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Advocard [28]
3 years ago
6

. Point charges q1 = q2 = 4.0 × 10−6 C are fixed on the x-axis at x = −3.0 m and x = 3.0 m. What charge q must be placed at the

origin so that the electric field vanishes at x = 0, y = 3.0 m?

Physics
1 answer:
mezya [45]3 years ago
5 0

Answer:

q_3=-2.83\cdot 10^{-6}\ c

Explanation:

<u>Electric Field</u>

The total electric field is the sum of all the individual electric fields produced by each charge. Please refer to the image below. The charges q1 and q2 produce the electric fields shown in the point (0,3). Since both charges are equal in magnitude and sign and are at the same distance from the point, the horizontal component of their electric fields cancel each other, only the vertical component remains and it's directed upwards.

The third charge q3 must be negative, so the total electric field is zero. Let's first compute the value of the angle \theta by analyzing the distances in the right triangle formed by the charges q1, q2, and the point (0,3)

\displaystyle tan\theta=\frac{3}{3}=1

It follows that \theta=45^o

The distance from q1 (or q2) to the point (0,3) is computed by

d^2=3^2+3^2=18\ m^2

Let's compute the magnitude of the electric of q1 or q2:

\displaystyle E=\frac{Kq_1}{d^2}=\frac{Kq_2}{d^2}

\displaystyle E=\frac{9\cdot 10^9\times 4\cdot  10^{-6}}{18}

E=2000\ N/c

The vertical component of both fields is given by

Ey=2000cos45^o=1414.21

The total field produced by q1 and q2 is twice that quantity

E_{yt}=2828.42\ N/c

That should be the value of E3 to make the total field vanish (equal to 0)

\displaystyle E_3=\frac{Kq_3}{d_3^2}=2828.42

Solving for q3

\displaystyle q_3=\frac{2828.42\cdot d_3^2}{K}=\frac{2828.42\cdot 3^2}{9\cdot 10^9}

\boxed{ q_3=-2.83\cdot 10^{-6}\ c}

We had already established the sign of q3 must be negative

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lora16 [44]

Answer:

D &B

Explanation:

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3 years ago
Write two examples of machine which changes the direction of force​
Ostrovityanka [42]

Answer:

Washign machine and swingset

Explanation:

4 0
2 years ago
If the window is 11 m above the ground, find the time the stone is in flight.
rjkz [21]
d=vi*t+(1/2)gt²

d=11 m
g=9.8 m/s²
vi=0 m/s

11 m=0 m/s*t+(1/2)9.8 m/s²t²
11 m=4.9 m/s²t²
t²=11 m / 4.9 m/s²
t=√(11 m / 4.9 m/s²)=1.489... s≈1.5 s

Answer: the time the sone is in flight is 1.5 s
5 0
3 years ago
To practice problem-solving strategy 22.1: gauss's law. an infinite cylindrical rod has a uniform volume charge density ρ (where
BabaBlast [244]

Let say the point is inside the cylinder

then as per Gauss' law we have

\int E.dA = \frac{q}{\epcilon_0}

here q = charge inside the gaussian surface.

Now if our point is inside the cylinder then we can say that gaussian surface has charge less than total charge.

we will calculate the charge first which is given as

q = \int \rho dV

q = \rho * \pi r^2 *L

now using the equation of Gauss law we will have

\int E.dA = \frac{\rho * \pi r^2* L}{\epcilon_0}

E. 2\pi r L = \frac{\rho * \pi r^2* L}{\epcilon_0}

now we will have

E = \frac{\rho r}{2 \epcilon_0}

Now if we have a situation that the point lies outside the cylinder

we will calculate the charge first which is given as it is now the total charge of the cylinder

q = \int \rho dV

q = \rho * \pi r_0^2 *L

now using the equation of Gauss law we will have

\int E.dA = \frac{\rho * \pi r_0^2* L}{\epcilon_0}

E. 2\pi r L = \frac{\rho * \pi r_0^2* L}{\epcilon_0}

now we will have

E = \frac{\rho r_0^2}{2 \epcilon_0 r}


7 0
3 years ago
A 78−kg skier is sliding down a ski slope at a constant velocity. The slope makes an angle of 21° above the horizontal direction
Feliz [49]

Answer:

274N 0.41

Explanation:

As he is sliding down in a constant speed then the force that accelerates him (weight) and the force that slows his down (friction) are equal.

then

<em>friction=mass x gravity x sin(21)</em>

Fr=78kg x 9.8m/s2 x sin(21)=274N

<em>friction= coefficient of kinetic friction x normal force of from the slope</em>

Fr= u x 78kg x 9.8m/s2 x cos(21)=274N

Fr= u x 78kg x 9.8m/s2 x cos(21)=274Nu=274/677=0.41

8 0
3 years ago
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