Electrostatics and Magnetostatics
Spatial Relationships
Learning Objectives:
- Learn about different coordinate systems, such as Cartesian coordinates and polar coordinates, and how they are used to represent spatial positions.
Types of Co-ordinate Systems:
- Rectangular or Cartesian Coordinate system: (x,y,z)
- Cylindrical coordiante system: (r, $\theta$, z)
- Spherical coordinate system (r, $\theta$, $\phi$)
Transformation:
- Cartesian into cylindrical: \begin{align*} r &= \sqrt{x^2 + y^2}\\ \theta &= \tan^{-1}\left(\dfrac{y}{x}\right)\\ z &= z \end{align*}
- Cartesian into cylindrical: \begin{align*} r &= \sqrt{x^2 + y^2 + z^2}\\ \theta &= \tan^{-1}\left(\dfrac{y}{x}\right)\\ \phi &= \cos^{-1}\left(\dfrac{z}{r}\right) \end{align*}
Andeggs, Public domain, via Wikimedia Commons
Solved Example: 9994-01
The electric field strength at distant point, P, due to a point charge, +q, located at the origin, is 100 $\mu$ V/m. If the point charge is now enclosed by a perfectly conducting metal sheet sphere whose center is at the origin, then the electric field strength at the point, P, outside the sphere, becomes:
A. Zero
B. 100 $\mu$ V/m
C. – 100 $\mu$ V/m
D. 50 $\mu$ V/m
The point charge +q will induce a charge – q on the surface of metal sheet sphere. Using Gauss’s law, the net electric fulx passing through a closed surface is equal to the charge enclosed = + q – q = 0 D = 0, E = 0 at point P.
Correct Answer: A
Solved Example: 9994-02
A metal sphere with 1 m radius and surface charge density of 10 Coulombs / m$^2$ is enclosed in a cube of 10 m side. The total outward electric displacement normal to the surface of the cube is:
A. 40 $\pi$ Coulombs
B. 10 $\pi$ Coulombs
C. 5 $\pi$ Coulombs
D. None of the above
The sphere is enclosed in a cube of side = 10m. using Gauss’s law, the net electric flux flowing out through a closed surface is equal to charge enclosed. \[\begin{aligned} \iint_s \bar(D) \cdot \bar{da} &= Q (enclosed)\\ &= P_S 4 \pi r^2\\ &= 10 \times 4 \pi\\ &= 40 \pi Coulombs\end{aligned}\]
Correct Answer: A
Solved Example: 9994-03
The thumb in Fleming's left hand rule indicate:
A. Motion
B. Current
C. Field
D. None from the above
Correct Answer: A
Solved Example: 9994-04
Electric flux is a _______ field, and its density is a _______ field.
A. Vector, vector
B. Scalar, vector
C. Vector, scalar
D. Scalar, scalar
Correct Answer: B
Solved Example: 9994-05
Find H = ___________ A/m at the center of a circular coil of diameter 1 m and carrying a current of 2 A.
A. 0.6366
B. 0.1636
C. 6.366
D. 2
Correct Answer: D
Solved Example: 9994-06
The force between two charges is 200 N. If the distance between the charges is doubled, the force will be _______.
A. 400 N
B. 100 N
C. 50 N
D. 200 N
Correct Answer: C
Vector Analysis
Stoke's Theorem:
Stoke's theorem converts line integration to surface integration and vice versa. \[\oint \bar{A}. \bar{dr} = \iint_s (\bar{\nabla} \times \bar{A}).\bar{dS}\]Divergence Theorem:
Divergence theorem converts volume integration to surface integration and vice versa. \[\iiint_V(\bar{\nabla}.\bar{A}) dV = \unicode{x222F} \bar{A}.\bar{dS}\]Maschen, CC0, via Wikimedia Commons
Solved Example: 9149-01
The divergence theorem converts:
A. Line to surface integral
B. Surface to volume integral
C. Volume to line integral
D. Surface to line integral
The divergence theorem for a function F is given by \[ \iint F. dS = \iiint Div (F). dV\] Thus it converts surface(double integral) to volume (triple integral).
Correct Answer: B
Solved Example: 9149-02
Evaluate Gauss law for D = 5r$^2$/4 in spherical coordinates with r = 4m and $\theta$ = $\dfrac{\pi}{4}$ as surface integral.
A. 600
B. 588.9
C. 577.8
D. 599.7
\[\iint D. ds =\iint \dfrac{5r^2}{4}. ds\] In spherical co-ordinates, $ds$= surface area = $r^2 \sin \theta d\theta d\phi$ \begin{align*} &= \iint \dfrac{5r^2}{4}. r^2\ \sin \theta d\theta\ d\phi\\ &= \iint \dfrac{5r^4}{4}\ \sin \theta d\theta\ d\phi \end{align*} Given r = 4 and it remains constant throughout the surface on a sphere, \begin{align*} &= \dfrac{5r^4}{4} \times \int_0^{\dfrac{\pi}{4}} \sin \theta d\theta \int_0^{2\pi} d\phi\\ &= \dfrac{5(4)^4}{4} \times \int_0^{\dfrac{\pi}{4}} \sin \theta d\theta \int_0^{2\pi} d\phi\\ &= 320 \times \left(-\cos \theta\right)_0^{\frac{\pi}{4}} [\phi]_0^{2\pi}\\ &= (-320) \times \left(\cos \dfrac{\pi}{4} - \cos 0\right)[2\pi]\\ &= (-320) \times \left(-0.29289\right)[2\pi]\\ &= 588.9 \end{align*}
Correct Answer: B