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Charge is uniformly distributed with den...

Charge is uniformly distributed with density `rho` in a cylindrical region of radius R and infinite length. The magnitude of electric field at distance `(R )/(2)` and 2R from the axis of the cylinder is `E_(1)` and `E_(2)` respectively. The ratio `(E_(1))/(E_(2))` is equal to ___________.

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To solve the problem of finding the ratio \((E_1)/(E_2)\) for the electric field at distances \((R/2)\) and \(2R\) from the axis of a uniformly charged infinite cylinder, we can use Gauss's law. Here's a step-by-step solution: ### Step 1: Understanding the Problem We have a uniformly charged infinite cylinder with charge density \(\rho\) and radius \(R\). We need to find the electric field at two different distances from the axis of the cylinder: \(E_1\) at \(r = R/2\) and \(E_2\) at \(r = 2R\). ### Step 2: Applying Gauss's Law Gauss's law states that the electric flux through a closed surface is equal to the charge enclosed divided by the permittivity of free space (\(\epsilon_0\)): \[ \Phi_E = \frac{Q_{\text{enc}}}{\epsilon_0} \] Where \(\Phi_E = \oint \vec{E} \cdot d\vec{A}\). ### Step 3: Finding \(E_1\) at \(r = R/2\) 1. **Choose a Gaussian surface**: A cylindrical surface of radius \(R/2\) and length \(L\). 2. **Calculate the enclosed charge**: The volume of the cylinder of radius \(R/2\) and length \(L\) is: \[ V = \pi \left(\frac{R}{2}\right)^2 L = \frac{\pi R^2 L}{4} \] The enclosed charge \(Q_{\text{enc}}\) is: \[ Q_{\text{enc}} = \rho \cdot V = \rho \cdot \frac{\pi R^2 L}{4} \] 3. **Calculate the electric field**: The electric field \(E_1\) is uniform over the curved surface of the cylinder: \[ \Phi_E = E_1 \cdot (2\pi \cdot \frac{R}{2} \cdot L) = E_1 \cdot \pi R L \] Setting the two expressions for flux equal gives: \[ E_1 \cdot \pi R L = \frac{\rho \cdot \frac{\pi R^2 L}{4}}{\epsilon_0} \] Simplifying: \[ E_1 = \frac{\rho R}{4 \epsilon_0} \] ### Step 4: Finding \(E_2\) at \(r = 2R\) 1. **Choose a Gaussian surface**: A cylindrical surface of radius \(2R\) and length \(L\). 2. **Calculate the enclosed charge**: The entire charge within the cylinder of radius \(R\) is: \[ Q_{\text{enc}} = \rho \cdot \pi R^2 L \] 3. **Calculate the electric field**: The electric field \(E_2\) is uniform over the curved surface: \[ \Phi_E = E_2 \cdot (2\pi \cdot 2R \cdot L) = E_2 \cdot 4\pi R L \] Setting the two expressions for flux equal gives: \[ E_2 \cdot 4\pi R L = \frac{\rho \cdot \pi R^2 L}{\epsilon_0} \] Simplifying: \[ E_2 = \frac{\rho R}{4 \epsilon_0} \] ### Step 5: Finding the Ratio \((E_1)/(E_2)\) Now we can find the ratio: \[ \frac{E_1}{E_2} = \frac{\frac{\rho R}{4 \epsilon_0}}{\frac{\rho R}{4 \epsilon_0}} = 1 \] ### Final Answer The ratio \(\frac{E_1}{E_2}\) is equal to **1**.

To solve the problem of finding the ratio \((E_1)/(E_2)\) for the electric field at distances \((R/2)\) and \(2R\) from the axis of a uniformly charged infinite cylinder, we can use Gauss's law. Here's a step-by-step solution: ### Step 1: Understanding the Problem We have a uniformly charged infinite cylinder with charge density \(\rho\) and radius \(R\). We need to find the electric field at two different distances from the axis of the cylinder: \(E_1\) at \(r = R/2\) and \(E_2\) at \(r = 2R\). ### Step 2: Applying Gauss's Law Gauss's law states that the electric flux through a closed surface is equal to the charge enclosed divided by the permittivity of free space (\(\epsilon_0\)): \[ ...
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