course Phy 202 The book says that the notation, say F31 means the force on 3 by 1 assignment #003 003. Physics II 10-17-2007
......!!!!!!!!...................................
01:21:36 In your own words explain the meaning of the electric field.
......!!!!!!!!...................................
RESPONSE --> The electric field is concentration of electrical force and measures magnitude and direction of the force experienced by one charged placed at another. confidence assessment: 2
.................................................
......!!!!!!!!...................................
01:21:42 STUDENT RESPONSE AND INSTRUCTOR COMMENT: electric field is the concentration of the electrical force ** That's a pretty good way to put it. Very specifically electric field measures the magnitude and direction of the electrical force, per unit of charge, that would be experienced by a charge placed at a given point. **
......!!!!!!!!...................................
RESPONSE --> ok self critique assessment: 2
.................................................
......!!!!!!!!...................................
01:35:11 Query Principles of Physics and General Physics problem 16.15 charges 6 microC on diagonal corners, -6 microC on other diagonal corners of 1 m square; force on each. What is the magnitude and direction of the force on the positive charge at the lower left-hand corner?
......!!!!!!!!...................................
RESPONSE --> The charges are 1 meter apart and they have opposite signs which means they attract. They are both .324 N, which is found by using Coloumb's Law: F = 9x10^9 N m^2/C^2 * (6x10^-6 C) * (6x10^-6 C)/ (1m)^2 = 324 x 10^3 = .324 N. Diagonal charges have like signs and have 'sqrt(2) meters = 1.41 m between them. There is a repulsive force of .162 N which is calculated by: F=9x10^9 N m^2/C^2 * (6x10^-6 C) * (6x10^-6 C)/ (1.41m)^2 = 162 x10^-3 N = .162 N. The charge at the lower left corner experiences the force of .324 N to the right, a force of .324 N upwards and a force of .162 N at 45 dgerees downward to the left. adding 180 to this gives us an angle of 225. The components of the .162 N force are: Fy= .162 N sin(225 deg) = -.115 N and Fx= .162 N cos(225 deg) =-.115 N The total force in the x direction is -.115 N + .324 N = .21 N. In the y direction it's -.115 N + .324 N = .21N So the net force has a magnitude of 'sqrt((.21 N)^2 + (.21 N)^2) + .29 N. The angle is tan^-1 (.21 N/.21 N) = tan^-1(1) = 45 degrees. The same application goes for the negative charge at the lower right corner, so it has .324 N to the left, .324 upward, and .162 N downwards to the right. The net force by the same vector component math and is .29 N up and ove rto the left. confidence assessment: 2
.................................................
......!!!!!!!!...................................
01:35:17 ** The charges which lie 1 meter apart are unlike and therefore exert attractive forces; these forces are each .324 Newtons. This is calculated using Coulomb's Law: F = 9 * 10^9 N m^2/C^2 * ( 6 * 10^-6 C) * ( 6 * 10^-6 C) / ( 1 m)^2 = 324 * 10^-3 N = .324 N. Charges across a diagonal are like and separated by `sqrt(2) meters = 1.414 meters, approx, and exert repulsive forces of .162 Newtons. This repulsive force is calculated using Coulomb's Law: F = 9 * 10^9 N m^2/C^2 * ( 6 * 10^-6 C) * ( 6* 10^-6 C) / ( 1.414 m)^2 = 162 * 10^-3 N = .162 N. The charge at the lower left-hand corner therefore experiences a force of .324 Newtons to the right, a force of .324 Newtons straight upward and a force of .162 Newtons at 45 deg down and to the left (at angle 225 deg with respect to the standard positive x axis, which we take as directed toward the right). This latter force has components Fy = .162 N sin(225 deg) = -.115 N, approx, and Fx = .162 N cos(225 deg) = -.115 N. The total force in the x direction is therefore -.115 N + .324 N = .21 N, approx; the total force in the y direction is -.115 N + .324 N = .21 N, approx. Thus the net force has magnitude `sqrt( (.21 N)^2 + (.21 N)^2) = .29 N at an angle of tan^-1( .21 N / .21 N) = tan^-1(1) = 45 deg. The magnitude and direction of the force on the negative charge at the lower right-hand corner is obtained by a similar analysis, which would show that this charge experiences forces of .324 N to the left, .324 N straight up, and .162 N down and to the right. The net force is found by standard vector methods to be about .29 N up and to the left. **
......!!!!!!!!...................................
RESPONSE --> ok self critique assessment: 3
.................................................
......!!!!!!!!...................................
