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Question
23.3 a charged isolated conductor positive charge ( q ) is placed on a conducting spherical shell with inner radius ( r_1 ) and outer radius ( r_2 ). a particle with charge ( q ) is placed at the center of the cavity. the net charge on the outer surface of the conducting shell is
( -q ).
( q - q ).
( q + q ).
zero.
( q ).
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Brief Explanations
- Recall the property of a conducting shell: In a static situation, the electric field inside a conductor (the material of the shell, between \(R_1\) and \(R_2\)) is zero. By Gauss's law, the net charge enclosed by any Gaussian surface within the conductor must be zero.
- The charge \(q\) at the center induces a charge \(-q\) on the inner surface of the shell (to make the net charge enclosed by a Gaussian surface in the conductor zero).
- The conducting shell initially has a charge \(Q\). The total charge on the shell (inner + outer surface) must be \(Q\). Let the charge on the outer surface be \(Q_{\text{outer}}\). We know that charge on inner surface is \(-q\), so \( -q + Q_{\text{outer}}=Q\). Solving for \(Q_{\text{outer}}\), we get \(Q_{\text{outer}} = Q + q\)? Wait, no, wait. Wait, the initial charge on the shell is \(Q\)? Wait, no, the problem says "Positive charge \(Q\) is placed on a conducting spherical shell" – so the shell has charge \(Q\) initially. Then a charge \(q\) is placed at the center. The inner surface will have \(-q\) (by induction, to cancel the field inside the conductor). Then the outer surface charge is \(Q + q\)? Wait, no, wait: the total charge on the shell is \(Q\) (initial). So inner surface charge (\(-q\)) plus outer surface charge (\(Q_{\text{outer}}\)) should equal \(Q\). So \(-q + Q_{\text{outer}} = Q\) → \(Q_{\text{outer}} = Q + q\)? Wait, no, maybe I misread. Wait, the problem says "Positive charge \(Q\) is placed on a conducting spherical shell" – so the shell's total charge is \(Q\). Then a charge \(q\) is at the center. The inner surface gets \(-q\) (because the electric field inside the conductor must be zero, so the Gaussian surface inside the conductor encloses \(q + \text{inner surface charge} = 0\) → inner surface charge is \(-q\)). Then the outer surface charge is total shell charge (\(Q\)) minus inner surface charge (\(-q\))? Wait, no: total charge on shell is inner + outer. So \(Q = (\text{inner charge}) + (\text{outer charge})\). Inner charge is \(-q\), so outer charge is \(Q - (-q)= Q + q\)? Wait, but maybe the shell was initially uncharged? Wait, no, the problem says "Positive charge \(Q\) is placed on a conducting spherical shell" – so the shell has charge \(Q\) initially. Wait, maybe I made a mistake. Wait, let's re-express:
- The conductor is isolated, so total charge on the conductor (shell) is \(Q\) (given: "Positive charge \(Q\) is placed on a conducting spherical shell").
- A charge \(q\) is placed at the center of the cavity.
- By induction, the inner surface (radius \(R_1\)) will have a charge \(-q\) (because in electrostatic equilibrium, the electric field inside the conductor (between \(R_1\) and \(R_2\)) is zero. Using Gauss's law, a Gaussian surface inside the conductor (radius between \(R_1\) and \(R_2\)) encloses \(q + \text{inner surface charge} = 0\) → inner surface charge \(= -q\).
- The total charge on the shell is the sum of the charge on the inner surface and the outer surface: \(Q = (\text{inner charge}) + (\text{outer charge})\).
- Substituting inner charge \(= -q\) into the equation: \(Q = -q + (\text{outer charge})\) → \(\text{outer charge} = Q + q\)? Wait, but the options include \(Q + q\) as one of the choices (the option " \(Q + q\)"). Wait, but let's check again. Wait, maybe the shell was initially uncharged? Wait, the problem says "Positive charge \(Q\) is placed on a conducting spherical shell" – so the shell has charge \(Q\) initially. Then adding a charge \(q\) at the center. The inner surface gets \(-q\), so the outer surface must have \(Q + q\) t…
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\(Q + q\) (the option labeled " \(Q + q\)")