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Ksenya-84 [330]
2 years ago
5

A particle initially located at the origin has an acceleration of a 2.00j m/s2 and an initial velocity of v-6.00i m/s. (a) Find

the vector position of the particle at any time t (where t is measured in seconds). ti+ t2 j) m (b) Find the velocity of the particle at any time t. I + tj) m/s (c) Find the coordinates of the particle at t 5.00 s. (d) Find the speed of the particle at t 5.00 s. m/s
Physics
1 answer:
s2008m [1.1K]2 years ago
4 0

Answer:

  • \vec{r}(t) = (-6.00 \frac{m}{s} \ t , \frac{1}{2} \ 2.00  \ \frac{m}{s^2} \ t^2 )
  • \vec{v}(t) = (-6.00 \frac{m}{s}, 2.00  \ \frac{m}{s^2} \ t )
  • \vec{r}( 5.00 \ s) = (-30.00 \ m , 25.00 \ m )
  • | \vec{v} (5.00 \ s) | =11.66 \frac{m}{s}

Explanation:

The initial position of the particle, \vec{r}_0, is:

\vec{r}_0 = (0,0)

the initial velocity is:

\vec{v}_0 = - 6.00 \ \frac{m}{s} \hat{i} = (-6.00 \frac{m}{s},0)

and the initial acceleration:

\vec{a} = 2.00  \ \frac{m}{s^2} \ \hat{j} = ( 0, 2.00  \ \frac{m}{s^2})

<h3>a</h3>

The position \vec{r} at time t is

\vec{r}(t) = \vec{r}_0 + \vec{v}_0  \ t   + \frac{1}{2} \ \vec{a} \ t^2

So, for our problem is:

\vec{r}(t) = (0,0) + (-6.00 \frac{m}{s},0)  \ t   + \frac{1}{2} \ ( 0, 2.00  \ \frac{m}{s^2}) \ t^2

\vec{r}(t) = (0 -6.00 \frac{m}{s} \ t , 0 +  \frac{1}{2} \ 2.00  \ \frac{m}{s^2} \ t^2 )

\vec{r}(t) = (-6.00 \frac{m}{s} \ t , \frac{1}{2} \ 2.00  \ \frac{m}{s^2} \ t^2 )

<h3>b</h3>

The velocity \vec{v} at time t is

\vec{v}(t) = \vec{v}_0  + \vec{a} \ t

So, for our problem is:

\vec{v}(t) = (-6.00 \frac{m}{s},0)   + ( 0, 2.00  \ \frac{m}{s^2}) \ t

\vec{v}(t) = (-6.00 \frac{m}{s}, 2.00  \ \frac{m}{s^2} \ t )

<h3>c</h3>

At time 5.00 seconds the position will be:

\vec{r}( 5.00 \ s) = (-6.00 \frac{m}{s} \ 5.00 \ s , \frac{1}{2} \ 2.00  \ \frac{m}{s^2} \ (5.00 \ s ) ^2 )

\vec{r}( 5.00 \ s) = (-30.00 \ m , 25.00 \ m )

<h3>d</h3>

and the speed will be :

| \vec{v} (5.00 \ s) | = |(-6.00 \frac{m}{s}, 2.00  \ \frac{m}{s^2} \ 5.00 \ s) |

| \vec{v} (5.00 \ s) | = |(-6.00 \frac{m}{s}, 10.00  \ \frac{m}{s}) |

| \vec{v} (5.00 \ s) | = \sqrt{ (-6.00 \frac{m}{s})^2 + (10.00  \ \frac{m}{s}))^2 }

| \vec{v} (5.00 \ s) | = \sqrt{ 36.00 \frac{m^2}{s^2} + 100.00  \ \frac{m^2}{s^2}}

| \vec{v} (5.00 \ s) | =11.66 \frac{m}{s}

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Since, the two resistors are in parallel connections, their equivalence can be obtained as follow:

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