PHYS 208 Lecture 20
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Inductance
An inductor is any device that produces a magnetic field.
Mutual Inductance
The current in one circuit affects emf in the other through magnetic fields
Failed to parse (MathML with SVG or PNG fallback (recommended for modern browsers and accessibility tools): Invalid response ("Math extension cannot connect to Restbase.") from server "https://wikimedia.org/api/rest_v1/":): {\displaystyle \Phi_2 = M_{21} i_1} , where Failed to parse (MathML with SVG or PNG fallback (recommended for modern browsers and accessibility tools): Invalid response ("Math extension cannot connect to Restbase.") from server "https://wikimedia.org/api/rest_v1/":): {\displaystyle M} is the mutual inductance of loop 2 due to loop 1
Failed to parse (MathML with SVG or PNG fallback (recommended for modern browsers and accessibility tools): Invalid response ("Math extension cannot connect to Restbase.") from server "https://wikimedia.org/api/rest_v1/":): {\displaystyle M} has units of Henry [V / (A / s) = V · s / A = H]
Example
(a) Calculate the inductance of a very long solenoid that has Failed to parse (MathML with SVG or PNG fallback (recommended for modern browsers and accessibility tools): Invalid response ("Math extension cannot connect to Restbase.") from server "https://wikimedia.org/api/rest_v1/":): {\displaystyle n} turns of wire per meter of radius Failed to parse (MathML with SVG or PNG fallback (recommended for modern browsers and accessibility tools): Invalid response ("Math extension cannot connect to Restbase.") from server "https://wikimedia.org/api/rest_v1/":): {\displaystyle a} carrying a current of Failed to parse (MathML with SVG or PNG fallback (recommended for modern browsers and accessibility tools): Invalid response ("Math extension cannot connect to Restbase.") from server "https://wikimedia.org/api/rest_v1/":): {\displaystyle i} . there is another coil with Failed to parse (MathML with SVG or PNG fallback (recommended for modern browsers and accessibility tools): Invalid response ("Math extension cannot connect to Restbase.") from server "https://wikimedia.org/api/rest_v1/":): {\displaystyle N} turns of radius Failed to parse (MathML with SVG or PNG fallback (recommended for modern browsers and accessibility tools): Invalid response ("Math extension cannot connect to Restbase.") from server "https://wikimedia.org/api/rest_v1/":): {\displaystyle R} around a section of the solenoid.
Failed to parse (MathML with SVG or PNG fallback (recommended for modern browsers and accessibility tools): Invalid response ("Math extension cannot connect to Restbase.") from server "https://wikimedia.org/api/rest_v1/":): {\displaystyle \begin{align} B_{solenoid} &= \mu_0 i(t) n & \mbox{along axis by RHR} \\ \Phi_R &= N \Phi_{one\ turn} = N \int \vec{B} \cdot \mathrm{b}\vec{A} \\ &= N B(t) (\pi a^2) & \vec{B} \mbox{ from solenoid is only flux through large loop} \\ &= N \mu_0 n i(t) (\pi a^2) \\ M &= \frac{Phi_R}{i(t)} \\ &= N \mu_0 Nn (\pi a^2) \end{align}}
For N = 100 turns, n = 1000 turns/meter, a = 10 cm:
- M = 4 π2 × 10−6 Henrys
(b) What is the emf induced in the R-loop if the current in the solenoid changes at a rate of Failed to parse (MathML with SVG or PNG fallback (recommended for modern browsers and accessibility tools): Invalid response ("Math extension cannot connect to Restbase.") from server "https://wikimedia.org/api/rest_v1/":): {\displaystyle \frac{\mathrm{d}i}{\mathrm{d}t}}
?
Failed to parse (MathML with SVG or PNG fallback (recommended for modern browsers and accessibility tools): Invalid response ("Math extension cannot connect to Restbase.") from server "https://wikimedia.org/api/rest_v1/":): {\displaystyle \mathcal{E} = -\frac{M}{\mathrm{d}i/\mathrm{d}t}}
Another Example
What is the inductance between a toroid with Failed to parse (MathML with SVG or PNG fallback (recommended for modern browsers and accessibility tools): Invalid response ("Math extension cannot connect to Restbase.") from server "https://wikimedia.org/api/rest_v1/":): {\displaystyle N_T} turns, an inner radius of Failed to parse (MathML with SVG or PNG fallback (recommended for modern browsers and accessibility tools): Invalid response ("Math extension cannot connect to Restbase.") from server "https://wikimedia.org/api/rest_v1/":): {\displaystyle a} , an outer radius of Failed to parse (MathML with SVG or PNG fallback (recommended for modern browsers and accessibility tools): Invalid response ("Math extension cannot connect to Restbase.") from server "https://wikimedia.org/api/rest_v1/":): {\displaystyle b} , and a height (thickness) of Failed to parse (MathML with SVG or PNG fallback (recommended for modern browsers and accessibility tools): Invalid response ("Math extension cannot connect to Restbase.") from server "https://wikimedia.org/api/rest_v1/":): {\displaystyle c} and a loop of radius Failed to parse (MathML with SVG or PNG fallback (recommended for modern browsers and accessibility tools): Invalid response ("Math extension cannot connect to Restbase.") from server "https://wikimedia.org/api/rest_v1/":): {\displaystyle R} around the toroid?
