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Phoenix [80]
3 years ago
7

A water molecule perpendicular to an electric field has 1.40×10−21 J more potential energy than a water molecule aligned with th

e field. The dipole moment of a water molecule is 6.2×10−30Cm.
What is the strength of the electric field?
Express your answer with the appropriate units.
Physics
1 answer:
vesna_86 [32]3 years ago
3 0

Answer:

The strength of the electric field is 2.258 x 10⁸ N/C

Explanation:

Potential energy = -p*ECosθ

where;

d is the dipole moment

E is the electric field  

θ is the angle of inclination

→When the water molecules is perpendicular to the field, θ =90° and potential energy = p*ECosθ = d*ECos0 = 0

Total potential energy = 0 + 1.40×10⁻²¹J, since it is 1.40×10⁻²¹J more

→When the water molecules is aligned to the field, θ =0°

potential energy = -p*ECosθ

dipole moment, p = 6.2×10⁻³⁰Cm

                            = -(6.2×10⁻³⁰)*(E) Cos0

0 + 1.40×10⁻²¹ J = -(6.2×10⁻³⁰)*(E),

E = (1.40×10⁻²¹ J)/(6.2×10⁻³⁰)

E = 2.258 x 10⁸ N/C

Therefore, the strength of the electric field is 2.258 x 10⁸ N/C

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Answer:

ΔQ = 0.1 kJ

\mathbf{v_f = 1.445*10^{-3}  m^3}

\mathbf{P_f = 156.5 \ kPa}

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The value negative is due to the fact that there is need to be the same amount of positive change in surrounding as a result of compression.

Explanation:

GIven that:

Diameter of the piston-cylinder = 12 cm

Pressure of the piston-cylinder = 100 kPa

Temperature =24 °C

Length of the piston = 20 cm

Boundary work ΔW = 0.1 kJ

The gas is compressed and The temperature of the gas remains constant during this process.

We are to find ;

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According to the first law of thermodynamics ;

ΔQ = ΔU + ΔW

Given that the temperature of the gas remains constant during this process; the isothermal process at this condition ΔU = 0.

Now

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ΔQ = 0.1 kJ

Thus; the amount of heat that was transferred to/from the gas is : 0.1 kJ

b. What is the final volume and pressure in the cylinder?

In an isothermal process;

Workdone W = \int dW

W = \int pdV \\ \\ \\W = \int \dfrac{nRT}{V}dv \\ \\ \\ W = nRt \int  \dfrac{dv}{V}  \\ \\ \\ W  = nRT In V |^{V_f} __{V_i}}  \\ \\ \\ W = nRT \ In \dfrac{V_f}{V_i}

Since the gas is compressed ; then v_f< v_i

However;

W =- nRT \ In \dfrac{V_f}{V_i}

W =- P_1V_1  \ In \dfrac{V_f}{V_i}

The initial volume for the cylinder is calculated as ;

v_1 = \pi r^2 h \\ \\   v_1 = \pi r^2 L \\ \\ v_1 = 3.14*(6*10^{-2})^2*(20*10^{-2}) \\ \\ v_1 = 2.261*10^{-3} \ m^3

Replacing over values into the above equation; we have :

100 =  - ( 100*10^3 *2.261*10^{_3}) In (\dfrac{v_f}{v_i}) \\ \\ - In (\dfrac{v_f}{v_i})= \dfrac{100}{(100*10^3*2.261*10^{-3})} \\ \\ - In \ v_f  + In \  v_i = \dfrac{100}{226.1} \\ \\   - In \ v_f  = - In \ v_i + \dfrac{100}{226.1}  \\ \\  - In \ v_f  = - In (2.261*10^{-3} + \dfrac{100}{226.1 } \\ \\  - In \ v_f  = 6.1 + 0.44 \\ \\  - In \ v_f  = 6.54 \\ \\  - In \ v_f  = -6.54 \\ \\ v_f = e^{-6.54} \\ \\ \mathbf{v_f = 1.445*10^{-3}  m^3}

The final pressure can be calculated by using :

P_1V_1 = P_2V_2 \\ \\ P_iV_i = P_fV_f

P_f =\dfrac{P_iV_i}{V_f}

P_f =\dfrac{100*2.261*10^{-3}}{1.445*10^{-3}}

P_f = 1.565*10^2 \ kPa

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c. Find the change in entropy of the gas. Why is this value negative if entropy always increases in actual processes?

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\Delta S=\dfrac{\Delta Q}{T}

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T =  24 °C = (24+273)K

T = 297 K

\Delta S=\dfrac{-100 \ J}{297 \ K}

ΔS = -0.337 J/K

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t=\dfrac{L}{v}\\\Rightarrow t=\dfrac{90}{343}\\\Rightarrow t=0.262390670554\ s

The time interval is 0.262390670554-0.0879772697913=0.174413400763\ s

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