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If the vector electris potential for an antenna is Fm4,F,-, find E=E,, TFF and H-H in...
Only 4.10 (b) using the vector potential approach... Thank you! 14.9. An infinitesimal magnetic dipole of constant current ,,, and length I is symmetrically placed about the origin along the z-axis. Find the (a) spherical E- and H-field components radiated by the dipole in all space (b) directivity of the antenna 10. For the infinitesimal magnetic dipole of Problem 4.9, find the far-zone fields when the element is placed along the (b) y-axis
Using the vector potential A and the procedure outlined in Section 3.6 of Chapter 3, derive the far-zone spherical electric and magnetic field components of a horizontal infinitesimal dipole placed at the origin of the coordinate system of Figure 4.1 Solution: Using (4-4), but for a horizontal infinitesimal dipole of uniform current directed along the y-axis, the corresponding vector potential can be written as uloleikr A = â 4πη with the corresponding spherical components, using the rectangular to spherical components...
1) A Hertzian dipole antenna is a short conducting wire carrying an approximately constant current over its length If such a dipole is placed along the z-axis with its midpoint at the origin, and if the current flowing through it is i(t) ż lo cosot, assume I to be sufficiently small so that the observation point is approximately equidistant to all points on the dipole; that is, assume RR then the corresponding magnetic field is described by: olk2 sin e...
RBH 11.28] Problem 5: A vector force field F is defined in Cartesian Coordinates by y's F Fo 'xy2 + a3 e*y/a2 j+ey/ak a Use Stokes' Theorem to calculate: F.dr L where L is the perimeter of the rectangle ABCD given by A = (0,1, 0), B = (1,1,0), C = (1,3, 0) and D = (0,3,0) RBH 11.28] Problem 5: A vector force field F is defined in Cartesian Coordinates by y's F Fo 'xy2 + a3 e*y/a2 j+ey/ak...
1. Find the divergence, curl and Laplacian of the following vector fields (a) E = psin o Ô-p?Ộ - zk, where p, 0, z are cylindrical coordinates. (b) F = sin O † – rsin e ôn, where r, 0, $ are spherical coordinates.
e) Find the electric Field vector at point (0, +a) (Calculate the magnitude, and draw the vector.) f Sketch the electric field lines. g) Find the electric Field at (x, 0) for「a. h) Find out the location (x, y) where the electric Field E becomes zero. (Hint: Use the solution of e).) +4Q -Q
e) Find the electric Field vector at point (0, +a) (Calculate the magnitude, and draw the vector.) f Sketch the electric field lines. g) Find the electric Field at (x, 0) for「a. h) Find out the location (x, y) where the electric Field E becomes zero. (Hint: Use the solution of e).) +4Q -Q
2. Potentials and a Conducting Surface The electric potential outside of a solid spherical conductor of radius R is found to be V(r, 9) = -E, cose (--) where E, is a constant and r and 0 are the spherical radial and polar angle coordinates, respectively. This electric potential is due to the charges on the conductor and charges outside of the conductor 1. Find an expression for the electric field inside the spherical conductor. 2. Find an expression for...
2. a) Find a potential of the vector field f(x, y) = (a2 +2xy - y2, a2 - 2ry - y2) b) Show that the vector field (e" (sin ry + ycos xy) +2x - 2z, xe" cos ry2y, 1 - 2x) is conservative.
A. Make a sketch of a vector F- (x,y, z), labeling the appropriate spherical coordinates. In addition, show the unit vectors r, θ, and φ at that point B. Write the vectors ŕ.0, and ф in terms of the unit vectors x, y, and г. Here's the easy way to do this 1. For r, simply use the fact that/r 2. For φ, use the following formula sin θ Explain why the above formula works 3. Compute θ via θ...