01:35:44 ** The 5 nC charge lies at distance sqrt( 4^2 + 3^2) cm from the 6 nC charge, which is 3 cm from the charge at (4 cm ,0). The force exerted on the 6 nC charge by the two respective forces have magnitudes .00011 N and .00012 N respectively. The x and y components of the force exerted by the charge at the origin are in the proportions 4/5 and 3/5 to the total charge, giving respective components .000086 N and .000065 N. The force exerted by the charge at (4 cm, 0) is in the negative y direction. So the y component of the resultant are .000065 N - .00012 N = -.000055 N and its x component is .000086 N. **
......!!!!!!!!...................................
RESPONSE --> N/A---in Phy 202 self critique assessment: 3
.................................................
......!!!!!!!!...................................
01:37:05 Query univ phy 21.76 (10th edition 22.60) quadrupole (q at (0,a), (0, -a), -2q at origin). For y > a what is the magnitude and direction of the electric field at (0, y)?
......!!!!!!!!...................................
RESPONSE --> N/A---in Phy 202 confidence assessment: 3
.................................................
......!!!!!!!!...................................
01:37:18 ** The magnitude of the field due to the charge at a point is k q / r^2. For a point at coordinate y on the y axis, for y > a, we have distances r = y-a, y+a and y. The charges at these distances are respectively q, q and -2q. So the field is k*q/(y - a)^2 + k*q/(y + a)^2 - 2k*q/y^2 = 2*k*q*(y^2 + a^2)/((y + a)^2*(y - a)^2) - 2*k*q/y^2 = 2*k*q* [(y^2 + a^2)* y^2 - (y+a)^2 ( y-a)^2) ] / ( y^2 (y + a)^2*(y - a)^2) = 2*k*q* [y^4 + a^2 y^2 - (y^2 - a^2)^2 ] / ( y^2 (y + a)^2*(y - a)^2) = 2*k*q* [y^4 + a^2 y^2 - y^4 + 2 y^2 a^2 - a^4 ] / ( y^2 (y + a)^2*(y - a)^2) = 2*k*q* [ 3 a^2 y^2 - a^4 ] / ( y^2 (y + a)^2*(y - a)^2) . For large y the denominator is close to y^6 and the a^4 in the numerator is insignifant compared to a^2 y^2 sothe expression becomes 6 k q a^2 / y^4, which is inversely proportional to y^4. **
......!!!!!!!!...................................
RESPONSE --> N/A---in Phy 202 self critique assessment: 3
.................................................
......!!!!!!!!...................................
01:37:25 query univ 22.102 annulus in yz plane inner radius R1 outer R2, charge density `sigma.What is a total electric charge on the annulus?
......!!!!!!!!...................................
RESPONSE --> N/A---in Phy 202 confidence assessment: 3
.................................................
......!!!!!!!!...................................
01:37:31 ** The total charge on the annulus is the product Q = sigma * A = sigma * (pi R2^2 - pi R1^2). To find the field at distance x along the x axis, due to the charge in the annulus, we first find the field due to a thin ring of charge: The charge in a thin ring of radius r and ring thickness `dr is the product `dQ = 2 pi r `dr * sigma of ring area and area density. From any small segment of this ring the electric field at a point of the x axis would be directed at angle arctan( r / x ) with respect to the x axis. By either formal trigonometry or similar triangles we see that the component parallel to the x axis will be in the proportion x / sqrt(x^2 + r^2) to the magnitude of the field from this small segment. By symmetry only the xcomponent of the field will remain when we sum over the entire ring. So the field due to the ring will be in the same proportion to the expression k `dQ / (x^2 + r^2). Thus the field due to this thin ring will be magnitude of field due to thin ring: k `dQ / (x^2 + r^2) * x / sqrt (x^2 + r^2) = 2 pi k r `dr * x / (x^2 + r^2)^(3/2). Summing over all such thin rings, which run from r = R1 to r = R2, we obtain the integral magnitude of field = integral ( 2 pi k r x /(x^2 + r^2)^(3/2) with respect to r, from R1 to R2). Evaluating the integral we find that magnitude of field = 2* pi k *x* | 1 /sqrt(x^2 + r1^2) - 1 / sqrt(x^2 + r2^2) | The direction of the field is along the x axis. If the point is close to the origin then x is close to 0 and x / sqrt(x^2 + r^2) is approximately equal to x / r, for any r much larger than x. This is because the derivative of x / sqrt(x^2 + r^2) with respect to x is r^2 / (x^2+r^2)^(3/2), which for x = 0 is just 1/r, having no x dependence. So at small displacement `dx from the origin the field strength will just be some constant multiple of `dx. **
......!!!!!!!!...................................
RESPONSE --> N/A---in Phy 202 self critique assessment: 3
.................................................