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Genrish500 [490]
4 years ago
11

A copper wire has a circular cross section with a radius of 1.50 mm. (a) If the wire carries a current of 2.60 A, find the drift

speed of the electrons in the wire. (Assume the density of charge carriers (electrons) in a copper wire is n = 8.46 1028 electrons/m3.) m/s (b) All other things being equal, what happens to the drift speed in wires made of metal having a larger number of conduction electrons per atom than copper? Explain.
Physics
1 answer:
AleksAgata [21]4 years ago
5 0

Answer:

Part a)

v_d = 2.72 \times 10^{-5} m/s

Part b)

it is inversely depends on the number density so on increasing the number density the drift speed will decrease

Explanation:

Part a)

As we know that the cross-sectional radius is

r = 1.50 mm

now we will have

A = \pi r^2

A = \pi(1.50 \times 10^{-3})^2

A = 7.07 \times 10^{-6} m^2

now we know that

i = neA v_d

so we will plug in all data

2.60 = (8.46 \times 10^{28})(1.6 \times 10^{-19})(7.07\times 10^{-6})v_d

v_d = 2.72 \times 10^{-5} m/s

Part b)

As we know that

i = neAv_d

now if all other things are same

v_d = \frac{i}{neA}

since it is inversely depends on the number density so on increasing the number density the drift speed will decrease

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An earthquake P wave traveling at 7.7km/s strikes a boundary within the Earth between two kinds of material.If it approaches the
Aloiza [94]

Answer:

c_2 = 6.04\ Km/s

Explanation:

given,

speed of wave, c₁ = 7.7 m/s

angle of incidence, i = 44°

angle of refraction, r = 33°

speed of wave in second medium.

using Snell's law

  n₁ sin i = n₂ sin r

\dfrac{n_1}{n_2}=\dfrac{sin\ r}{sin\ i}

\dfrac{n_1}{n_2}=\dfrac{sin\ 33^0}{sin\ 44^0}

\dfrac{n_1}{n_2}=0.784

now,

calculation of velocity in the medium

n₁ c₁ = n₂ c₂

\dfrac{n_1}{n_2}=\dfrac{c_2}{c_1}

c_2 = c_1\times \dfrac{n_1}{n_2}

c_2 = 7.7\times 0.784

c_2 = 6.04\ Km/s

Speed of wave in the second medium is equal to 6.04 Km/h

6 0
3 years ago
4 points
zubka84 [21]

(a) 25lx

(b) 11.11lx

<u>Explanation:</u>

Illuminance is inversely proportional to the square of the distance.

So,

I = k\frac{1}{r^2}

where, k is a constant

So,

(a)

If I = 100lx and r₂ = 2r Then,

I_2 = k\frac{1}{(2r)^2}

Dividing both the equation we get

\frac{I_1}{I_2} = \frac{k}{r^2} X\frac{(2r)^2}{k} \\\\\frac{I_1}{I_2} = 4\\\\I_2 = \frac{I_1}{4}\\\\I_2 = \frac{100}{4}  = 25lx

When the distance is doubled then the illumination reduces by one- fourth and becomes 25lx

(b)

If I = 100lx and r₂ = 3r Then,

I_2 = k\frac{1}{(3r)^2}

Dividing equation 1 and 3 we get

\frac{I_1}{I_2} = \frac{k}{r^2} X\frac{(3r)^2}{k} \\\\\frac{I_1}{I_2} = 9\\\\I_2 = \frac{I_1}{9}\\\\I_2 = \frac{100}{9}  = 11.11lx

When the distance is tripled then the illumination reduces by one- ninth and becomes 11.11lx

3 0
3 years ago
Corresponde al conjunto de puntos por donde pasa un cuerpo al moverse
Anna35 [415]

Answer:

Means?

Explanation:

6 0
3 years ago
At a particular instant the magnitude of the momentum of a planet is 2.60 × 10^29 kg·m/s, and the force exerted on it by the sta
aleksley [76]

Answer:

F=(-4.8*10^22,0,0) N

Explanation:

<u>Given  :</u>

We are given the magnitude of the momentum of the planet and let us call this momentum (p_now) and it is given by p_now = 2.60 × 10^29 kg·m/s. Also, we are given the force exerted on the planet F = 8.5 × 10^22 N. and the angle between the planet and the star is Ф = 138°

Solution :

We are asked to find the parallel component of the force F The momentum here is not constant, where the planet moving along a curving path with varying speed where the rate change in momentum and the force may be varying in magnitude and direction. We divide the force here into two parts: a parallel force F to the momentum and a perpendicular force F' to the momentum.  

The parallel force exerted to the momentum will speed or reduce the velocity of the planet and does not change its moving line. Let us apply the direction cosines, we could obtain the parallel force as next  

F=|F|cosФp            (1)

Where the parallel force F is in the opposite direction of p as the angle between them is larger than 90°. Now we can plug our values for 0 and I F I into equation (1) to get the parallel force to the planet  

F=|F|cosФp

 =-4.8*10^22 N*p

<em>As this force is in one direction, we could get its vector as next  </em>

F=(-4.8*10^22,0,0) N

F=(0,-4.8*10^22,0) N

F=(0,0-4.8*10^22) N

The cosine of 138°, the angle between F and p is, is a negative number, so F is opposite to p. The magnitude of the planet's momentum will decrease.

8 0
3 years ago
An angler experiences a glare of light coming from the water's surface. Which type of glasses should she wear to minimize the gl
Vaselesa [24]
The glasses that she should wear are the glasses that block horizontally polarized light coming from glares, like polaroid sunglasses, because these type of glasses block out the light being reflected from the water's surface by the vertically oriented polarizers in the lenses. 
6 0
3 years ago
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