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alexandr402 [8]
3 years ago
6

What does a main sequence star become after it uses up its hydrogen in its core

Physics
1 answer:
Alexandra [31]3 years ago
6 0
After<span> the </span>hydrogen<span> fuel at the </span>core<span> has been consumed, the </span>star<span> evolves away from the </span>main sequence<span> on the HR diagram. The behavior of a </span>star<span> now depends on </span>its <span>mass, with </span>stars<span> below 0.23 M</span>☉ becoming<span> white dwarfs directly, whereas </span>stars<span> with </span>up<span> to ten solar masses pass through a red giant stage.</span>
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An electron is constrained to the central perpendicular axis of a ring of charge of radius 2.2 m and charge 0.021 mC. Suppose th
igomit [66]

Answer:

T = 1.12 10⁻⁷ s

Explanation:

This exercise must be solved in parts. Let's start looking for the electric field in the axis of the ring.

All the charge dq is at a distance r

           dE = k dq / r²

Due to the symmetry of the ring, the field perpendicular to the axis is canceled, leaving only the field in the direction of the axis, if we use trigonometry

            cos θ =\frac{dE_x}{dE}

             dEₓ = dE cos θ

              cos θ = x / r

substituting

                dEₓ = k \frac{dq}{r^2 } \ \frac{x}{r}

                DEₓ = k dq x / r³

let's use the Pythagorean theorem to find the distance r

             r² = x² + a²

where a is the radius of the ring

we substitute

              dEₓ = k \frac{x}{(x^2 + a^2 ) ^{3/2} } \ dq

we integrate

               ∫ dEₓ =k \frac{x}{(x^2 + a^2 ) ^{3/2} }  ∫ dq

               Eₓ = k \ Q \ \frac{x}{(x^2+a^2)^{3/2}}

In the exercise indicate that the electron is very central to the center of the ring

                x << a

                Eₓ = k \ Q \frac{x}{a^3 \ ( 1 +(x/a)^2)^{3/2})}

if we expand in a series

                  (\ 1+ (x/a)^2 \  )^{-3/2} = 1 - \frac{3}{2} (\frac{x}{a} )^2

we keep the first term if x<<a

                 Eₓ = \frac{ k Q}{a^3} \ x

the force is

                 F = q E

                 F = - \frac{kQ  }{a^3} \ x

this is a restoring force proportional to the displacement so the movement is simple harmonic,

                 F = m a

                 - \frac{keQ}{a^3} \x = m \frac{d^2 x}{dt^2 }

                 \frac{d^2 x}{dt^2} = \frac{keQ}{ma^3}  \ x

the solution is of type

                  x = A cos (wt + Ф)

with angular velocity

                w² = \frac{keQ}{m a^3}

angular velocity and period are related

                 w = 2π/ T

             

we substitute

               4π² / T² = \frac{keQ}{m a^3}

                T = 2π  \sqrt{\frac{m a^3 }{keQ} }

let's calculate

                T = 2π \sqrt{ \frac{ 9.1 \ 10^{-31} \ 2.2^3 }{9 \ 10^9 \ 1.6 \ 10^{-19}  \ 0.021  \ 10^{-3} }  }

                 T = 2π pi \sqrt{320.426 \ 10^{-18} }

                 T = 2π  17.9 10⁻⁹ s

                 T = 1.12 10⁻⁷ s

6 0
3 years ago
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