Two wires are made of the same material. The first wire dissipates power P with a current of I. If the second wire is 3 times as long and has twice the diameter, what will the current need to be through the second wire to dissipate the same power P as the first wire?

A particle enters a magnetic field with velocity v. Find the mass of the particle in terms of v, B, and x.

Using the idea of resistors in series and in parallel, we conclude that:

resistance is proportional to length, and
inversely proportional to the area.

That should be sufficient to solve the first problem.

To find the current needed through the second wire to dissipate the same power P as the first wire, we can use the formula for power dissipation in a wire:

P = I^2 * R

where P is the power, I is the current, and R is the resistance.

Since both wires are made of the same material, they have the same resistivity. The resistance of a wire is given by the formula:

R = (ρ * L) / A

where ρ is the resistivity, L is the length of the wire, and A is the cross-sectional area of the wire.

Let's assume the length and diameter of the first wire are L1 and D1, respectively. And let L2 and D2 be the length and diameter of the second wire.

Given that the second wire is 3 times as long as the first wire (L2 = 3L1) and has twice the diameter (D2 = 2D1), we can determine the cross-sectional area of the second wire:

A2 = π * (D2/2)^2 = π * (2D1/2)^2 = 4π * D1^2

Now, equating the power dissipation in both wires, we have:

I1^2 * R1 = I2^2 * R2

Substituting the resistance formula, we get:

I1^2 * (ρ * L1) / A1 = I2^2 * (ρ * L2) / A2

Since both wires have the same resistivity, this simplifies to:

I1^2 * L1 / A1 = I2^2 * L2 / A2

Substituting the values we have:

I1^2 * L1 / (π * D1^2) = I2^2 * L2 / (4π * D1^2)

Canceling out the common terms:

I1^2 * L1 = I2^2 * L2 / 4

Simplifying further:

I1^2 = (I2^2 * L2) / (4 * L1)

Finally, solving for I2, we get:

I2^2 = (I1^2 * 4 * L1) / L2

Taking the square root of both sides:

I2 = sqrt((I1^2 * 4 * L1) / L2)

So, the current needed through the second wire to dissipate the same power P as the first wire is sqrt((I1^2 * 4 * L1) / L2).

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To find the mass of a particle in terms of v (velocity), B (magnetic field), and x (the path of the particle), we can use the equation for the force experienced by a charged particle moving in a magnetic field:

F = q * v * B

where F is the force, q is the charge of the particle, v is the velocity, and B is the magnetic field.

The force experienced by the particle is equal to the rate of change of momentum, which is given by:

F = (dP) / dt

Since momentum is given by mass times velocity (P = m * v), we can rewrite the equation as:

(m * v) / dt = q * v * B

Canceling out the velocity term:

(m / dt) = q * B

Since dt represents a small change in time, we can rewrite it as dt = dx / v, where dx represents a small change in position.

Substituting this into the equation, we get:

(m / (dx / v)) = q * B

Simplifying, we have:

m = (q * B * dx) / v

Therefore, the mass of the particle in terms of v, B, and x is given by:

m = (q * B * dx) / v.