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Semenov [28]
3 years ago
10

A 3-mm-diameter electrical wire is insulated by a 2-mm-thick rubberized sheath with k = 0.13 W/m·K, and the wire/sheath interfac

e is characterized by a thermal contact resistance of R ’’ t,c=3 × 10−4 m2 ·K/W. The convection heat transfer coefficient at the outer surface of the sheath is 15 W/m2 ·K, and the ambient air temperature is 20°C. If the temperature of the sheath may not exceed 50°C, what is the maximum allowable electrical power that may be dissipated per unit length of the conductor? What is the critical radius of the insulating sheath?
Physics
1 answer:
Phoenix [80]3 years ago
4 0

Answer:

Q_{max} = 6,3928 W/m

Explanation:

The thermal resistances in this case act as series resistances, so to get the total resistance you need to add al resitances:

R_{tot}  = R_{contact} +  R_{conductive} +  R_{convective}

To get the contact resistence per unit length we have to multiply the contact resistance by the perimeter of the contact area:

P_{wire-sheath}  = \pi * 0,003m = 9,4248 * 10^{-3}  m

R_{contact} = \frac{3*10^{-4} m2 K/W}{9,4248 * 10^{-3}  m} = 0,03183 m K/W

For the conductive resistance on the sheath:

R_{conductive}  = \frac{thickness}{k*P_{wire-sheath}}  = \frac{ 0,002m}{9,4248 * 10^{-3}  m * 0,13 W/mK} = 1,63 mK/W

Convective resistance:

The perimeter of the auter surfice is:

P_{out-sheath}  = \pi * 0,007m = 2,199* 10^{-2}  m

R_{convective}  = \frac{1}{Convection coeficient * P_{out-sheath} }  = \frac{ 1}{15 W/m^{2}K * 2,199* 10^{-2}  m} = 3,031 mK/W

Total Resistance:

R_{tot} = 4,6928 mK/W

Heat transfer:

Q = dT/R_{tot}

dT = T_{wire} -  T_{amb} = 323 K - 293 K = 30 K

Q_{max} = \frac{30K}{4,6928 mK/W} = 6,3928 W/m

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Two tiny particles having charges of +5.00 μC and +7.00 μC are placed along the x-axis. The +5.00-µC particle is at x = 0.00 cm,
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Answer:

The third charged particle must be placed at x = 0.458 m = 45.8 cm

Explanation:

To solve this problem we apply Coulomb's law:  

Two point charges (q₁, q₂) separated by a distance (d) exert a mutual force (F) whose magnitude is determined by the following formula:  

F = \frac{k*q_1*q_2}{d^2} Formula (1)  

F: Electric force in Newtons (N)

K : Coulomb constant in N*m²/C²

q₁, q₂: Charges in Coulombs (C)  

d: distance between the charges in meters (m)

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1μC= 10⁻⁶C

1m = 100 cm

Data

K = 8.99 * 10⁹ N*m²/C²

q₁ = +5.00 μC = +5.00 * 10⁻⁶ C

q₂= +7.00 μC = +7.00 * 10⁻⁶ C

d₁ = x (m)

d₂ = 1-x (m)

Problem development

Look at the attached graphic.

We assume a positive charge q₃ so F₁₃ and F₂₃ are repulsive forces and must be equal so that the net force is zero:

We use formula (1) to calculate the forces F₁₃ and F₂₃

F_{13} = \frac{k*q_1*q_3}{d_1^2}

F_{23} = \frac{k*q_2*q_3}{d_2^2}

F₁₃ = F₂₃

\frac{k*q_1*q_3}{d_1^2} = \frac{k*q_2*q_3}{d_2^2} We eliminate k and q₃ on both sides

\frac{q_1}{d_1^2}= \frac{q_2}{d_2^2}

\frac{q_1}{x^2}=\frac{q_2}{(1-x)^2}

\frac{5*10^{-6}}{x^2}=\frac{7*10^{-6}}{(1-x)^2} We eliminate 10⁻⁶ on both sides

(1-x)^2 = \frac{7}{5} x^2

1-2x+x^2=\frac{7}{5} x^2

5-10x+5x^2=7 x^2

2x^2+10x-5=0

We solve the quadratic equation:

x_1 = \frac{-b+\sqrt{b^2-4ac} }{2a} = \frac{-10+\sqrt{10^2-4*2*(-5)} }{2*2} = 0.458m

x_2 = \frac{-b-\sqrt{b^2-4ac} }{2a} = \frac{-10-\sqrt{10^2-4*2*(-5)} }{2*2} = -5.458m

In the option x₂, F₁₃ and F₂₃ will go in the same direction and will not be canceled, therefore we take x₁ as the correct option since at that point the forces are in  opposite way .

x = 0.458m = 45.8cm

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Q 19.23: A proton is initially moving at 3.0 x 105 m/s. It moves 3.5 m in the direction of a uniform electric field of magnitude
DENIUS [597]

Answer:

The kinetic energy of the proton at the end of the motion is 1.425 x 10⁻¹⁶ J.

Explanation:

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initial velocity of proton, v_p_i = 3 x 10⁵ m/s

distance moved by the proton, d = 3.5 m

electric field strength, E = 120 N/C

The kinetic energy of the proton at the end of the motion is calculated as follows.

Consider work-energy theorem;

W = ΔK.E

W =K.E_f - K.E_i

where;

K.Ef is the final kinetic energy

W is work done in moving the proton = F x d  = (EQ) x d = EQd

K.E_f =EQd + \frac{1}{2}m_pv_p_i^2

m_p \ is \ mass \ of \ proton = 1.673 \ \times \ 10^{-27} kg \\\\Q \ is \ charge \ of \ proton = 1.6 \times 10^{-19} C

K.E_f = 120\times 1.6 \times 10^{-19} \times 3.5   \ + \ \frac{1}{2}(1.673\times 10^{-27})(3\times 10^5)^2 \\\\

K.E_f = 6.72\times 10^{-17} \ + \ 7.53 \times 10^{-17} \\\\K.E_f = 14.25 \times 10^{-17} J\\\\K.E_f = 1.425\times 10^{-16} \ J

Therefore, the kinetic energy of the proton at the end of the motion is 1.425 x 10⁻¹⁶ J.

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3 years ago
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