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xenn [34]
2 years ago
5

A boy throws a baseball onto a roof and it rolls back down and off the roof with a speed of 4.05 m/s. If the roof is pitched at

34.0° below the horizon and the roof edge is 2.10 m above the ground, find the time the baseball spends in the air and the horizontal distance from the roof edge to the point where the baseball lands on the ground.
(a) the time the baseball spends in the air (in s)

(b) the horizontal distance from the roof edge to the point where the baseball lands on the ground (in m)
Physics
1 answer:
AlekseyPX2 years ago
8 0

(a) The time the baseball spends in the air is 0.92 s.

(b) The horizontal distance from the roof edge to the point where the baseball lands on the ground is 3.1 m.

<h3>Time spent in air by the baseball</h3>

h = vt - ¹/₂gt²

-2.1 = (4.05 x sin 34)t  - ¹/₂(9.8)(t²)

-2.1 = 2.26t - 4.9t²

4.9t² - 2.26t - 2.1 = 0

t = 0.92 s

<h3>Horizontal distance traveled by the baseball</h3>

R = Vx(t)

R = (4.05 x cos 34)(0.92)

R = 3.1 m

Thus, the time the baseball spends in the air is 0.92 s.

The horizontal distance from the roof edge to the point where the baseball lands on the ground is 3.1 m.

Learn more about horizontal distance here: brainly.com/question/24784992

#SPJ1

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There are seven SI base units, which are:

m - Meter - Length.

s - Second - Time.

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K - Kelvin - Temperature.

cd - Candela - Luminous Intensity.

kg - Kilogram - Mass.

I think that the delivered units are how they are used such as watts which are equal to one joule per second. Others are “ergs per second (erg/s), horsepower (hp), metric horsepower (Pferdestärke (PS) or cheval vapeur (CV)), and foot-pounds per minute.”

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A thick, spherical shell made of solid metal has an inner radius a = 0.18 m and an outer radius b = 0.46 m, and is initially unc
KonstantinChe [14]

(a) E(r) = \frac{q}{4\pi \epsilon_0 r^2}

We can solve the different part of the problem by using Gauss theorem.

Considering a Gaussian spherical surface with radius r<a (inside the shell), we can write:

E(r) \cdot 4\pi r^2 = \frac{q}{\epsilon_0}

where q is the charge contained in the spherical surface, so

q=5.00 C

Solving for E(r), we find the expression of the field for r<a:

E(r) = \frac{q}{4\pi \epsilon_0 r^2}

(b) 0

The electric field strength in the region a < r < b is zero. This is due to the fact that the charge +q placed at the center of the shell induces an opposite charge -q on the inner surface of the shell (r=a), while the outer surface of the shell (r=b) will acquire a net charge of +q.

So, if we use Gauss theorem for the region  a < r < b, we get

E(r) \cdot 4\pi r^2 = \frac{q'}{\epsilon_0}

however, the charge q' contained in the Gaussian sphere of radius r is now the sum of the charge at the centre (+q) and the charge induced on the inner surface of the shell (-q), so

q' = + q - q = 0

And so we find

E(r) = 0

(c) E(r) = \frac{q}{4\pi \epsilon_0 r^2}

We can use again Gauss theorem:

E(r) \cdot 4\pi r^2 = \frac{q'}{\epsilon_0} (1)

where this time r > b (outside the shell), so the gaussian surface this time contained:

- the charge +q at the centre

- the inner surface, with a charge of -q

- the outer surface, with a charge of +q

So the net charge is

q' = +q -q +q = +q

And so solving (1) we find

E(r) = \frac{q}{4\pi \epsilon_0 r^2}

which is identical to the expression of the field inside the shell.

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We said that at r = a, a charge of -q is induced. The induced charge density will be

\sigma_a = \frac{-q}{4\pi a^2}

where 4 \pi a^2 is the area of the inner surface of the shell. Substituting

q = 5.00 C

a = 0.18 m

We find the induced charge density:

\sigma_a = \frac{-5.00 C}{4\pi (0.18 m)^2}=-12.3 C/m^2

(e) -1.9 C/m^2

We said that at r = b, a charge of +q is induced. The induced charge density will be

\sigma_b = \frac{+q}{4\pi b^2}

where 4 \pi b^2 is the area of the outer surface of the shell. Substituting

q = 5.00 C

b = 0.46 m

We find the induced charge density:

\sigma_b = \frac{+5.00 C}{4\pi (0.46 m)^2}=-1.9 C/m^2

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