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luda_lava [24]
3 years ago
12

EARTH SPACE SCIENCE.

Physics
1 answer:
Luden [163]3 years ago
8 0

Answer:

c,e,f,d

Explanation:

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31.5 would be the acceleration.
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shepuryov [24]

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Explanation:

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8 0
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A ball is tossed from an upper-story window of a building. The ball is given an initial velocity of 8.00 m/s at an angle of 20.0
Leya [2.2K]

Explanation :

When a ball is tossed from an upper storey window off a building, the height of the object as a function of time is given by :

h(t)=ut+\dfrac{1}{2}at^2

Here, u = 8 m/s

The ball strikes at an angle of 20 degrees below the horizontal. We need to find the time taken by the ball to reach a point 10 meters below the level of launching such that, h (t) = 10 m and a = g = 9.8

10=ucos(20)t+\dfrac{1}{2}\times 9.8\times (t)^2

10=0.93\times 8t+4.9t^2

10=7.51t+4.9t^2

After solving the above equation, t = 0.855 seconds

So, the ball will take 0.855 seconds to reach a point 10 m below the level of launching. Hence, this is the required solution.

3 0
3 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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