Recall that the magnetic field of a solenoid at a distance Failed to parse (MathML with SVG or PNG fallback (recommended for modern browsers and accessibility tools): Invalid response ("Math extension cannot connect to Restbase.") from server "https://wikimedia.org/api/rest_v1/":): {\displaystyle r} from the center (hole) of the donut is given by Failed to parse (MathML with SVG or PNG fallback (recommended for modern browsers and accessibility tools): Invalid response ("Math extension cannot connect to Restbase.") from server "https://wikimedia.org/api/rest_v1/":): {\displaystyle B(r) = \frac{\mu_0 i N}{2 \pi r}} (B-field is non-uniform)
Failed to parse (MathML with SVG or PNG fallback (recommended for modern browsers and accessibility tools): Invalid response ("Math extension cannot connect to Restbase.") from server "https://wikimedia.org/api/rest_v1/":): {\displaystyle \begin{align} \Phi_{1\ loop} &= \int \mathrm{B} \cdot \mathrm{d}\vec{A} = \int_a^b \left( \frac{\mu_0 i N_T}{2 \pi r} \right) \left( c \mathrm{d}r \right) \\ &= \frac{\mu_0 i N_T c}{2 \pi} \int_a^b \frac{\mathrm{d}r}{r} \\ &= \frac{\mu_0 i N_T c}{2 \pi} \ln \left( \frac{b}{a} \right) \\ M &= \frac{\Phi_{tot}}{i(t)} = \frac{\mu_0 N_T N c}{2 \pi} \ln \left( \frac{b}{a} \right) \end{align}}
Self Inductance
a circuit that produces a magnetic field affects its own magnetic flux and thus its own emf. The induced emf counters the emf of the system and is called "back emf"
for Failed to parse (MathML with SVG or PNG fallback (recommended for modern browsers and accessibility tools): Invalid response ("Math extension cannot connect to Restbase.") from server "https://wikimedia.org/api/rest_v1/":): {\displaystyle N} turns,
Example
Self-inductance of toroid in #Another Example
Failed to parse (MathML with SVG or PNG fallback (recommended for modern browsers and accessibility tools): Invalid response ("Math extension cannot connect to Restbase.") from server "https://wikimedia.org/api/rest_v1/":): {\displaystyle \begin{align} L &= \frac{\Phi_{tot}}{I} = \frac{N \Phi_{1\ turn}}{I} \\ &= \frac{\mu_0 N^2 c}{2 \pi} \ln \left( \frac{b}{a} \right) \end{align}}
Magnetic Energy
Suppose we start with an inductor that initially has no current. As we add current, the back emf counters the addition, so work is being done to produce the magnetic field. Therefore, the magnetic field of an inductor stores energy.
Work done by power supply:
So the work done is
Example
Find the energy stored in a finite solenoid of length Failed to parse (MathML with SVG or PNG fallback (recommended for modern browsers and accessibility tools): Invalid response ("Math extension cannot connect to Restbase.") from server "https://wikimedia.org/api/rest_v1/":): {\displaystyle L} with a radius Failed to parse (MathML with SVG or PNG fallback (recommended for modern browsers and accessibility tools): Invalid response ("Math extension cannot connect to Restbase.") from server "https://wikimedia.org/api/rest_v1/":): {\displaystyle R} , a current Failed to parse (MathML with SVG or PNG fallback (recommended for modern browsers and accessibility tools): Invalid response ("Math extension cannot connect to Restbase.") from server "https://wikimedia.org/api/rest_v1/":): {\displaystyle I} , and Failed to parse (MathML with SVG or PNG fallback (recommended for modern browsers and accessibility tools): Invalid response ("Math extension cannot connect to Restbase.") from server "https://wikimedia.org/api/rest_v1/":): {\displaystyle N} turns
Failed to parse (MathML with SVG or PNG fallback (recommended for modern browsers and accessibility tools): Invalid response ("Math extension cannot connect to Restbase.") from server "https://wikimedia.org/api/rest_v1/":): {\displaystyle \begin{align} B &= \mu_0 i \frac{N}{L} \\ \Phi_{1\ loop} &= \frac{\mu_0 i N}{L} (\pi R^2) \\ L &= \frac{N^2 \mu_0 \pi R^2}{L} \\ U_B &= \frac{1}{2} \left( \frac{N^2 \mu_0 \pi R^2}{L} \right) I^2 \\ &= \frac{1}{2} B^2 \frac{L \pi R^2}{\mu_0} \\ \frac{U_B}{\pi R^2 L} = u_B &= \frac{1}{2} \frac{B^2}{\mu_0} \end{align}}
Recall from our study of electric fields that the potential energy per unit volume of an electric field is
Failed to parse (MathML with SVG or PNG fallback (recommended for modern browsers and accessibility tools): Invalid response ("Math extension cannot connect to Restbase.") from server "https://wikimedia.org/api/rest_v1/":): {\displaystyle u_E = \frac{1}{2} \epsilon_0 E^2}