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Question: A circle, having radius “r” has a line charge distribution over its circumference having linear char...

A circle, having radius “r” has a line charge distribution over its circumference having linear charge density λ=λ0cos2θ\lambda = {\lambda _0}{\cos ^2}\theta . Calculate the total electric charge residing on the circumference of the circle. [02πcos2θdθ=π]\left[ {\int\limits_0^{2\pi } {{{\cos }^2}\theta d\theta = \pi } } \right]

Explanation

Solution

Hint: The differential charge element for length dldl from circumference in terms of dθd\theta is dl=rdθdl = rd\theta

Formula Used:
1. Q=dqQ = \int {dq} over the entire domain. …… (a)
2. Charge density, λ=dqdl\lambda = \dfrac{{dq}}{{dl}} …… (b)
3. Differential element, dl=rdθdl = rd\theta …… (c)
4. Given required integral to use, 02πcos2θdθ=π\int\limits_0^{2\pi } {{{\cos }^2}\theta d\theta = \pi } …… (d)

Complete step by step answer:

Given,
charge density λ=λ0cos2θ\lambda = {\lambda _0}{\cos ^2}\theta …… (1)
radius of circle =r = r

Step 1 of 6:

Figure 1 shows the relationship between variables of integrand dθd\theta and dldl

Step 2 of 6:

Substituting values from equation (c) in equation (b) we get
λ=dqrdθ\lambda = \dfrac{{dq}}{{rd\theta }} where dl=rdθdl = rd\theta
dq=λdl=λrdθ\Rightarrow dq = \lambda dl = \lambda rd\theta …… (2)

Step 3 of 6:

Putting value from equation (2) in equation (a) gives us
Q=dqQ = \int {dq} Q=λrdθ\Rightarrow Q = \int {\lambda rd\theta } where QQis total charge distribution on given domain …… (3)

Step 4 of 6:

Substituting equation (1) in equation (3) we get
Q=λ0rcos2θdθQ = \int {{\lambda _0}r{{\cos }^2}\theta d\theta } where λ0{\lambda _0} and rr are constants …… (4)

Step 5 of 6:

Moving constants out of integration and supplying integration limit 0 to 2π\pi we get-
Q=λ0r02πcos2θdθQ = {\lambda _0}r\int\limits_0^{2\pi } {{{\cos }^2}\theta d\theta } …… (5)

Step 6 of 6:

Substituting value from equation (d) in equation (5) we get Q=πλ0rQ = \pi {\lambda _0}r

Correct Answer:

Q=πλ0rQ = \pi {\lambda _0}r

Additional Information:
Integrals like equations (d) are very useful in solving problems with circular symmetric axis. Above problem is solved in the polar coordinate system. Similarly, if surface or volume charge density is given then, one should focus on change of variable in integration so that it transforms into some known integral form. For example, equation (d)

Note: We should always try to solve our problem considering the given hints from the question itself. Here, integration was already provided which saved a lot of time.