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Anuta_ua
1 month ago
15

The magnitude J(r) of the current density in a certain cylindrical wire is given as a function of radial distance from the cente

r of the wire's cross section as J(r) = Br, where r is in meters, J is in amperes per square meter, and B = 2.35 ✕ 105 A/m3. This function applies out to the wire's radius of 2.00 mm. How much current is contained within the width of a thin ring concentric with the wire if the ring has a radial width of 11.5 μm and is at a radial distance of 1.20 mm?
Physics
2 answers:
Softa [3K]1 month ago
7 0
J(r) = Br. We know that the area of a small segment, dA, is represented as 2 π dr. Thus, I = J A and dI = J dA. Plugging in the values gives us dI = B r. 2 π dr which simplifies to dI= 2π Br² dr. Now, integrating the above equation: Given that B= 2.35 x 10⁵ A/m³, with r₁ = 2 mm and r₂ equal to 2 + 0.0115 mm, or 2.0115 mm.
serg [3.5K]1 month ago
6 0
18.1 x 10^-6 A. A cylindrical wire exhibits a current density described as J(r) = Br. Given B = 2.35 x 10^5 A/m^3, the current across a specified area is calculated by multiplying the current density with that area. For a ring at a radial distance r, with an infinitesimal width of Δr, the area is given as A= 2rΔr, where 2r represents the circumference and Δr is the width. Therefore, we can express I=J(2rΔr) leading to I=2Br²Δr. Substituting the assigned values results in I= 2(2.35 x 10^5)(1.2 x 10^-3)^2(11.5 x 10^-6), yielding a result of 18.1 x 10^-6 A.
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The drawing shows an adiabatically isolated cylinder that is divided initially into two identical parts by an adiabatic partitio
Yuliya22 [3333]

Answer:

the temperature on the left side is 1.48 times greater than that on the right

Explanation:

GIVEN DATA:

\gamma = 5/3

T1 = 525 K

T2 = 275 K

It is known that

P_1 = \frac{nRT_1}{v}

P_2 = \frac{nrT_2}{v}

n and v are constant on both sides. Therefore we have

\frac{P_1}{P_2} = \frac{T_1}{T_2} = \frac{525}{275} = \frac{21}{11}

P_1 = \frac{21}{11} P_2..............1

let the final pressure be P and the temperature T_1 {f} and T_2 {f}

P_1^{1-\gamma} T_1^{\gamma} = P^{1 - \gamma}T_1 {f}^{\gamma}

P_1^{-2/3} T_1^{5/3} = P^{-2/3} T_1 {f}^{5/3}..................2

similarly

P_2^{-2/3} T_2^{5/3} = P^{-2/3} T_2 {f}^{5/3}.............3

divide equation (2) by equation (3)

\frac{21}{11}^{-2/3} \frac{21}{11}^{5/3} = [\frac{T_1 {f}}{T_2 {f}}]^{5/3}

T_1 {f} = 1.48 T_2 {f}

thus, the left side temperature equals 1.48 times the right side temperature

6 0
1 month ago
Derive an equation for the acceleration of block 3 for any arbitrary values of m3 and m2. Express your answer in terms of m3, m2
Ostrovityanka [3204]

The complete question is;

Block 1 sits on the floor with block 2 resting atop it. Block 3, which is stationary on a frictionless table, is attached to block 2 via a string that passes over a pulley depicted in the illustration below. Both the string and pulley have negligible mass.

Once block 1 is taken away without impacting block 2.

Derive an equation for the acceleration of block 3 considering arbitrary values for m3 and m2. Express your answer in terms of m3, m2, and relevant physical constants as needed.

Answer:

a = (m2)g/(m3 + m2)

Explanation:

Examining the attached illustration, by analyzing the free body diagram for block 3 and utilizing Newton's first law of motion, we reach the following formula;

T = (m3)a - - - (eq 1)

where;

T is the tension in the string

a is acceleration

m3 is the mass of block 3

Simultaneously, doing the same for Block 2, the free body diagram yields the equation; (m2)g - T = (m2)a

Rearranging for T results in;

T = (m2)g - (m2)a - - - (eq 2)

where;

g represents acceleration due to gravity

T is the tension in the string

a is acceleration

m2 is the mass of block 2

To deduce the acceleration, we will substitute (m3)a in place of T in eq 2.

Thus;

(m3)a = (m2)g - (m2)a

(m3)a + (m2)a = (m2)g

a(m3 + m2) = (m2)g

a = (m2)g/(m3 + m2)

3 0
28 days ago
Mosses don't spread by dispersing seeds; they disperse tiny spores. The spores are so small that they will stay aloft and move w
Keith_Richards [3271]

Solution:

Em_{f} / Em₀ = 0.30

Explanation:

In this problem, we apply the connection between mechanical energy, kinetic energy, and gravitational potential energy.

      K = ½ m v²

      U = mgh

We assess the mechanical energy at two positions:

Initial. Lower

    Em₀ = K = ½ m v²

At its highest point

    Em_{f} = U = mg and

Now let's compute

    Em₀ = ½ m 3.6²

    Em₀ = m 6.48

    Em_{f} = m 9.8 × 0.2

    Em_{f} = m 1.96

Thus the energy lost is given by:

    Em_{f} / Em₀ = m 1.96 / m 6.48

   Em_{f} / Em₀ = 0.30

This means that 30% of the sun's energy is transformed into potential energy.

There are various conversion possibilities.

This energy changes into thermal energy affecting the spores and air, since it cannot be regained.

8 0
2 months ago
A conducting sphere 45 cm in diameter carries an excess of charge, and no other charges are present. You measure the potential o
Maru [3345]

Answer:

The excess charge is Q = 3.5 *10^{-7} \ C

Explanation:

According to the question, we are informed that

The diameter is d = 45 \ cm = 0.45 \ m

The potential of the surface is V = 14 \ kV = 14 *10^{3} \ V

The radius of the sphere is

r = \frac{d}{2}

by plugging in given values

r = \frac{0.45}{2}

r = 0.225 \ m

The potential at the surface is mathematically expressed as

V = \frac{k * Q }{r }

Where k is Coulomb's constant with a value k = 9*10^{9} \ kg\cdot m^3\cdot s^{-4} \cdot A^{-2}.

Based on the question stating there are no other charges, Q represents the excess charge

Therefore

Q = \frac{V* r}{ k}

inserting the numerical values

Q = \frac{14 *10^{3} 0.225}{ 9*10^9}

Q = 3.5 *10^{-7} \ C

7 0
29 days ago
The energy gaps between the valence and conduction bands are called band gaps. For silicon, the band gap is 1.1 eV; for fused si
serg [3582]
I appreciate you bringing your question here. I trust this response will be beneficial. Don’t hesitate to reach out with additional queries.
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6 0
1 month ago
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