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Aleksandr-060686 [28]
3 years ago
11

A square loop of side length a =4.5 cm is placed a distance b = 1.1 cm from a long wire carrying a current that varies with time

at a constant rate, i.e. I(t) = Qt, where Q = 5.9 A/s is a constant. In what direction does this current flow?
Part (b) What is the magnitude of the flux through the loop? Select the correct expression Correct Part (c) If the loop has a resistance of 2.5 Ω, how much induced current flows in the loop
Physics
2 answers:
Rasek [7]3 years ago
5 0

Answer:

a) The current will flow in a clockwise direction

b) The magnitude of the flux through the loop is given by the equation ; \phi = \frac{\mu_o Q{at}}{2 \pi}In (\frac{b+a}{b})

c) The amount of the induced current that flows in the loop = 3.50*10^{-8} \ \ A

Explanation:

The magnitude of the flux through the loop is given by the equation ; \phi = \frac{\mu_o Q{at}}{2 \pi}In (\frac{b+a}{b})

The amount of the induced current that flows in the loop can be calculated as:

Emf induced  E = -  \frac{d \phi}{dt}

E =   \frac{- \mu_o Q_a }{2 \pi} In (\frac{b+a}{b}) \frac{dt}{dt}

E =   \frac{- \mu_o Q_a }{2 \pi} In (\frac{b+a}{b})

E =   \frac{- 4 \pi *10^{-7}*5.9*4.5*10^{-2} }{2 \pi} In (\frac{(4.5+1.1)*10^{-2}}{1.1*10^{-2}})

E = -5.37*10^{-8}*1.627\\\\E = -8.737*10^{-8}\ \  V

The current induced I = \frac{E}{R}

\frac{-8.737*10^{-8}}{2.5} \\\\= 3.50*10^{-8} \ \ A

sergey [27]3 years ago
3 0

Answer:

a)Current will flow perpendicularly.

b)Magnitude of flux will be 2.987 N m2 C−1

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Explanation:

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System diagram for given situation is shown in attached Fig. 1

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a_{x} = -\omega^{2}  x

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<h3>PROOF:</h3>

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                                  I=\frac{1}{2}MR^{2} -----(1)

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                                             ∑τ = Iα ------(2)

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By definition of torque:

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                                       RF=\frac{1}{2}MR^{2}\alpha

                                       RF=\frac{1}{2}MR^{2}\alpha

from Fig 3 it can be seen that fs is force by which the cylinders roll without slipping as they oscillate

So above equation becomes

                                   f_{s}=\frac{1}{2}MR\alpha------ (5)

As angular acceleration is related to linear by:

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Eq (5) becomes

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Put (7) in (3)

                                  f_{s} - kx  = Ma_{x}[/tex] -----(8)

Using (6) in (8)

                               \frac{1}{2}Ma_{x} - kx =Ma_{x}

                                     a_{x} = \frac{2k}{3M} x --- (9)

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                                  a= -\omega^{2} x ----- (10)

Equating (9) and (10)

                                  \omega^{2} = \frac{2k}{3M}

\omega = \sqrt{ \frac{2k}{3M}}

then (9) becomes

                                a_{x} = - \omega^{2}x

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This proves that the motion of the center of mass of the cylinders is simple harmonic.

<h3 /><h3>B) Time Period</h3>

Time period is related to angular frequency as:

                                   T=\frac{2\pi }{\omega}

                                  T = 2\pi \sqrt{\frac{3M}{2k}

                           

 

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The total mechanical energy of the ball is equal to its maximum P.E

                                      E = mgh

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At height h', the P.E becomes

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