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professor190 [17]
3 years ago
5

If a proton and an electron are released when they are 6.50×10⁻¹⁰ m apart (typical atomic distances), find the initial accelerat

ion of each of them.
a) Acceleration of electron
b) Acceleration of proton
Physics
1 answer:
Cerrena [4.2K]3 years ago
3 0

Answer:

(a) Acceleration of electron= 5.993×10²⁰ m/s²

(b) Acceleration of proton= 3.264×10¹⁷ m/s²

Explanation:

Given Data

distance r= 6.50×10⁻¹⁰ m

Mass of electron Me=9.109×10⁻³¹ kg

Mass of proton Mp=1.673×10⁻²⁷ kg

Charge of electron qe= -e = -1.602×10⁻¹⁹C

Charge of electron qp= e = 1.602×10⁻¹⁹C

To find

(a) Acceleration of electron

(b) Acceleration of proton

Solution

Since the charges are opposite the Coulomb Force is attractive

So

F=\frac{1}{4(\pi)Eo }\frac{|qp*qe|}{r^{2} }\\   F=(8.988*10^{9}Nm^{2}/C^{2})*\frac{(1.602*10^{-19})^{2}  }{(6.50*10^{-10} )^{2}  } \\F=5.46*10^{-10}N

From Newtons Second Law of motion

F=ma

a=F/m

For (a) Acceleration of electron

a=F/Me\\a=(5.46*10^{-10} )/9.109*10^{-31}\\ a=5.993*10^{20}m/s^{2}

For(b) Acceleration of proton

a=F/Mp\\a=(5.46*10^{-10} )/1.673*10^{-27} \\a=3.264*10^{17}m/s^{2}

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a) The time of flight is 3.78 s

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Explanation:

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a)

The motion of the ball is a projectile motion, which consists of two independent motions:

- A uniform motion (constant velocity) along the horizontal direction  

- A uniformly accelerated motion, with constant acceleration (acceleration of gravity) in the downward direction  

We start by considering the vertical motion, to find the time of flight of the ball. We do it by using the following suvat equation: for the y-displacement:

y=u_y t+\frac{1}{2}at^2

where we have:

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u_y=u sin \theta is the initial vertical velocity, with u being the initial velocity (unknown) and \theta=-27.0^{\circ} the angle of projection

t is the time of the fall

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Along the x-direction, the equation of motion is instead

x=(u cos \theta)t

where ucos \theta is the horizontal component of the velocity. Rewriting this equation as

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And using the fact that the horizontal range is

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And solving for t, we find the time of flight:

t=\sqrt{\frac{y-x tan \theta}{g}}=\sqrt{\frac{-45-(59.0)(tan(-27^{\circ}))}{-9.8}}=3.78 s

b)

We can now find the initial speed, u, by using the equation of motion along the x-direction

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where we know that:

x = 59.0 m is the horizontal range

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u=\frac{x}{cos \theta t}=\frac{59.0}{(cos (-23^{\circ}))(3.78)}=17.0 m/s

c)

First of all, we notice that the horizontal component of the velocity remains constant during the motion, and it is equal to

v_x = u cos \theta = (17.0)(cos (-23^{\circ})=15.6 m/s

The vertical velocity instead changes according to the equation

v_y = u sin \theta + gt

Substituting all the values and t = 3.78 s, the time of flight, we find the vertical velocity at the time of impact:

v_y = (17.0)(sin (-23^{\circ}))+(-9.8)(3.78)=-43.7 m/s

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A closely wound circular coil has a radius of 6.00 cmand carries a current of 2.65 A. How many turns must it have if the magneti
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Answer:

Given:

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B = \frac{\mu_{o}NI}{2R}

Therefore,

N = \frac{2BR}{\mu_{o}I}

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Answer:

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(B) 589.9 m/s

(C)   0.0008707 m^{3} =  8.71 cm^{2}

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inlet temperature of steam (T1) = 400 degree celcius

inlet velocity (V1) = 60 m/s

outlet pressure (P2) = 2 MPa

outlet temperature (T2) = 300 degree celcius

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rate of heat loss (Q) = 75 kJ/s

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m = \frac{0.005 x 60}{0.07343}

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(B) we can get the outlet velocity using the energy balance equation

  E in = E out

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V2 = \sqrt{2(h1 - h2) +(V1)^{2} - 2\frac{Q}{m}

where h1 and h2 are the enthalpies and are gotten from table A-6

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(C) the outlet area is gotten from mass flow rate (m) = \frac{A2 x V2}{α}

  A2 = (α2 x m) / V2

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A2 = (0.12552 x 4.09) / 589.5 = 0.0008707 m^{3} =  8.71 cm^{2}

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