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PolarNik [594]
3 years ago
11

Which equation describes the line containing the points (-2, 3) and (1, 2)​

Physics
1 answer:
snow_lady [41]3 years ago
8 0

Answer:

y =  \frac{ - 1}{3}x +  \frac{7}{3}

Explanation:

\frac{y - 3}{2 - 3}  =  \frac{x + 2}{1 + 2}  \\  \ - y + 3 =  \frac{x + 2}{3}  \\  y =   \frac{ - 1}{3}x  +  \frac{7}{3}

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State the laws of vibration of a stringed Instrument​
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Read 2 more answers
The magnetic flux through a metal ring varies with time t according to ΦB = at3 − bt2, where ΦB is in webers, a = 6.00 Wb s−3, b
pychu [463]

To solve this problem it is necessary to apply the second derivative of the function to find the maximum time reference and thus calculate the maximum voltage.

With the maximum voltage by Ohm's Law it is possible to find the maximum current.

Ohm's law defines that

E = I*R

Where,

I = Current

R= Resistance

On the other hand by faraday studies and the potential can be expressed at the rate of change of the electric flow, that is

E = \frac{d\phi}{dt}

Replacing with our values we have that

E = \frac{d(6t^3-18t^2)}{dt}

E = -18t^2 +36t

The second derivative is

E' = -36t+36

When E' = 0 we have a Maximum, then

0 = -36t+36

t = 1

Therefore when the time is 1s E has a Maximum, replacing at the function

E(t) = -18t^2 +36t

E(1) = -18(1)^2 +36(1)

E = 18V

Then the maximum current will be given by

I = \frac{E}{R}

I = \frac{18}{2.8}

I = 6.42A

Therefore the maximum current induced in the ring is 6.42A

6 0
4 years ago
A circuit consists of a coil that has a self-inductance equal to 4.3 mH and an internal resistance equal to 16 Ω, an ideal 9 V b
fredd [130]

Answer:

t = 186.2 μs

Explanation:

Current in LR series circuit

I(t) = I_{s}( 1 - e^{-Rt/L)}----(1)

steady current =  I_{s} = V/R

time constant = τ =L/R =4.3 * 10^{-3} / 16\\

                                              = 0.268 ms

magnetic energy stored in coil = U_{L} = \frac{1}{2}LI^{2}

rate at which magnetic energy stored in coil= \frac{d}{dt}U_{L} =\frac{d}{dt} \frac{1}{2}LI^{2}   \\                            = LI\frac{dI}{dt}\\----(2)

rate at which power is dissipated in R:

                                       P = I^{2}R---(3)

To find the time when the rate at which energy is dissipated in the coil equals the rate at which magnetic energy is stored in the coil equate (2) and (3)

I^{2}R=LI \frac{dI}{dt}

[/tex]I=\frac{L}{R}\frac{dI}{dt}[/tex]----(4)

differentiating (1) w.r.to t

I(t)=I_{f} (1-e^{\frac{Rt}{L} })

\frac{dI}{dt} = I_{f}\frac{d}{dt}(1-e^{\frac{-Rt}{L} }   )

\frac{dI}{dt}= I_{f}(-\frac{R}{L} e^{\frac{-Rt}{L} } )\\---(5)

substituting (5) in (4)

I=I_{f}e^{-\frac{Rt}{L} }----(6)

equating (1) and (6)

I_{f}( 1- e^{-\frac{Rt}{L} } ) = I_{f}e^{-\frac{Rt}{L} }

1 - e^{-\frac{Rt}{L} } =  e^{-\frac{Rt}{L} }

\frac{1}{2}= e^{-\frac{Rt}{L} }

t= -\frac{L}{R}ln\frac{1}{2}

L= 4.3 mH

R= 16 Ω

t = 186.2 μs

3 0
3 years ago
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