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Ainat [17]
4 years ago
9

Proton is placed 100 micrometers from a helium nucleus. Gravity pulls the proton and nucleus together while the electric force p

ushes them apart. Which is stronger and by how much ?
Physics
1 answer:
skad [1K]4 years ago
3 0

Answer:

Electric force is 6.2\cdot 10^{35} times stronger than gravitational force

Explanation:

The gravitational force between two objects is given by:

F_G = G\frac{m_1 m_2}{r^2}

where

G is the gravitational constant

m1, m2 are the masses of the two objects

r is the separation between the objects

Here we have:

m_1 = 1.67\cdot 10^{-27}kg (mass of the proton)

m_2=4\cdot 1.67\cdot 10^{-27} =6.68\cdot 10^{-27} kg (mass of the helium nucleus is equal to 4 times the mass of a proton)

r=100 \mu m = 100\cdot 10^{-6} m

So,

F_G = (6.67\cdot 10^{-11}) \frac{(1.67\cdot 10^{-27})(6.68\cdot 10^{-27})}{(100\cdot 10^{-6})^2}=7.44\cdot 10^{-56} N

The electric force between two charged object is given by

F_E=k\frac{q_1 q_2}{r^2}

where

k is the  Coulomb constant

q1, q2 are the two charges

r is the separation

Here we have

q_1 = 1.6\cdot 10^{-19}C (charge of the proton)

q_2 = 2\cdot (1.6\cdot 10^{-19})=3.2\cdot 10^{-19}C (charge of the helium nucleus is twice that of the proton)

r=100 \mu m = 100\cdot 10^{-6} m

So,

F_E=(9\cdot 10^9) \frac{(1.6\cdot 10^{-19})(3.2\cdot 10^{-19})}{(100\cdot 10^{-6})^2}=4.6\cdot 10^{-20}N

Therefore, we see that the electric force is much stronger than the gravitational force, by a factor of:

\frac{F_E}{F_G}=\frac{4.6\cdot 10^{-20}}{7.44\cdot 10^{-56}}=6.2\cdot 10^{35}

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Inga [223]
If the density of the object is lower than the density of the liquid it is floating in then it will float. if the density is larger it will sink. density is mass/volume
3 0
3 years ago
A force of 44 N will stretch a rubber band 88 cm ​(0.080.08 ​m). Assuming that​ Hooke's law​ applies, how far will aa 11​-N forc
Setler79 [48]

Answer:

<em>The rubber band will be stretched 0.02 m.</em>

<em>The work done in stretching is 0.11 J.</em>

Explanation:

Force 1 = 44 N

extension of rubber band = 0.080 m

Force 2 = 11 N

extension = ?

According to Hooke's Law, force applied is proportional to the extension provided elastic limit is not extended.

F = ke

where k = constant of elasticity

e = extension of the material

F = force applied.

For the first case,

44 = 0.080K

K = 44/0.080 = 550 N/m

For the second situation involving the same rubber band

Force = 11 N

e = 550 N/m

11 = 550e

extension e = 11/550 = <em>0.02 m</em>

<em>The work done to stretch the rubber band this far is equal to the potential energy stored within the rubber due to the stretch</em>. This is in line with energy conservation.

potential energy stored = \frac{1}{2}ke^{2}

==> \frac{1}{2}* 550* 0.02^{2} = <em>0.11 J</em>

3 0
3 years ago
A piston–cylinder device initially contains steam at 3.5 MPa, superheated by 5°C. Now, steam loses heat to the surroundings and
velikii [3]

<u>Answer :</u>

(a) The Initial temperature of the steam is 247.557°C

(b) The enthalpy change per unit mass of the steam is -1771 kJ/kg

(c) The final pressure is 1555 kPa, and the liquid vapor mixture contains small mass of vapor.

<u>Explanation :</u>

From the given statements, we know

Initial steam pressure (P_1) = 3.5 MPa

Degree of Super heat = 5°C

Saturation Temperature (T_s_a_t) = 242.557°C [From Steam Table]

Now, the Initial temperature (T_1) of steam is given by-

T_1 = T_s_a_t + Degree of Superheat

 = 242.557 + 5 = 247.557°C

(b)To find: The enthalpy change per unit mass of the steam is  

We know enthalpy (h) change is given by

Δh = h_2 – h_1

From steam Table, properties of the gas at state 1 and state 2  

h_1 = 2821.1 kJ/kg

h_2 = 1049.7 kJ/kg

On substituting the values, we get

or, Δh = 1049.7 - 2821.1 = -1771 kJ/kg

(c) To Find: The final pressure of the liquid vapor mixture contains small mass of vapor.

We find that the gas at the final position, i.e., at position 3

Final Temperature (T_3) = 200°C [Given] ……………………………..(1)

Specific Volume (v_3) = Specific Volume (v_2) = 0.00123 m^3/kg ….....(2)

Using steam table for corresponding values of (1) and (2), we get

Final Pressure P_3 = 1555 kPa

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6 0
3 years ago
An infinite long straight wire is uniformly charged, the charge density is a. Use Coulomb's law to calculate the electric field
bixtya [17]

Answer:

\vec{E} = \frac{a}{2\pi \epsilon_0 R}\^R

Explanation:

Since the wire is infinitely long, we will use Gauss' Law:

\int\vec{E}d\vec{a} = \frac{Q_{enc}}{\epsilon_0}

We will draw an imaginary cylindrical surface with height h around the wire. The electric flux through the imaginary surface will be equal to the net charge inside the surface.

In that case, the net charge inside the imaginary surface will be the portion of wire with height h. Then the charge of that portion will be equal to

Q_{enc} = ah

The left-hand side of the Gauss' Law is the flux through the imaginary surface. Since we choose our surface as a cylinder, of which we know the area, we do not have to take the surface integral.

\int\vec{E}d\vec{a} = E2\pi R h

where R is the radius of the imaginary cylinder.

Finally, Gauss' Law gives

E2\pi Rh = \frac{ah}{\epsilon_0}\\E = \frac{a}{2\pi \epsilon_0 R}

The vector expression is

\vec{E} = \frac{a}{2\pi \epsilon_0 R}\^R

As you can see, the electric field is independent from the height h, since that is merely an imaginary cylinder to apply Gauss' Law. In the end, what matters is the charge density of the wire and the distance from the wire.

4 0
4 years ago
Problem: The frequency of an FM radio station is 89.3 MHz. Calculate its period. Part B: From the Library, select the general eq
vekshin1

Answer:

Time period, T=1.11\times 10^{-8}\ s

Explanation:

We have,

The frequency of an FM radio station is 89.3 MHz.

It is required to find the period of the wave.

The reciprocal of frequency is called time period of a wave. It can be given by :

T=\dfrac{1}{f}\\\\T=\dfrac{1}{89.3\times 10^{6}\ Hz}\\\\T=1.11\times 10^{-8}\ s

So, the period of the wave is 1.11\times 10^{-8}\ s.

5 0
3 years ago
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