A charge of #-2 C# is at the origin. How much energy would be applied to or released from a # 4 C# charge if it is moved from # (-7 ,1 ) # to #(4 ,-6 ) #?

Answer 1

#197# #MJ# of energy is released.

Electrostatic Potential Energy: The electrostatic potential energy of a charge pair #Q# and #q# separated by a distance #r# is :
#U(r) = -k(Qq)/r; \qquad k \equiv 1/(4\pi\epsilon_0) = 8.99\times10^9 (N.m^2)/C^2#
Assuming that the units of the coordinates are in meters. #r_i = \sqrt{(-7m)^2+(1m)^2} = \sqrt{50}# #m = 7.071# #m# #r_f = \sqrt{(4m)^2+(-6m)^2} = 7.211# #m#
#\Delta U = U_f - U_i = -kQq(1/r_f - 1/r_i)# #= -(8.99\times10^9 (Nm^2)/C^2)(-2C)(4C)(1/(7.211m) - 1/(7.071m))#
#= - 197# #MJ#

A negative change in potential energy indicates a decrease in potential energy, which releases the energy.

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Answer 2

The energy applied to or released from a 4 C charge when moved from (-7, 1) to (4, -6) due to the presence of a -2 C charge at the origin can be calculated using the formula for electric potential energy:

U = k * (q1 * q2) / r

Where: U is the electric potential energy k is Coulomb's constant (8.99 × 10^9 N m²/C²) q1 and q2 are the charges (in coulombs) r is the distance between the charges (in meters)

First, we need to calculate the distance between the two charges using the distance formula:

Distance = √((x2 - x1)² + (y2 - y1)²)

Plugging in the coordinates, we get:

Distance = √((4 - (-7))² + ((-6) - 1)²) = √(11² + (-7)²) = √(121 + 49) = √170

Now, we can calculate the energy:

U = (8.99 × 10^9 N m²/C²) * ((-2 C) * (4 C)) / (√170 m) U ≈ -9.59 × 10^8 J

The negative sign indicates that energy is released from the 4 C charge as it moves from (-7, 1) to (4, -6) in the presence of the -2 C charge at the origin.

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Answer from HIX Tutor

When evaluating a one-sided limit, you need to be careful when a quantity is approaching zero since its sign is different depending on which way it is approaching zero from. Let us look at some examples.

When evaluating a one-sided limit, you need to be careful when a quantity is approaching zero since its sign is different depending on which way it is approaching zero from. Let us look at some examples.

When evaluating a one-sided limit, you need to be careful when a quantity is approaching zero since its sign is different depending on which way it is approaching zero from. Let us look at some examples.

When evaluating a one-sided limit, you need to be careful when a quantity is approaching zero since its sign is different depending on which way it is approaching zero from. Let us look at some examples.

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