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Practice questions for the toroidal solenoid.

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A coil comprised from {turns} turns is wrapped around a ferrite core carrying a peak flux density of {Bfield} T varying sinusoidally at a frequency of {frequency} kHz. The cross sectional area of the core is {xsection} mm2.

\n

Use the values of constant provided in the course when performing calculations.  Submit numerical answers to four significant figures and you may use scientific notation.  

", "advice": "

The point to this question is that we need a time varying field to induce a current.  We're told the flux density varies sinusoidally with a given frequency, $f$, and provided with a peak amplitude, $B_0$.  We're also told that the flux is zero at $t=0$s.  We can therefore express the $B$-field as 

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$B(t)=B_0 \\sin(\\omega t+\\gamma)$

\n

where $\\omega$ is the angular frequency $2 \\pi f$, and $\\gamma$ is the phase angle.  Since the flux (and therefore the flux density) is zero at $t=0$s, the phase angle can be taken to be zero or $\\pi$ radians.  We can choose zero for simplicity in this case.

\n

The flux is related to the flux density as $\\phi(t)=B(t)A$, and use the relationship that the flux linkage is $\\Psi=N\\phi$ to write $\\Psi(t)$.  

\n

Applying Faraday's Law requires a derivitive of the flux linkage, which is easily obtained as 

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$\\displaystyle{{d\\Psi\\over dt}={d\\over dt}N\\phi={d\\over dt}NAB(t)=NA{dB(t)\\over dt} = N A B_0 \\omega \\cos(\\omega t)}$. 

\n

Hence $|V|=NA\\omega B_0=2\\pi NAfB_0$.

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Peak B-field amplitude in T.

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Cross-sectional area of ferrite core in mm2.

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Calculated amplitude of sinusoidally varying induced voltage, Volts.

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Sinusoidal frequency in kHz.

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Number of turns in the solenoid.

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Caclulated angular frequency in cycles/s.

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Calculated flux in Wb (note conversion of area from mm2 to m2)

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What the mathematical expression for the maximum flux in the ferrite core in terms of one or more of the following variables: $B$ (peak magnetic flux density), $\\mu$ (permeability), $A$ (cross-sectional area), $N$ (number of turns) and $f$ (frequency).

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$\\phi_m=$[[0]]

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What is the value of the flux in this case?

\n

$\\phi_m=$[[0]] Wb

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What is the mathematical form of the magnetic flux as a function of time ($t$), frequency ($f$), and peak flux ($\\phi_m$)?  You may assume that the flux is zero at $t=0$s.

\n

$\\phi(t)=$[[0]]

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What is the relationship between the flux, $\\phi$ and flux-linkage, $\\Psi$ for the coil?

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Using Faraday's Law,

\n

$|V|=\\displaystyle{\\left|{{d\\Psi}\\over{dt}}\\right|},$

\n

that relates the voltage flux linkage, determine the amplitude of the induced voltage.

\n

$V_{\\rm max}=$[[0]]Volts

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A toriodal solenoid is constructed to act as an inductor.  It has the following properties:

\n\n

When entering formulae use only the above symbols along with the symbol for permeability of free space, $\\mu_0$ (mu_0), the magnetic flux, $\\phi$ (phi), the magnetic flux density, $B$, the magnetising field strength, $H$, the flux linkage, $\\Psi$ (psi), the inductance, $L$, the reluctance, $S$, and the stored energy, $U$.  In each case use the simplest formula based upon the quantity from the previous part.

\n

When providing numerical answers you may express them using scientific notation.  Express values to four significant figures and use the values of physical constants as provided in the course notes.

", "advice": "

This question is an example of a series of linked quantities. 

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${\\rm MMF}= N i=${mmf} Amps

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$|H|=\\displaystyle{{\\rm MMF}\\over {\\rm path~length}}=\\displaystyle{Ni\\over2\\pi R}=${Hfield} A/m

\n

$|B|=\\mu_0\\mu_r|H|=\\mu|H|=${Bfield} T

\n

$\\phi=B A=${phi} Wb

\n

$\\Psi = N \\phi=${Psi} Wb

\n

$L = \\displaystyle{\\Psi\\over i}=${inductance} Henrys

\n

$\\text{Stored energy}={1\\over2}Li^2=${energy} Joules

\n

The field that a given ferro-magnetic material can amplify is limited to its saturation value.  Raising the current beyond this point does not increase the flux density beyond the base-line $\\mu_0$ level.  If we know the saturation field, $B_{\\rm sat}$, then we can determine the current since we can re-arrange the formulae above to give

\n

$B_{\\rm sat}=\\mu H=\\displaystyle{\\mu N i_{\\rm sat}\\over 2\\pi R}\\Rightarrow i_{\\rm sat}=\\displaystyle{2\\pi RB_{\\rm sat}\\over \\mu_0 \\mu_r N}=${isat} Amps

\n

The flux-linkage rises up to the point of saturation, so a current increase beyond this point simply reduces the inductance (since $L=\\Psi_{\\rm sat}/i$).

