Problem 30
Question
\(\bullet$$\bullet$$\bullet\) A charge \(+Q\) is located at the origin and a second charge, \(+4 Q,\) is at distance \(d\) on the \(x\) -axis. Where should a third charge, \(q,\) be placed, and what should be its sign and magnitude, so that all three charges will be in equilibrium?
Step-by-Step Solution
Verified Answer
Place charge \(-16Q\) at \(x = -\frac{d}{2}\) to achieve equilibrium.
1Step 1: Determine the Forces on Each Charge
For equilibrium, the net force on each charge should be zero. Consider only the forces due to other charges since the environment is unspecified. The force between two point charges is given by Coulomb's Law, \( F = \frac{{k \cdot |q_1 \cdot q_2|}}{{r^2}} \), where \( k \) is Coulomb's constant, \( q_1 \) and \( q_2 \) are the magnitudes of charges, and \( r \) is the distance between them.
2Step 2: Analyze Forces on Charge +Q at the Origin
The forces acting on charge \(+Q\) are due to charges \(+4Q\) and \(q\). * Force due to \(+4Q\) is repulsive and acts along the positive x-axis.* Force due to \(q\) (yet to be defined) must be in the opposite direction to achieve equilibrium.
3Step 3: Analyze Forces on Charge +4Q at Position x = d
The forces on charge \(+4Q\) are from \(+Q\) and \(q\). * Force due to \(+Q\) is repulsive and directed toward negative x-axis.* Force due to \(q\) should balance the force from \(+Q\) so it must act towards positive x-axis.
4Step 4: Calculate Equilibrium Condition for Charge +Q
Assume charge \(q\) is at position \(x\).Equilibrium condition states: \( F_q = F_{4Q} \)Using Coulomb's law, equate the forces:\[ \frac{k \cdot Q \cdot |q|}{x^2} = \frac{k \cdot Q \cdot 4Q}{d^2} \]The \(k\) and \(Q\) cancel out:\[ \frac{|q|}{x^2} = \frac{4Q}{d^2} \]
5Step 5: Solve for Position and Sign of Charge q
Assuming \(x = -a\) (to be left of \(+Q\) on x-axis), substitute \(x = -a\):\[ \frac{|q|}{a^2} = \frac{4Q}{d^2} \]Calculate \(a\) from balancing forces on all charges:\( a = \frac{d}{2} \).Since the charge \(q\) provides the opposite force direction on \(+Q\) and is left of it:\(q\) must be negative to balance the positive charges \(+Q\) and \(+4Q\).
6Step 6: Determine the Magnitude of Charge q
Substitute \( a = \frac{d}{2}\) into the equilibrium condition:\[ \frac{|q|}{(\frac{d}{2})^2} = \frac{4Q}{d^2} \]Solve for \(|q|\):\[ |q| = \frac{4Q}{(\frac{d}{2})^2} \, \Rightarrow \, |q| = 16Q \]Thus, the required \(q = -16Q\).
7Step 7: Verify Conditions for All Charges
Check if the derived position and charge magnitude ensure equilibrium for all charges by substituting back and confirming the net forces equate to zero.
Key Concepts
Electric ChargeForce EquilibriumPoint Charges
Electric Charge
Electric charge is a fundamental property of matter. It comes in two types: positive and negative. Charges interact with one another through forces described by Coulomb's Law. Coulomb's Law tells us the magnitude of the force between two point charges. It's determined by the formula:
This concept is crucial in many physics problems and applications, including this exercise where charges need to balance to achieve an equilibrium state.
- \( F = \frac{{k \, |q_1 \cdot q_2|}}{{r^2}} \)
This concept is crucial in many physics problems and applications, including this exercise where charges need to balance to achieve an equilibrium state.
Force Equilibrium
Force equilibrium occurs when all the forces acting on a system result in a net force of zero. For a system of charged particles, this means arranging the charges so that each one is subject to no unbalanced forces.
In this problem, we want the charges placed such that the net force on each charge is zero.
In this problem, we want the charges placed such that the net force on each charge is zero.
- The force on charge \(+Q\) due to other charges must be cancelled out by the force of another charge.
- Similarly, charge \(+4Q\) experiences two forces that should also be balanced.
- The third charge, \( q \), needs to be positioned so that it counteracts the repulsive forces experienced by each charge.
Point Charges
Point charges are simplified models of charges where the size of each charge is considered to be insignificantly small. This allows us to focus purely on the mathematical description of electric forces without having to consider charge shape or distribution.
In equilibrium problems involving point charges like this one, you calculate forces based on the assumption that the charges are concentrated at a single point in space.
In equilibrium problems involving point charges like this one, you calculate forces based on the assumption that the charges are concentrated at a single point in space.
- It simplifies mathematical calculations, making it easier to apply Coulomb's Law.
- Assuming charges as point charges, we can ignore additional complexities like surface area effects.
Other exercises in this chapter
Problem 22
\(\bullet$$\bullet\) Two point charges are placed on the \(x\) axis as follows: Charge \(q_{1}=+4.00 \mathrm{nC}\) is located at \(x=0.200 \mathrm{m},\) and cha
View solution Problem 28
\(\bullet$$\bullet\) Two unequal charges repel each other with a force \(F .\) If both charges are doubled in magnitude, what will be the new force in terms of
View solution Problem 31
\(\bullet\) A small object carrying a charge of \(-8.00 \mathrm{nC}\) is acted upon by a downward force of 20.0 \(\mathrm{nN}\) when placed at a certain point i
View solution Problem 32
\(\bullet\) (a) What must the charge (sign and magnitude) of a 1.45 \(\mathrm{g}\) particle be for it to remain balanced against gravity when placed in a downwa
View solution