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aev [14]
3 years ago
8

A cyclist maintains a constant velocity of 4.1 m/s headed away from point A. At some initial time, the cyclist is 244 m from poi

nt A. What will be his displacement from his starting position after 60 s?
Physics
1 answer:
astra-53 [7]3 years ago
6 0

Answer:

d=490\ m is his final displacement from the point A after 60 seconds.

Explanation:

Given:

Cyclist is moving away from A.

  • velocity of cyclist, v=4.1\ m.s^{-1}
  • displacement of the cyclist from point A at the time of observation, d_i=244\ m
  • time after which the next observation is to be recorded, t=60\ s

Now as the cyclist is moving away from point A his change in displacement after the mentioned time:

\Delta d=v.t

\Delta d = 4.1 \times 60

\Delta d=246\ m

<u>Now the the final displacement from point A after the mentioned time:</u>

d=d_i+\Delta d

d=244+246

d=490\ m

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In outer space, a piece of rock continues moving at the same velocity for
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The absence of external force in the outer space, allows the piece of rock to continue moving at the same velocity for thousands of years.

<h3>Absence of external force on the outer space</h3>

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2 years ago
There are 2.2 pounds in a kilogram. if a boys mass is 40kg, what is his height in pounds?
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\frac{1}{2.2} = \frac{40}{x}

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3 0
3 years ago
Read 2 more answers
A solenoid 1.85 m long and 2.20 cm in diameter carries a current of 21.0 A. The magnetic field inside the solenoid is 25.0 mT. F
kobusy [5.1K]

Answer:

A wire carrying a 30.0-A current passes between the poles of a strong magnet that is perpendicular to its field and experiences a 2.16-N force on the 4.00 cm of wire in the field. What is the average field strength?

Explanation:

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2 years ago
a particle is moving along a circular path having a radius of 4 in such that its position as a function of time is given by thet
ANTONII [103]

Answer:

Explanation:

Given

radius of circular path r=4\ in.

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\theta =\cos 2t---1

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\frac{\mathrm{d} \theta }{\mathrm{d} t}=\omega =-2\sin 2t----2

Differentiate 2 to get angular acceleration

\frac{\mathrm{d} \omega }{\mathrm{d} t}=-2^2\cos 2t ---3

Net acceleration is the vector summation of tangential and centripetal force

a_t=\alpha \times r

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a_r=\omega ^2\cdot r

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a_{net}=\sqrt{a_r^2+a_t^2}

a_{net}=\sqrt{(16\sin ^2(2t)+(-16\cos 2t)^2}

a_{net}=\sqrt{256\cos ^2(2t)+256\sin ^4(2t)}                                                    

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3 years ago
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