Respuesta :
Answer:
Explanation:
Magnetic field due to a long wire
B = ( μ₀ / 4π ) x 2 I / r ( I is current through the wire )
= (μ₀ Q t ) / ( 2 π r ) [ I = Q t ]
b ) Magnetic field will change through the length of the square shaped loop . So we shall have to take the help of integration to calculate the flux through the loop.
Flux Φ = ∫ B dA
=∫ ( μ₀ / 4π ) x 2 I / r dA
10⁻⁷ x 2 I ∫ a dr/r
2 x 10⁻⁷ x Qt x a [ ln (2.9+1.2) / 1.2 ]
4.6 x 10⁻⁷ x 2.9 x 10⁻² t ln 4.1 / 1.2
16.4 x 10⁻⁹ t
Φ( t ) = 16.4 x 10⁻⁹ t
Induced emf = dΦ( t ) / dt = 16.4 x 10⁻⁹ v
current
16.4 x 10⁻⁹ / 2.5
= 6.56 x 10⁻⁹
(a) The expression for the magnetic field due to the wire is [tex]B(t) = \frac{2.3\mu_0 t}{2\pi r}[/tex].
(b) The magnitude of the flux through the loop is 3.224 x 10⁻⁸ Tm².
(c) The induced current flowing in the loop is 1.29 x 10⁻⁸ A.
Magnetic field due to the field
The magnetic field at a given distance due to current carrying wire is given as;
[tex]B = \frac{\mu_0 I}{2\pi r}[/tex]
when the current, I is given as a function flow rate of charge, the magnetic field becomes.
I = Qt = 2.3t
[tex]B(t) = \frac{\mu_0 Qt}{2\pi r}= \frac{2.3\mu_0 t}{2\pi r}[/tex]
Magnetic flux through the loop
The magnetic flux through the loop is calculated as follows;
Ф = BA
where;
- A is the area of the square loop
A = L² = 0.029 x 0.029 = 0.000841 m²
Relationship between, Q, and 'I'; Q = It ---(1)
I(t) = Qt ---(2)
Substitute (1) into (2)
I = (It)t
1 = t²
t = 1 s
[tex]B(t) = \frac{2.3\mu_0t}{2\pi r} \\\\B(1) = \frac{2.3 \times (4\pi \times 10^{-7}) \times (1)}{2\pi \times (0.012)} \\\\B (1) = 3.833 \times 10^{-5} \ T[/tex]
Ф = BA
Ф = (3.833 x 10⁻⁵) x (0.000841)
Ф = 3.224 x 10⁻⁸ Tm²
Induced emf
The emf induced in the loop is calculated as follows;
[tex]emf = \frac{d\phi}{dt} \\\\emf = \frac{dAB(t)}{dt} \\\\emf = A\frac{dB(t)}{dt} \\\\emf = AB = 3.224 \times 10^{-8} \ V[/tex]
Induced current in the loop
V = IR
[tex]I = \frac{V}{R} \\\\I = \frac{3.224 \times 10^{-8}}{2.5} \\\\I = 1.29 \times 10^{-8} \ A[/tex]
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