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mash [69]
3 years ago
13

In the following figure, electric field at y axis will be maximum at y=?

Physics
2 answers:
Strike441 [17]3 years ago
5 0

Because of symmetry electric field component in the x axis cancels out. Now just use electric field formula and slap that sine of theta cause you want the vertical component of electric field and multiply that by two since there’s two charges. I’ve shown my work. Hope it helps✌

Anton [14]3 years ago
3 0

Answer:

y = \frac{d}{\sqrt2}

Explanation:

As we know that electric field due to each charge at any given height y due to the point charges is given by

E = \frac{kq}{d^2 + y^2}

now we know that horizontal component of electric field due to each charge will cancel out while vertical component will be added due to both

So here we can say

E_{net} = \frac{kqy}{(d^2 + y^2)^{3/2}}

now we know that for maximum value of Electric field

\frac{dE}{dy} = 0

after solving this we will have

y = \frac{d}{\sqrt2}

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Two wires of the same material and having the same volume, are fixed
Setler79 [48]

Answer:

48 kg

Explanation:

Given that the two wires are of same material, so their value of young's modulus will be same

Assuming that the wires are cylindrical in shape

As radius of the first wire is half that of the second wire and therefore the area of cross-section of the first wire will be one-fourth of the second wire( ∵ wire is cylindrical, the cross-sectional part will be circle and the area of the circle = π × r² )

As the volume is same for both wires

∴ π × (r_{1})² × l_{1} = π × (r_{2})² × l_{2}

Here

r_{1} is the radius of the first wire

r_{2} is the radius of the second wire

l_{1} is the length of the first wire

l_{2} is the length of the second wire

⇒ π × ((r_{2})² ÷ 4) × l_{1} = π × (r_{2})² × l_{2} (∵ radius of first wire is half that of the second wire)

By cancelling the same terms on both sides

we get

l_{1} = 4 × l_{2}

⇒ Length of first wire will be four times of the length of second wire

<h3>Strain is defined as the elongation per unit length</h3>

Strain in first wire = ΔL ÷ l_{1} = ΔL ÷ (4 × l_{2})

where ΔL is the elongation of the wire which in this case is same in both wires

Strain in second wire = ΔL ÷ l_{2}

∴ Strain in second wire is four times of strain in first wire

<h3>Stress = F ÷ A</h3>

where F is the force perpendicular to the cross-sectional area

A is the area of cross-section

Force in first wire = m_{1} × g

where m_{1} is the mass hanged to the first wire

g is the acceleration due to gravity

Force in second wire = m_{2} × g

where m_{2} is the mass hanged to the second wire

g is the acceleration due to gravity

Let A_{1} be the cross-sectional area of first wire

A_{2} be the cross-sectional area of second wire

A_{2} = 4 × A_{1} (∵ cross=sectional area of the wire = π × (radius of the wire)² )

Stress in first wire = (m_{1} × g) ÷ (A_{1})

Stress in second wire = (m_{2} × g) ÷ (A_{2}) = (m_{2} × g) ÷ (4 × A_{1})

<h3>Young's modulus is defined as Stress per unit strain</h3>

As Young's modulus is same for both wires, Stress per unit strain must be same for both wires

Stress per unit strain of first wire = ((m_{1} × g) ÷ (A_{1})) ÷ (ΔL ÷ (4 × l_{2}))

Stress per unit strain of second wire = ((m_{2} × g) ÷ (4 × A_{1})) ÷ (ΔL ÷ l_{2})

By equating them we get

m_{2} = 16 × m_{1}

⇒ m_{2} = 16 × 3 = 48 kg

∴ m_{2} = 48 kg

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