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Transcript
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. Part A Find the force height on an object of mass in a uniform direction), like the gravitational field in the uniform gravitational field when it is at . Express in terms of , , , and . =-m*g*z_unitCorrect Because we are in a uniform field, the force does not depend on the object's location. Therefore, the variable does not appeaer in the correct answer. Part B Now find the gravitational potential energy height . Take zero potential to be at position of the object when it is at an arbitrary . Express in terms of , , and . Note that because potential energy is a scalar, and not a vector, there will be no unit vector in the answer. =m*g*zCorrect Part C In what direction does the object accelerate when released with initial velocity upward? downward Correct Electric Force and Potential Energy Now consider the analogous case of a particle with charge placed in a uniform electric field of strength Part D Find , pointing downward (in the direction) , the electric force on the charged particle at height . Express in terms of , , , and . =-q*E*z_unitCorrect Part E Now find the potential energy of this charged particle when it is at height . Take zero potential to be at position Express . (a scalar quantity) in terms of , , and . =q*E*zCorrect Part F In what direction does the charged particle accelerate when released with upward initial velocity? upward or downward depending on its charge Correct Electric Field and Electric Potential The electric potential is defined by the relationship potential energy of a particle with charge . Part G , where is the electric Find the electric potential of the uniform electric field . Note that this field is not pointing in the same direction as the field in the previous section of this problem. Take zero potential to be at position Express in terms of , . , and . =-E*zCorrect Part H The SI unit for electric potential is the volt. The volt is a derived unit, which means that it can be written in terms of other SI units. What are the dimensions of the volt in terms of the fundamental SI units? Express your answer in terms of the standard abbreviations for the fundamental SI units: (meters), (kilograms), (seconds), and volts =kg*m^2/(s^2*C)Correct (coulombs) Part I The electric field can be derived from the electric potential, just as the electrostatic force can be determined from the electric potential energy. The relationship between electric field and electric potential is , where is the gradient operator: . The partial derivative variables constant. means the derivative of Consider again the electric potential corresponding to the field potential depends on the z coordinate only, so Find an expression for the electric field with respect to , holding all other . This and in terms of the derivative of . . Express your answer as a vector in terms of the unit vectors , , and/or . Use the derivative of for with respect to . =-dV/dz * z_unitCorrect Part J A positive test charge will accelerate toward regions of ________ electric potential and ________ electric potential energy. Choose the appropriate answer combination to fill in the blanks correctly. lower; lowerCorrect Part K A negative test charge will accelerate toward regions of ________ electric potential and ________ electric potential energy. Choose the appropriate answer combination to fill in the blanks correctly. higher; lower Correct A charge in an electric field will experience a force in the direction of decreasing potential energy. Since the electric potential energy of a charge is equal to the charge times the electric potential ( ), the direction of decreasing electric potential energy is the direction of increasing electric potential. The Fate of an Electron in a Uniform Electric Field First, let us review the relationship between an electric field and its associated electric potential Part A . For now, ignore the electron located between the plates. Calculate the electric potential inside the capacitor as a function of height . Take the potential at the bottom plate to be zero. Express in terms of and . =E*hCorrect Now an electron of mass and charge (where within the electric field (see the figure) at height Part B is a positive quantity) is placed . Calculate the electon's potential energy , neglecting gravitational potential energy. Express your answer in terms of . , , and =-q_e*E*h_0Correct Part C The electron, having been held at height (i.e., , is now released from rest. Calculate its speed ) when it reaches the top plate. Express in terms of , , , , , and other given quantities and constants. =sqrt(2*q_e*E*(h_1-h_0)/m)Correct Now we consider the effect of changing either the charge or the mass of the charged particle that is released from rest at height . Part D Imagine a particle that has three times the mass of the electron. All other quantities given above remain the same. What is the ratio of the kinetic energy that this heavy particle would have when it reaches the upper plate to the kinetic energy electron would have? That is, what is 1 Correct that the ? Part E Imagine a third particle, which we will call a cyberon. It has three times the mass of an electron ( ). It has a positive charge that is three times the magnitude ( ) of the charge on an electron. What is the ratio of the speed that the cyberon would have when it reaches the upper plate after being released from rest at position to the speed that the electron would have? That is, what is ? none of the above: the cyberon will never reach the upper plateCorrect Because it has positive instead of negative charge, the cyberon will accelerate downward, toward the lower plate. Energy Stored in a Charge Configuration Part A What is , the amount of work it took to assemble this charge configuration if the point charges were initially infinitely far apart? Express your answer in terms of some or all of the variables , , and . =0Correct The hints led you through the problem by adding one charge at a time. A little thought shows that this is equivalent to simply adding the energies of all possible pairs: . Note that this is not equivalent to adding the potential energies of each charge. Adding the potential energies will give you double the correct answer because you will be counting each charge twice. Part B Which of the following figures depicts a charge configuration that requires less work to assemble than the configuration in the problem introduction? Assume that all charges have the same magnitude . figure a Correct Charged Mercury Droplets Part A Find , the ratio of , the electric potential of the initial drop, to potential of one of the smaller drops. The ratio should be dimensionless and should depend only on , the electric =n^(2/3)Correct Potential of a Finite Rod Part A What is , the electric potential at point A (see the figure), located a distance above the midpoint of the rod on the y axis? Express your answer in terms of , , , and . =k*q/L*ln((sqrt(L^2/4+d^2)+L/2)/(sqrt(L^2/4+d^2)-L/2))Correct If , this answer can be approximated as . For , . For this problem, this means that the logarithm can be further approximated as , and the expression for potential reduces to This is what we expect, because it means that from far away, the potential due to the charged rod looks like that due to a point charge. . Part B What is , the electric potential at point (on the x axis)? , located at distance from one end of the rod Give your answer in terms of , , , and . =(k*q*ln((d+L)/d))/LCorrect This result can be written as . As before, for , . Thus, for , the logarithm approaches , in which case the result reduces to . This is what we expect, because it means that from far away, the potential due to the charged rod looks like that due to a point charge.