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| 184_notes:pc_force [2021/01/26 21:15] – bartonmo | 184_notes:pc_force [2021/01/27 15:57] (current) – [Two Point Charges] bartonmo |
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| $$\vec{F}_{net \rightarrow q}=q*\vec{E}_{net}$$ | $$\vec{F}_{net \rightarrow q}=q*\vec{E}_{net}$$ |
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| Where we are using the notation of $net \rightarrow q$ to show that this is the force //from// the net electric field //on// the charge q. Since electric field is a vector and charge is a scalar, when they are multiplied together, the result is a vector (electric force). This vector points in the same direction as the electric field for positive charges and in the opposite direction of the electric field in the case of negative charges. **Note that this is the electric force from the //external electric field// on the //charge//**. A charge's own electric field cannot affect the charge itself (for the same reason that you can't lift a board while standing on it and fly). **Also note that electric force is not the same thing as electric field**, but they are related. The electric field is the //electric force per unit charge// at a given location; in a sense, it tells you how large (magnitude) and which way (direction) the force could be. //Note there's some ambiguity about the direction of the force as it would matter which kind of charge is placed in the field.// | Where we are using the notation of $net \rightarrow q$ to show that this is the force //from// the net electric field //on// the charge q. Since electric field is a vector and charge is a scalar, when they are multiplied together, the result is a vector (electric force). This vector points in the same direction as the electric field for positive charges and in the opposite direction of the electric field in the case of negative charges. **Note that this is the electric force from the //external electric field// on the //charge//**. A charge's own electric field cannot affect the charge itself (for the same reason that you can't lift a board while standing on it and fly). **Also note that electric force is not the same thing as electric field**, but they are related. The electric field is the //electric force per unit charge// at a given location; in a sense, it tells you how large (magnitude) and which way (direction) the force could be. //Note there is some ambiguity about the direction of the force as it would matter which kind of charge is placed in the field.// |
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| The electric force works in the same way as any other force that you learned about in Mechanics: | The electric force works in the same way as any other force that you learned about in Mechanics: |
| * The electric force has units of newtons (N). | * **The electric force has units of newtons (N).** |
| * The electric force can be combined with any other forces acting on an object to find the [[183_notes:momentum_principle#Net_Force|net force]] on that object. | * The electric force can be combined with any other forces acting on an object to find the [[183_notes:momentum_principle#Net_Force|net force]] on that object. |
| * The electric force can contribute to a [[183_notes:momentum_principle|change in the object's momentum]] (in other words the electric force can accelerate a charge). | * The electric force can contribute to a [[183_notes:momentum_principle|change in the object's momentum]] (in other words the electric force can accelerate a charge). |
| $$\vec{F}_{1 \rightarrow 2}=\frac{1}{4\pi\epsilon_0}\frac{q_{1}q_{2}}{(r_{1 \rightarrow 2})^3}\vec{r}_{1 \rightarrow 2}=\frac{1}{4\pi\epsilon_0}\frac{q_{1}q_{2}}{(r_{1 \rightarrow 2})^2}\hat{r}_{1 \rightarrow 2}$$ | $$\vec{F}_{1 \rightarrow 2}=\frac{1}{4\pi\epsilon_0}\frac{q_{1}q_{2}}{(r_{1 \rightarrow 2})^3}\vec{r}_{1 \rightarrow 2}=\frac{1}{4\pi\epsilon_0}\frac{q_{1}q_{2}}{(r_{1 \rightarrow 2})^2}\hat{r}_{1 \rightarrow 2}$$ |
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| Where here we have used the [[184_notes:math_review#Unit_Vectors|definition of the unit vector]] ($\hat{r}=\frac{\vec{r}}{r}$) to get the two different versions of the equation. There are a few things to notice about this equation. First, this equation is **only true for the electric force between two point charges**. Second, this force is **not a constant force** - it depends on the separation distance between the two charges. The closer the two charges are, the stronger the push/pull will be. Finally, this equation may look familiar from mechanics - if you change the charges into masses and change the constant, you will get the equation for [[183_notes:gravitation|Newtonian gravity]] that describes the gravitational interaction between two large masses. It turns out that there are many parallels between the gravitational force and the electric force. | Where here we have used the [[184_notes:math_review#Unit_Vectors|definition of the unit vector]] ($\hat{r}=\frac{\vec{r}}{r}$) to get the two different versions of the equation. There are a few things to notice about this equation. First, this equation is **only true for the electric force between two point charges**. Second, this force is **not a constant force** - it depends on the separation distance between the two charges. **The closer the two charges are, the stronger the push/pull will be.** Finally, this equation may look familiar from mechanics - if you change the charges into masses and change the constant, you will get the equation for [[183_notes:gravitation|Newtonian gravity]] that describes the gravitational interaction between two large masses. It turns out that there are many parallels between the gravitational force and the electric force. |
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| ==== Examples ==== | ==== Examples ==== |
| [[:184_notes:examples:Week3_balloon_wall|Ballon Stuck to a Wall]] | [[:184_notes:examples:Week3_balloon_wall|Ballon Stuck to a Wall]] |