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Calculated MMF, Amps.

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Cross-sectional area of core (m^2).

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Core radius in metres.

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Ring radius in metres.

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Calculated inductance (H^-1)

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Calculated flux (T).

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Calculated stored energy (J).

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Number of turns in the solenoid.

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Flux linkage, Wb

", "templateType": "anything"}, "Bsat": {"name": "Bsat", "group": "Ungrouped variables", "definition": "Bfield+random(0.8..1.2#0.1)", "description": "

Flux density at which the ferrite core 'saturates' in Tesla.

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Current in the coil (Amps)

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Total permeability.

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Permeability of free space, H/m

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Calculated inductance (Henry)

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Relative permeability of the core.

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Calculated current to achieve saturated B-field (Amps)

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Calculated H-field, A/m.

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The mathematical expression for the MMF is ${\\rm MMF} =$[[0]].

\n

The value of the MMF is [[1]] Amps.

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The mathematical expression for the magnetising field strength in the core is $|H| =$[[0]].

\n

The value of $|H|$ is [[1]] Amps/m.

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The mathematical expression for the magnetic flux density in the core is $|B| =$[[0]].

\n

The value of $|B|$ is [[1]] Tesla.

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The mathematical expression for the magnetic flux in the core is $\\phi =$[[0]].

\n

The value of $\\phi$ is [[1]] Wb.

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The mathematical expression for the flux linkage with the coil is $\\Psi =$[[0]].

\n

The value of $\\Psi$ is [[1]] Wb.

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The mathematical expression for the solenoid inductance is $L =$[[0]].

\n

The value of $L$ is [[1]] Henrys.

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The mathematical expression for the solenoid reluctance is $S =$[[0]].

\n

The value of $S$ is [[1]] H$^{-1}$.

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The mathematical expression for the energy stored by the solenoid is $U =$[[0]].

\n

The value of $U$ is [[1]] Joules.

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The ferrite core saturates at a flux density of {Bsat} T.

\n

Determine the mathematical expression for the current that would produce this $B$-field: $i_{\\rm sat} =$[[0]].

\n

The value of $i_{\\rm sat}$ is [[1]] Amps.

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If the current is increased above the value that produces the saturated $B$-field, what is the impact upon the inductance?

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A toroidal solenoid is constructed using an iron core, {turns} turns of wire carrying a current of {current} A. The torus has a circular cross-section of area {areacm} cm2, and diameter of {diametercm} cm.

\n

When providing numerical answers you may express them using scientific notation.  Express values to four significant figures and use the values of physical constants as provided in the course notes.

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The equations linking the properties of a solenoid inductor should be familiar.  This question starts in the familiar way,

\n

$\\displaystyle {\\rm MMF}=Ni$

\n

$\\displaystyle |\\vec{H}|= {\\rm MMF\\over path~length}={Ni\\over \\pi d}$,

\n

where $d$ is the diameter of the ring. However, then the pathway differs in that we are provided with $\\phi$, and asked to calculate $B$ and $\\mu_r$.  This requires some alegbra

\n

$\\displaystyle \\phi =|\\vec{B}| A \\Rightarrow|\\vec{B}| = {\\phi\\over A}$

\n

and

\n

$\\displaystyle |\\vec{B}|= \\mu |\\vec{H}| = \\mu_0\\mu_r |\\vec{H}| \\Rightarrow \\mu_r = {|\\vec{B}|\\over \\mu_0|\\vec{H}| }$.

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Magnetomotive force, A

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Magnetic flux density, T.

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Magnetising field strength, A/m.

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Current throught the solenoid, A.

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Diameter of the ring in m.

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Cross-sectional area of core, cm^2.

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Cross-sectional area of core, m^2.

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Number of turns.

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Flux through core in Wb.

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Flux through core in micro-Wb.

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Permeability of free space, H/m.

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Diameter of the ring in cm.

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Relative permeability of the core.

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Calculate the magnetomotive force generate by the current in the coil.

\n

MMF= [[0]] A

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Calculate the magnetising field strength in the core.

\n

$|\\vec{H}|=$[[0]] A/m

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If the flux passing through the core is {fluxu}$\\mu$Wb, calculate the magnetic flux density in the core.

\n

$|\\vec{B}|=$[[0]] T

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Hence, calculate the relative permeability of the core.

\n

$\\mu_r=$[[0]] 

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