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Luda [366]
4 years ago
10

The box now rests on a frictionless ramp angled at 15◦ . The mover pulls up on a rope attached to the box to move it up the incl

ine. 33 kg F 29 ◦ 15◦ If the rope makes an angle of 29 ◦ with the horizontal, what is the smallest force the mover would have to exert to move the box up the ramp? The acceleration due to gravity is 9.81 m/s 2 .

Physics
1 answer:
Nataly [62]4 years ago
3 0

Answer:

F = 84.61 N

Explanation:

As in the figure, since there is no friction so if component of Force applied along the incline is greater than the component of weight along the incline, then the object will move up the incline.

component of Force along the incline = F cos(23° - 15°) = F cos(8°)

component of weight along the incline = 33*g*sin(15°) = 33*9.81*sin(15°)

Equating the above two components of forces will give the minimum Force required.

F cos(8°) = 33*9.81*sin(15°)

F = 33*9.81*sin(15°) / cos(8°)                  (calculate the value using a scientific calculator)

<u>F = 84.61 N</u>

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Given the function f(x) = 8x3 − 3x2 − 5x 8, what part of the function indicates that the left and right ends point in opposite d
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Answer: The degree of the first term.

Explanation:

The function:

f(x) = 8x^3-3x^2-5x^8

The left and right ends would be indicated when x is changed to -x. When this is substituted, the change is indicated by the first term because only the degree of first term is odd.

Let the left hand side be donated by -x.

Then,

f(-x) =8(-x)^3-3(-x)^2-5(-x)^8\\ \Rightarrow f(-x)=-8x^3-3x^2-5x^8

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A certain water wave has a wavelength of 25 m and a frequency of 4.0 Hz. What is its velocity?
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8 0
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We have an initially uncharged hollow metallic sphere with radius of 5.0 cm. I place a small object with a charge of +20 µC at t
Advocard [28]

Answer:

d. 1.8E+7 N/C

Explanation:

In order to find the electric field outside the hollow metallic sphere, we can apply Gauss' Law, using a spherical gaussian surface with radius equal to 10 cm from the center of the sphere.

As the electric field must be normal to the surface at any point (no tangential fields can exist in electrostatic conditions) it must be radially pointed. By symmetry, at a same radius, the magnitude of the field must be the same.

As the dA vector is always normal to the surface and aiming outward, the dot product E*dA, can be taken out of the integral, as follows:

E*A = \frac{Qenc}{\epsilon0}

where Qenc, is the total charge enclosed by the gaussian surface. Just due to the conservation of charge, this charge must be equal to +20 μC.

Now, how can this charge be distributed on the outer surface of the shell?

If we apply Gauss´Law to a gaussian surface with a radius just inside the sphere (between the inner and outer surface), we will find that the flux is 0, due to the electric field is 0 inside a conductor.

We could write the same equation as above:

E*A = \frac{Qenc}{\epsilon0} = 0

If the left side of the equation is 0, the right one must be zero too:

⇒ Qenc = 0  ⇒ Qc + Qin = 0 ⇒ Qin = -20 μC.

As the metallic sphere must remain neutral, an equal and opposite charge must build up on the outer surface:

⇒ Qou = +20 μC

The other parameters in the equation are:

r = 0.1 m

ε₀ = 8.85*10⁻¹² C²/N*m²

Replacing by the values, we can solve for E as follows:

E = \frac{1}{4*\pi*\epsilon0} *\frac{Qenc}{r^{2}} = \frac{1}{4*\pi*8.85e-12} *\frac{+20e-6C}{(0.1m)^{2}} = 1.8e7 N/C

⇒ E = 1.8*10⁷ N/C

So, the statement d. is true.

3 0
3 years ago
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