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184_notes:ind_graphs [2022/11/26 15:20] – valen176 | 184_notes:ind_graphs [2022/12/07 14:43] (current) – valen176 | ||
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===== Induction Graphs ===== | ===== Induction Graphs ===== | ||
- | In these notes, we will examine a few examples of changing magnetic fluxes and associated induced voltages. | + | In these notes, we will examine a few examples of changing magnetic fluxes and associated induced voltages. |
- | First let's consider when ΦB rises and falls linearly with the same magnitude of slope: | + | Vind=−dΦbdt |
+ | |||
+ | This is saying that the induced current is the **negative slope** of the magnetic flux. In other words, if the magnetic flux is increasing, then Vind will be negative, if the magnetic flux is decreasing, then Vind will be positive, and if the magnetic flux is constant, then Vind=0. | ||
+ | |||
+ | First let's consider when an example where ΦB rises and falls linearly with the same magnitude of slope: | ||
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\end{cases} | \end{cases} | ||
$$ | $$ | ||
- | Which finally means that Vind | + | Now we can multiply by −1 because of the negative sign in Faraday' |
$$ | $$ | ||
V_{ind}= | V_{ind}= | ||
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[{{184_notes: | [{{184_notes: | ||
- | We can see that from t=0 to t=10, ΦB(t) has a positive slope, so Vind is negative on that time interval. However, ΦB(t) is steeper from t=5 to t=10, so Vind is **more negative** on that time interval than from t=0 to t=5. From t=10 to t=15, ΦB(t) has a constant and negative slope, so Vind is constant and positive on that time interval. | + | We can see that from t=0 to t=10, ΦB(t) has a positive slope, so Vind is negative on that time interval. However, ΦB(t) is steeper from t=5 to t=10, so Vind is **more negative** on that time interval than from t=0 to t=5. From t=10 to t=15, ΦB(t) has a constant and negative slope, so Vind is constant and positive on that time interval. |
+ | |||
+ | |||
+ | $$ | ||
+ | \Phi_B(t)= | ||
+ | \begin{cases} | ||
+ | 2t & \text{if } 0< | ||
+ | 5t -15 & \text{if } 5< | ||
+ | -10t + 135 & \text{if } 10< | ||
+ | \end{cases} | ||
+ | $$ | ||
+ | Which means dΦBdt is: | ||
+ | $$ | ||
+ | \frac{d \Phi_B}{dt}= | ||
+ | \begin{cases} | ||
+ | 2 & \text{if } 0< | ||
+ | 5 & \text{if } 5< | ||
+ | -10 & \text{if } 10< | ||
+ | \end{cases} | ||
+ | $$ | ||
+ | Which finally means that Vind is: | ||
+ | $$ | ||
+ | V_{ind}= | ||
+ | \begin{cases} | ||
+ | -2 & \text{if } 0< | ||
+ | -5 & \text{if } 5< | ||
+ | 10 & \text{if } 10< | ||
+ | \end{cases} | ||
+ | $$ | ||
Finally, let's look at an example with a non-linear ΦB(t): | Finally, let's look at an example with a non-linear ΦB(t): |