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| 184_notes:examples:week2_conducting_insulating_balls [2018/01/22 00:43] – tallpaul | 184_notes:examples:week2_conducting_insulating_balls [2018/05/17 16:37] – [Example: Attempting to Charge Insulators by Induction] curdemma |
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| ===== Attempting to Charge Insulators by Induction ===== | [[184_notes:charging_discharging|Return to Charging and Discharging]] |
| | ===== Example: Attempting to Charge Insulators by Induction ===== |
| In the notes on [[184_notes:charging_discharging#Charging|Charging and Discharging]], we saw how to charge a pair of conductors using induction. The relevant figure is shown below as a representation. Is it possible to charge a pair of insulators using induction? Why or why not? | In the notes on [[184_notes:charging_discharging#Charging|Charging and Discharging]], we saw how to charge a pair of conductors using induction. The relevant figure is shown below as a representation. Is it possible to charge a pair of insulators using induction? Why or why not? |
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| ===Representations=== | ===Representations=== |
| * From the notes, we can pull a representation for how we would charge //conductors// using induction: | * From the notes, we can pull a representation for how we would charge //conductors// using induction: |
| {{ 184_notes:induction.png?300 |Induction with Conductors}} | [{{ 184_notes:induction.png?300 |Induction with Conductors}}] |
| * We can model the atoms in an insulator as little ovals (like the one below), that show when one side of the atom is more positive or negative than the other side. When ovals are not shown, this will just mean the atoms are not polarized. | * We can model the atoms in an insulator as little ovals (like the one below), that show when one side of the atom is more positive or negative than the other side. When ovals are not shown, this will just mean the atoms are not polarized. |
| {{ 184_notes:polarizedatom.png?100 }} | [{{ 184_notes:polarizedatom.png?100|Polarized Atom }}] |
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| ===Goal=== | ===Goal=== |
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| ====Solution==== | ====Solution==== |
| | <WRAP TIP> |
| ===Approximations & Assumptions=== | === Assumption === |
| * We will use the same induction process as we did for conductors. | Right away, we make the assumption that an induction process for insulators would look the same as it does for conductors. The reason we make this assumption is because this process, as described in the notes, is our basis for understanding how charging by induction works. If it looks the same and involves the same steps, we can more easily describe what we think will happen. |
| * The insulators start out neutral, meaning there are no excess electrons on the surface or any unbounded electrons (all electrons have a corresponding positive nuclei). | </WRAP> |
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| We show the analogous "induction with insulators" with a step-by-step representation below. We knew from the facts that electrons cannot move freely between insulators, which is one of the key differences between insulators and conductors. At time $t=t_0$, both of the insulating balls start out as neutral. At time $t=t_1$, when the connected balls are moved close the charged object, the atoms in the insulators would polarize, but the electrons are not free to move further or to move from one ball to the next. This means when the insulating balls are separated at $t=t_2$, there are two polarized but overall neutral balls. As the balls are pulled farther away from the positive charge, they become less and less polarized, eventually returning to the same state that they were before at $t=t_0$ (neutral, not polarized). | We show the analogous "induction with insulators" with a step-by-step representation below. We knew from the facts that electrons cannot move freely between insulators, which is one of the key differences between insulators and conductors. At time $t=t_0$, both of the insulating balls start out as neutral. At time $t=t_1$, when the connected balls are moved close the charged object, the atoms in the insulators would polarize, but the electrons are not free to move further or to move from one ball to the next. This means when the insulating balls are separated at $t=t_2$, there are two polarized but overall neutral balls. As the balls are pulled farther away from the positive charge, they become less and less polarized, eventually returning to the same state that they were before at $t=t_0$ (neutral, not polarized). |