Respuesta :
Answer:
see explanation
Explanation:
Let me fill the rest of the question for you, it is a problem where you are supposed to find the electromotive force when a certain amount of time [tex]t[/tex] has passed, additionally, you have to find the direction of the induced current in the loop...
So you have a circular loop made out of iron with a circumference equal to 1.65 [m], (this is only so we can get the cross section area of the loop to fit it in an equation) and the decreasing rate of such is 0.12 [m/s].
Now a constant magnetic field which magnitude is 0.5 [T] is oriented perpendicular to the ring, we have to define whether if it is entering the plane of the ring or going outside,
If the magnetic field is entering the plane, by the right hand rule we have that the currrent is going clockwise, if the magnetic field is going outside it will go counter-clockwise
Now let's solve the problem
let's get the cross section area of the loop
we have the perimeter [tex]P=2\pi r[/tex] where r is the radius of the circle, we have P which is 1.65 [m], then [tex]r = \frac{P}{2\pi }[/tex]
now the area A is [tex]A = \pi r^2=\pi \frac{P^2}{4\pi^2}= \frac{P^2}{4\pi }[/tex]
Next we have that the EMF is the derivative of the flux with respect to t, and flux is [tex]\Phi = \int \vec B. \vec{dA}[/tex], so B and A are in the same direction so that is equal to
[tex]\Phi = \int B*dA*cos(0) =B* \int dA = BA=B*\frac{P^2}{4\pi }[/tex]
next the EMF [tex]\epsilon[/tex] will be [tex]|\epsilon| = |\frac{d}{dt }\Phi | = | \frac{B}{4\pi } \frac{d}{dt}(P^2)| = |\frac{BP}{2\pi } \frac{dP}{dt}|[/tex]
now the perimeter will be a function of t
[tex]P(t) = P - \frac{dP}{dt}*t[/tex]
you just need to replace the values in order to get the answer
let's say that [tex]t=5 [s][/tex]
so we will have [tex]P(t) = 1.65 - 0.12*5=1.05[m][/tex]
next we replace in the emf equation:
[tex]|\epsilon(t=5)| =|\frac{(0.5[T])*(1.05[m])}{2\pi }*0.12[m/s]| = 10 mV[/tex]