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Stells [14]
2 years ago
9

The drawing shows an end-on view of three wires. They are long, straight, and perpendicular to the plane of the paper. Their cro

ss-sections lie at the corners of a square. The currents in wires 1 and 2 are ????1 = ????2 = ???? and are directed into the paper. What is the direction of the current in wire 3, and what is the ratio ????3⁄????, so that the net magnetic field at the empty corner is zero?
Physics
1 answer:
notka56 [123]2 years ago
8 0

Answer:

l3/l = 2

Explanation:

Suppose B1 is the magnetic field due to cable 1 and B2 is the field due to cable 2. Therefore, the magnitude of the field at a distance from the cable is equal to:

B = (uo*I)/(2*pi*r)

B1-2 = (B1^2 + B2^2)^1/2 = ((((uo*I)/(2*pi*r)^2 + (uo*I)/(2*pi*r)^2))))))^1/2 = (2^1/2)*(uo*l)/(2*pi*r)

From this equation we can say that the direction of the field will be from the corner that is empty and cable 3:

B3 = B1-2

(uo*l3)/(2*pi*(2^1/2)*r = (2^1/2)*(uo*l)/(2*pi*r)

From here we have that the relationship between both currents will be equal to:

l3/l = 2

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The Role of Heat Transfer Methods in the Distribution of Earth's Energy

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A confused dragonfly flies forward and backward in a straight line. Its motion is shown on the following graph of horizontal pos
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2 years ago
A compact, dense object with a mass of 2.90 kg is attached to a spring and is able to oscillate horizontally with negligible fri
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(a) 80 N/m

The spring constant can be found by using Hooke's law:

F=kx

where

F is the force on the spring

k is the spring constant

x is the displacement of the spring relative to the equilibrium position

At the beginning, we have

F = 16.0 N is the force applied

x = 0.200 m is the displacement from the equilibrium position

Solving the formula for k, we find

k=\frac{F}{m}=\frac{16.0 N}{0.200 m}=80 N/m

(b) 0.84 Hz

The frequency of oscillation of the system is given by

f=\frac{1}{2\pi}\sqrt{\frac{k}{m}}

where

k = 80 N/m is the spring constant

m = 2.90 kg is the mass attached to the spring

Substituting the numbers into the formula, we find

f=\frac{1}{2\pi}\sqrt{\frac{80 N/m}{2.90 kg}}=0.84 Hz

(c) 1.05 m/s

The maximum speed of a spring-mass system is given by

v=\omega A

where

\omega is the angular frequency

A is the amplitude of the motion

For this system, we have

\omega=2\pi f=2\pi (0.84 Hz)=5.25 rad/s

A=0.200 m (the amplitude corresponds to the maximum displacement, so it is equal to the initial displacement)

Substituting into the formula, we find the maximum speed:

v=(5.25 rad/s)(0.200 m)=1.05 m/s

(d) x = 0

The maximum speed in a simple harmonic motion occurs at the equilibrium position. In fact, the total mechanical energy of the system is equal to the sum of the elastic potential energy (U) and the kinetic energy (K):

E=U+K=\frac{1}{2}kx^2+\frac{1}{2}mv^2

where

k is the spring constant

x is the displacement

m is the mass

v is the speed

The mechanical energy E is constant: this means that when U increases, K decreases, and viceversa. Therefore, the maximum kinetic energy (and so the maximum speed) will occur when the elastic potential energy is minimum (zero), and this occurs when x=0.

(e) 5.51 m/s^2

In a simple harmonic motion, the maximum acceleration is given by

a=\omega^2 A

Using the numbers we calculated in part c):

\omega=2\pi f=2\pi (0.84 Hz)=5.25 rad/s

A=0.200 m

we find immediately the maximum acceleration:

a=(5.25 rad/s)^2(0.200 m)=5.51 m/s^2

(f) At the position of maximum displacement: x=\pm 0.200 m

According to Newton's second law, the acceleration is directly proportional to the force on the mass:

a=\frac{F}{m}

this means that the acceleration will be maximum when the force is maximum.

However, the force is given by Hooke's law:

F=kx

so, the force is maximum when the displacement x is maximum: so, the maximum acceleration occurs at the position of maximum displacement.

(g) 1.60 J

The total mechanical energy of the system can be found by calculating the kinetic energy of the system at the equilibrium position, where x=0 and so the elastic potential energy U is zero. So we have

E=K=\frac{1}{2}mv_{max}^2

where

m = 2.90 kg is the mass

v_{max}=1.05 m/s is the maximum speed

Solving for E, we find

E=\frac{1}{2}(2.90 kg)(1.05 m/s)^2=1.60 J

(h) 0.99 m/s

When the position is equal to 1/3 of the maximum displacement, we have

x=\frac{1}{3}(0.200 m)=0.0667 m

so the elastic potential energy is

U=\frac{1}{2}kx^2=\frac{1}{2}(80 N/m)(0.0667 m)^2=0.18 J

and since the total energy E = 1.60 J is conserved, the kinetic energy is

K=E-U=1.60 J-0.18 J=1.42 J

And from the relationship between kinetic energy and speed, we can find the speed of the system:

v=\sqrt{\frac{2K}{m}}=\sqrt{\frac{2(1.42 J)}{2.90 kg}}=0.99 m/s

(i) 1.84 m/s^2

When the position is equal to 1/3 of the maximum displacement, we have

x=\frac{1}{3}(0.200 m)=0.0667 m

So the restoring force exerted by the spring on the mass is

F=kx=(80 N/m)(0.0667 m)=5.34 N

And so, we can calculate the acceleration by using Newton's second law:

a=\frac{F}{m}=\frac{5.34 N}{2.90 kg}=1.84 m/s^2

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A truck collides with a car on horizontal ground. At one moment during the collision, the magnitude of the acceleration of the t
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Answer:

The magnitude of the acceleration of the car is 35.53 m/s²

Explanation:

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acceleration of the truck, a_t = 12.7 m/s²

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mass of the car, m_c = 890 kg

let the acceleration of the car at the moment they collided = a_c

Apply Newton's third law of motion;

Magnitude of force exerted by the truck = Magnitude of force exerted by the car.

The force exerted by the car occurs in the opposite direction.

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