Definitions [3]
Define ampere.
Current passed through each of the two infinitely long parallel straight conductors kept at a distance of one meter apart in vacuum causes each conductor to experience a force of 2 × 10-7 newton per meter length of the conductor.
A long solenoid is a coil whose length is much greater than its radius, producing a uniform magnetic field inside and nearly zero field outside.
Define the term ‘current sensitivity’ of a moving coil galvanometer.
The current sensitivity of a galvanometer is defined as the deflection produced in the galvanometer when a unit current flows through it.
Mathematically, it can be given by:
IS = `(NBA)/k`
Where k is the couple per unit twist.
Current sensitivity is defined as the deflection e per unit current.
Formulae [5]
\[\vec{E}=\frac{1}{4\pi\varepsilon_0}\frac{Q}{r^2}\hat{r}\]
\[\vec{B}=\frac{\mu_0IR^2}{2(x^2+R^2)^{3/2}}\hat{i}\]
Where:
- I = current
- R = radius of loop
- x = distance from centre along axis
- μ0 = permeability of free space
B = μ0nI
Where:
- μ0 = permeability of free space
- n = number of turns per unit length
- I = current
\[\vec{m}=I\vec{A}\]
For N turns:
\[\vec{m}=NI\vec{A}\]
\[B=\frac{\mu_0}{4\pi}\frac{2m}{x^3}\]
Magnetic Field on the Equatorial Line (for x ≫ R)
\[B=\frac{\mu_0}{4\pi}\frac{m}{x^3}\]
Theorems and Laws [1]
Obtain an expression for magnetic induction of a toroid of ‘N’ turns about an axis passing through its centre and perpendicular to its plane.
The toroid is a solenoid bent into the shape of a hollow doughnut.
According to Ampere's circuital law.
`phivecB.vec(dL) = mu_0I`
Here current 'I' flow through the ring as many times as there are the N no. of turns.
∴ `phivecB.vec(dL) = mu_0NI` ......(1)
Now, B and dL are in the same direction.
∴ `phivecB.vec(dL) = BphidL`
∴ `phivecB.vec(dL) = B.(2pir)` .....(2)
From (1) and (2),
`mu_0NI = B.(2pir)`
∴ B = `(mu_0NI)/(2pir)`
Concepts [13]
- Introduction to Moving Charges and Magnetism
- Magnetic force
- Motion in a Magnetic Field
- Biot-Savart Law
- Magnetic Field on the Axis of a Circular Current Loop
- Ampere’s Circuital Law
- Solenoid and the Toroid - the Solenoid
- Force Between Two Parallel Currents, the Ampere
- Torque on a Rectangular Current Loop in a Uniform Magnetic Field
- Circular Current Loop as a Magnetic Dipole
- Moving Coil Galvanometer
- Applications of Ampere’s Circuital Law > Magnetic Field of a Toroidal Solenoid
- Conversion of a Galvanometer into a Voltmeter
