, the electric field a distance r from the center of a charged rod isErod = Thus, the force is1Q4 0 r r 2 +
Kettering - MASTERING - PHYS
28.4. Model: The electric flux flows out of a closed surface around a region of space containing a netpositive charge and into a closed surface surrounding a net negative charge. Visualize: Please refer to Figure EX28.4. Let A be the area in m2 of each o
Kettering - MASTERING - PHYS
29.28. Model: The electric potential at the dot is the sum of the potentials due to each charge.Visualize: Please refer to Figure EX29.28. Solve: The electric potential at the dot isV=1 q1 1 q2 1 q3 + + 4 0 r1 4 0 r2 4 0 r3 5.0 109 C 5.0 109 C q = ( 9
Kettering - MASTERING - PHYS
MasteringPhysics5/10/09 3:33 PMAssignment Display Mode:View Printable Answers[ Print ]phy260S09HW9Due at 11:00pm on Thursday, April 16, 2009View Grading DetailsCharged Aluminum SpheresDescription: Find the number of electrons in an aluminum sphe
Kettering - MASTERING - PHYS
MasteringPhysics5/10/09 3:36 PMAssignment Display Mode:View Printable Answers[ Print ]phy260S09HW10Due at 11:00pm on Tuesday, April 28, 2009View Grading DetailsCharged RingDescription: Find the electric field from a uniformly charged ring (quali
Kettering - MASTERING - PHYS
MasteringPhysics5/10/09 3:39 PMAssignment Display Mode:View Printable Answers[ Print ]phy260S09HW11Due at 11:00pm on Tuesday, May 5, 2009View Grading DetailsEnergy Stored in a Charge ConfigurationDescription: Find the work required to assemble f
Kettering - MASTERING - PHYS
MasteringPhysics5/10/09 3:42 PMAssignment Display Mode:View Printable Answers[ Print ]phy260S09HW12Due at 11:00pm on Tuesday, May 12, 2009View Grading DetailsCapacitors in SeriesDescription: Contains several questions that help practice basic ca
Kettering - MASTERING - PHYS
MasteringPhysics5/10/09 3:55 PMAssignment Display Mode:View Printable Answersphy260S09HW13Due at 12:00am on Monday, June 1, 2009View Grading DetailsHeating a Water BathDescription: Calculate the time required for a resistor to heat a water bath t
Ohio State - BUSFIN - 600
MID TERM ESSAY QUESTIONS A. Variable life insurance has the premiums invested in separate accounts and the face value may increase if the investment results are favorable. Prospects are those who desire life insurance at a fixed, level premium but want to
Ohio State - BUSFIN - 600
BF 640 AUTUMN 2008 FINAL MULTIPLE CHOICE EXAM INSTRUCTOR: CHARLES A. BRYAN NAME: _ Place your answer on the answer sheet and turn the answer sheet in. You may keep the exam. Answers will be posted on Carmen within three days. 1. Risk can be defined as a.
Ohio State - BUSFIN - 600
BF 640 AUTUMN 2008 MID TERM EXAM MULTIPLE CHOICE QUESTIONS ANSWER SHEET NAME: _ Place your answer on the answer sheet and turn the answer sheet in. You may keep the exam. Answers will be posted on Carmen. 1. Risk can be defined as a. Uncertainty concernin
Indiana - MATH - 311
University of Alaska Southeast - CIS - 29977
Fall 2003 Hulstein &amp; Hulstein Intermediate Accounting Chapter # 9 Quiz B Name _1. Designated market value a. is always the middle value of replacement cost, net realizable value, and net realizable value less a normal profit margin. b. should always be e
U. Houston - ASSEMBLY - 0356
Laboratory Short CourseIntroduction to CodeWarrior Running Assembly Programs on the Microcontrollerwww.freescale.com/universityprogramsFreescale and the Freescale logo are trademarks of Freescale Semiconductor, Inc. All other product or service names a
Clarkson - ES - 220
Clarkson - ES - 220
Clarkson - ES - 220
Clarkson - ES - 220
Clarkson - ES - 220
Clarkson - ES - 220
Clarkson - ES - 220
Clarkson - ES - 220
Clarkson - ES - 220
Clarkson - ES - 220
Clarkson - ES - 220
Clarkson - ES - 220
Academy of Art University - ARTS - arts 101
Note that the following lectures include animations and PowerPoint effects such as fly ins and transitions that require you to be in PowerPoint's Slide Show mode (presentation mode).Chapter 4The Origin of Modern AstronomyGuidepostThe sun, moon, and pl
DeAnza College - ARTS - arts 101
Review question from chapter 1:3, What is the difference between our solar system, our galaxy a nd the universe? Our solar system is made up of the Sun (the nearest star), and bodies (like the planets) which are gravitationally bound to it. It is much sm
New York College of Podiatric Medicine - AUD - 5721
1Chapter 1 Introduction to Federal Taxation and Understanding the Federal Tax LawSUMMARY OF CHAPTERThis chapter presents information on the magnitude of federal taxes collected and on taxpayer obligations. Also, the history of U.S. federal taxation is
New York College of Podiatric Medicine - ACT - 3243
9Chapter 2 Tax Research, Practice, and ProcedureSUMMARY OF CHAPTERTax practice involves the preparation of tax returns and representation of clients before the audit or appellate divisions of the Internal Revenue Service. To become a competent professi
Cornell - HADM - 3301
Challenge1 Afterrunningchallenge1withandwithoutbatching,itbecameimmediatelyclearthatBenihana mustusebatchingtoproducethemostprofitableresults.Inoursimulationwithbatchingthe averageprofitwas360.00.Withoutbatchingprofitwasintheredat139.00.Fromthetableyou ca
Cornell - H ADM - 301
The only way to address the bottleneck issue is to get another oven. Kristen has two options, she can either rent an oven from her neighbor or buy another one. If she were to rent another oven, the process would change. Kristen would have to run back and
Cornell - H ADM - 3387
HADM 387 9/16/08 Sexual HarassmentThe original title VII did not include sex so you could technically exclude women from your restaurant There is very little history on sex in the title 1986 Sex.H starts under federal law. Bill passed by congress added
Lawson State - BUSINESS - Acct113
Quiz 4 (20 points) 1. Which of the following circumstances creates a future taxable amount? A. Service fees collected in advance from customers: taxable when received, recognized for f inancial reporting when earned. B. Accrued compensation costs for futu
University of Texas - M - M408K
Frameset OverviewThe Blackboard Learn environment includes a header frame with images and buttons customized by the institution and tabs that navigate to different areas within Blackboard Learn. Clicking on a tab will open that area in the content frame.
University of Texas - M - M408K
Frameset OverviewThe Blackboard Learn environment includes a header frame with images and buttons customized by the institution and tabs that navigate to different areas within Blackboard Learn. Clicking on a tab will open that area in the content frame.
University of Texas - M - M408K
amaefule (bca357) HW02 Gilbert (57195) This print-out should have 13 questions. Multiple-choice questions may continue on the next column or page nd all choices before answering. 001 10.0 points1t (seconds) 0 1 2 3 4 5 s (feet) 0 20 28 36 50 62 Find the
Minnesota - BIOLOGY - A&P
BIOL 237 Case History 1 A 27 year old man, who works outdoors, notices a growth on the skin which includes a darkly pigmented spot surrounded by a halo of inflamed skin. This man has a very fair complexion, with numerous freckles and blond hair. Because o