Rotating charged half ring

A charged half ring of radius R R is held fixed on a plane. Let the center of the half ring be O O .

Let us complete the circle C C which contains the half ring. A point P P is taken on the circumference of C C , such that P O \overrightarrow {PO} passes through the center of mass of the half ring.

The plane is then rotated with an angular velocity ω \omega about an axis passing through P P and perpendicular to the plane.

Find the value of B P E P 1 0 16 \dfrac {|\vec{B_P}|}{|\vec{E_P}|} \cdot 10^{16} where B P |\vec{B_P}| and E P |\vec{E_P}| are the magnitudes of magnetic and electric fields at point P P respectively.

Assumptions \textbf{Assumptions}

\bullet \ \ \ The mass distribution of the half ring is uniform.

\bullet \ \ \ \ The charge distribution of the half ring is uniform.

\bullet \ \ \ \ The above procedure is carried out in vacuum, so the permeability μ o = 4 π × 1 0 7 H/m \mu_{o}=4\pi \times 10^{-7} \ \text {H/m}

\bullet \ \ \ \ When the plane rotates, the angular velocity of the half ring with respect to the plane is 0 0

\bullet \ \ \ \ Coulomb's constant k = 9 × 1 0 9 N m 2 / C 2 k=9 \times 10^9 \ \text {N} \text{m}^2/\text {C}^2

ω = 9 rad/s \bullet \ \ \ \ \omega=9 \ \text{rad/s}

R = 1 m \bullet \ \ \ \ R=1 \ \text{m}


The answer is 2.

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1 solution

Jatin Yadav
Aug 19, 2014

Using simple trigonometry, we get:

A P = 2 R cos x 2 AP = 2R \cos \dfrac{x}{2}

B P = π / 2 π / 2 μ 0 λ R ω d x 2 π 2 × 2 R cos x 2 B_{P} = \displaystyle \int_{-\pi/2}^{\pi/2} \dfrac{\frac{\mu_{0} \lambda R \omega dx}{2 \pi}}{2 \times 2R \cos \frac{x}{2}}

= μ 0 λ ω 8 π π / 2 π / 2 d x cos x 2 \dfrac{\mu_{0} \lambda \omega}{8 \pi } \displaystyle \int_{-\pi/2}^{\pi/2} \dfrac{dx }{\cos \frac{x}{2}}

In Electric field only vertical component is summed.

E P = π / 2 π / 2 λ R d x cos x 2 4 π ϵ 0 × 4 R 2 cos 2 x 2 E_{P} = \displaystyle \int_{-\pi/2}^{\pi/2} \dfrac{\lambda R dx \cos \frac{x}{2}}{4 \pi \epsilon_{0} \times 4R^2 \cos^2 \frac{x}{2}}

= λ 16 π ϵ 0 R π / 2 π / 2 d x cos x 2 = \displaystyle \dfrac{\lambda }{16 \pi \epsilon_{0}R}\int_{-\pi/2}^{\pi/2} \dfrac{dx }{\cos \frac{x}{2}}

Hence, B P E P = 2 μ 0 4 π ω R 1 4 π ϵ 0 \dfrac{B_{P}}{E_{P}} = \dfrac{ 2 \frac{\mu_{0}}{4 \pi} \omega R}{\frac{1}{4 \pi \epsilon_{0}}}

Can anyone please explain what the question is saying.....

Tushar Gopalka - 6 years, 9 months ago

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@Tushar Gopalka The question asks to find the ratio of magnetic field and electric field at point P P , which is as shown ---

Charged Half-Ring Charged Half-Ring

Pratik Shastri - 6 years, 9 months ago

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Thanks....

Tushar Gopalka - 6 years, 9 months ago

Isn't there any elegant method . I thought there would be something to it.

Rohit Shah - 6 years, 8 months ago

Awesome solution.....

Tushar Gopalka - 6 years, 9 months ago

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