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erma4kov [3.2K]
3 years ago
8

Can u find the . in this?

Physics
2 answers:
nikklg [1K]3 years ago
4 0

Answer:

Yeah it's right there from the one next to the exclamation point

Yanka [14]3 years ago
4 0

Answer:

its not there

Explanation:

its literally not there

You might be interested in
c) If the ice block (no penguins) is pressed down even with the surface and then released, it will bounce up and down, until fri
eduard

Answer:

y = 20.99 V / A

there is no friction    y = 20.99 h

Explanation:

Let's solve this exercise in parts: first find the thrust on the block when it is submerged and then use the conservation of energy

when the block of ice is submerged it is subjected to two forces its weight  hydrostatic thrust

         

              F_net= ∑F = B-W

the expression stop pushing is

              B = ρ_water g V_ice

where rho_water is the density of pure water that we take as 1 10³ kg / m³ and V is the volume d of the submerged ice

We can write the weight of the body as a function of its density rho_hielo = 0.913 10³ kg / m³

             W = ρ-ice g V

              F_net = (ρ_water - ρ_ ice) g V

this is the net force directed upwards, we can find the potential energy with the expression

            F = -dU / dy

            ΔU = - ∫ F dy

            ΔU = - (ρ_water - ρ_ ice) g ∫ (A dy) dy

            ΔU = - (ρ_water - ρ_ ice) g A y² / 2

we evaluate between the limits y = 0,  U = 0, that is, the potential energy is zero at the surface

             U_ice = (ρ_water - ρ_ ice) g A y² / 2

now we can use the conservation of mechanical energy

starting point. Ice depth point

             Em₀ = U_ice = (ρ_water - ρ_ ice) g A y² / 2

final point. Highest point of the block

             Em_{f} = U = m g y

as there is no friction, energy is conserved

            Em₀ = Em_{f}

            (ρ_water - ρ_ ice) g A y² / 2 = mg y

let's write the weight of the block as a function of its density

            ρ_ice = m / V

            m = ρ_ice V

we substitute

             (ρ_water - ρ_ ice) g A y² / 2 = ρ_ice V g y

              y = ρ_ice / (ρ_water - ρ_ ice) 2 V / A

let's substitute the values

             y = 0.913 / (1 - 0.913) 2 V / A

             y = 20.99 V / A

This is the height that the lower part of the block rises in the air, we see that it depends on the relationship between volume and area, which gives great influence if there is friction, as in this case it is indicated that there is no friction

                V / A = h

where h is the height of the block

                 y = 20.99 h

7 0
4 years ago
which term describes soil that is able to transmit water? a. permeable b. horizontal c. biotic d. aggregate
Hatshy [7]

The answer would be permeable i know this because i just took the test on apex.

7 0
3 years ago
Read 2 more answers
two point charges of 5*10^-19 C and 20*10^-19C are separated by a distance of 2m. at which point on the line joining them will h
Aneli [31]

Answer:

On that line segment between the two charges, at approximately 0.7\; \rm m away from the smaller charge (the one with a magnitude of 5 \times 10^{-19}\; \rm C,) and approximately 1.3\; \rm m from the larger charge (the one with a magnitude of 20 \times 10^{-19}\; \rm C.)

Explanation:

Each of the two point charges generate an electric field. These two fields overlap at all points in the space around the two point charges. At each point in that region, the actual electric field will be the sum of the field vectors of these two electric fields.

Let k denote the Coulomb constant, and let q denote the size of a point charge. At a distance of r away from the charge, the electric field due to this point charge will be:

\displaystyle E = \frac{k\, q}{r^2}.

At the point (or points) where the electric field is zero, the size of the net electrostatic force on any test charge should also be zero.

Consider a positive test charge placed on the line joining the two point charges in this question. Both of the two point charges here are positive. They will both repel the positive test charge regardless of the position of this test charge.

When the test charge is on the same side of both point charges, both point charges will push the test charge in the same direction. As a result, the two electric forces (due to the two point charges) will not balance each other, and the net electric force on the test charge will be non-zero.  

On the other hand, when the test charge is between the two point charges, the electric forces due to the two point charges will counteract each other. This force should be zero at some point in that region.

Keep in mind that the electric field at a point is zero only if the electric force on any test charge at that position is zero. Therefore, among the three sections, the line segment between the two point charges is the only place where the electric field could be zero.

Let q_1 = 5\times 10^{-19}\; \rm C and q_2 = 20 \times 10^{-19}\; \rm C. Assume that the electric field is zero at r meters to the right of the 5\times 10^{-19}\; \rm C point charge. That would be (2 - r) meters to the left of the 20 \times 10^{-19}\; \rm C point charge. (Since this point should be between the two point charges, 0 < r < 2.)

The electric field due to q_1 = 5\times 10^{-19}\; \rm C would have a magnitude of:

\displaystyle | E_1 | = \frac{k\cdot q_1}{r^2}.

The electric field due to q_2 = 20 \times 10^{-19}\; \rm C would have a magnitude of:

\displaystyle | E_2 | = \frac{k\cdot q_2}{(2 - r)^2}.

Note that at all point in this section, the two electric fields E_1 and E_2 will be acting in opposite directions. At the point where the two electric fields balance each other precisely, | E_1 | = | E_2 |. That's where the actual electric field is zero.

| E_1 | = | E_2 | means that \displaystyle \frac{k\cdot q_1}{r^2} = \frac{k\cdot q_2}{(2 - r)^2}.

Simplify this expression and solve for r:

\displaystyle q_1\, (2 - r)^2 - q_2 \, r^2 = 0.

\displaystyle 5\times (2 - r)^2 - 20\, r^2 = 0.

Either r = -2 or \displaystyle r = \frac{2}{3}\approx 0.67 will satisfy this equation. However, since this point (the point where the actual electric field is zero) should be between the two point charges, 0 < r < 2. Therefore, (-2) isn't a valid value for r in this context.

As a result, the electric field is zero at the point approximately 0.67\; \rm m away the 5\times 10^{-19}\; \rm C charge, and approximately 2 - 0.67 \approx 1.3\; \rm m away from the 20 \times 10^{-19}\; \rm C charge.

8 0
3 years ago
Microphones and loudspeakers are used in an auditorium because the sound waves at the stage compared to the sound waves at the b
MaRussiya [10]
Acoustics (sounds)
Hope the this helps!
6 0
3 years ago
Explain why atomic radius decreases as you move to the right across a period for main-group elements but not for transition elem
Aleksandr-060686 [28]

Answer:

Explained.

Explanation:

Only the first question has been answered

In a period from left to right the nuclear charge increases and hence nucleus size is compressed. Thus,  atomic radius decreases.

In transition elements, electrons in ns^2 orbital remain same which is the outer most orbital having 2 electrons and the electrons are added to (n-1) d orbital. So, outer orbital electron experience almost same nuclear attraction and thus size remains constant.

7 0
3 years ago
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