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marysya [2.9K]
4 years ago
9

A charge Q creates an electric field. A test charge q is usedto measure the strength of the electric field at a distance d from

Q. The electric field strength is defined as ____
Physics
1 answer:
ki77a [65]4 years ago
4 0

Answer:

E=\frac{1}{4\pi.\epsilon_o} \times \frac{Q}{ d^2}

Explanation:

In the given question we have a test charge q at a distance of d from form another charge Q which creates the field.

The electric field strength is force force per unit test charge, according to the Coulomb's law the force between two charges is given as:

F=\frac{1}{4\pi.\epsilon_0} \times \frac{Q.q}{d^2}

where:

\epsilon_0= permittivity of free space

Therefore,

E=\frac{F}{q}

E=\frac{1}{4\pi.\epsilon_o} \times \frac{Q}{ d^2}

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A speeding car is pulling away from a police car. The police car is moving at 30 m/s. The radar gun in the police car emits an e
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Answer:

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F=20\times 10^9 Hz

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v=\frac{\Delta F}{2F}\times c\\\Rightarrow v=\frac{4750}{2\times 20\times 10^9}\times 3\times 10^8\\\Rightarrow v=35.625\ m/s

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⇒Velocity of speeder = 30 + 35.625 = 65.625 m/s

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Answer:

d. all of the above

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An "ideal" banking angle assumes no friction is required to keep a car on the road as it turns. Let <em>θ</em> denote the banking angle, and consult the attached free-body diagram for a car making the turn. There are only 2 relevant forces acting on the car,

• the normal force with magnitude <em>n</em>

• the car's weight with magnitude <em>w</em>

and the net force points toward the center of the circle made by the turn, with centripetal acceleration

<em>a</em> = (125 km/h)² / (2.00 km) = 7812.5 km/h² ≈ 0.603 m/s²

Split up the forces into components acting perpendicular (⟂) and parallel (//) to the banked curve, so that by Newton's second law,

∑ <em>F</em> (⟂) = <em>N</em> + <em>W</em> (⟂) = <em>m</em> <em>a</em> (⟂)

and

∑ <em>F</em> (//) = <em>W</em> (//) = <em>m a</em> (//)

Let the direction of <em>N</em> be the positive perpendicular axis, and down the incline and toward the center of the circle the positive parallel axis. The net force vector and acceleration both make an angle <em>θ</em> with the banked curve, and <em>W</em> makes the same angle with the negative perpendicular axis, so that the equations above reduce to

<em>N</em> - <em>m g</em> cos(<em>θ</em>) = <em>m</em> <em>a</em> sin(<em>θ</em>)

and

<em>m g</em> sin(<em>θ</em>) = <em>m a</em> cos(<em>θ</em>)

The second equation is all we need at this point to find the ideal <em>θ</em>. The mass <em>m</em> cancels out, and we can solve for <em>θ</em> to get

tan(<em>θ</em>) = <em>a</em>/<em>g</em> ≈ (0.603 m/s²) / (9.80 m/s²) ≈ 0.0615

→   <em>θ</em> ≈ 3.52°

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