Two charges of # 2 C # and # 8 C# are positioned on a line at points # -3 # and # 6 #, respectively. What is the net force on a charge of # -3 C# at # -2 #?

Answer 1

#Delta F=50,625*10^9*C^2#


#F=k*(q_1*q_2)/d^2 #
# F: "Force between two charges acting each other"#
#q_1,q_2: "charges" #
#d:"distance between two charges"#

#step:1#
#color(red)(F_(AB))=k*(q_A*q_B)/(d_(AB)^2#
#color(red)(F_(AB))=9*10^9(2C*(-3C))/1^2#
#color(red)(F_(AB))=-54*C^2*10^9#

#step:2#
#color(blue)(F_(CB))=k*(q_C*q_B)/(d_(CB)^2#
#color(blue)(F_(CB))=9*10^9(cancel(8)C*(-3C))/cancel(8)^2#
#color(blue)(F_(CB))=-27*10^9*C^2/8#
#color(blue)(F_(CB))=-3,375*10^9*C^2#

#step:3#
#Delta F=color(blue)(F_(CB))-color(red)(F_(AB))#
#Delta F=-3,375*10^9*C^2-(-54*10^9*C²)#
#Delta F=-3,375*10^9*C^2+54*10^9*C^2#
#Delta F=50,625*10^9*C^2#

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Answer 2

To calculate the net force on the charge of -3 C at -2, we use Coulomb's law, which states that the force between two charges is directly proportional to the product of their magnitudes and inversely proportional to the square of the distance between them. The net force is the vector sum of the forces due to each charge.

First, we calculate the force due to the 2 C charge at -3:
F1=kq1qr12F_1 = \frac{k \cdot |q_1 \cdot q|}{r_1^2}
F1=(9×10923)1F_1 = \frac{(9 \times 10^9 \cdot 2 \cdot 3)}{1}
F1=6×109NF_1 = 6 \times 10^9 \, N

Next, we calculate the force due to the 8 C charge at 6:
F2=kq2qr22F_2 = \frac{k \cdot |q_2 \cdot q|}{r_2^2}
F2=(9×10988)64F_2 = \frac{(9 \times 10^9 \cdot 8 \cdot 8)}{64}
F2=9×109NF_2 = 9 \times 10^9 \, N

Since both charges exert attractive forces on the -3 C charge, we sum the forces:
Fnet=F1F2F_{\text{net}} = F_1 - F_2
Fnet=6×1099×109F_{\text{net}} = 6 \times 10^9 - 9 \times 10^9
Fnet=3×109NF_{\text{net}} = -3 \times 10^9 \, N

Therefore, the net force on the charge of -3 C at -2 is 3×109-3 \times 10^9 N.

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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.

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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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