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Four equal charges each 16 muC are place...

Four equal charges each `16 muC` are placed on four corners of a square of side 0.4m. Calculate force on q is zero, how are Q and q related ?

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To solve the problem, we need to analyze the forces acting on the charges placed at the corners of the square. ### Step-by-Step Solution: 1. **Understanding the Setup**: - We have four equal charges \( Q = 16 \, \mu C \) placed at the corners of a square with side length \( a = 0.4 \, m \). 2. **Identifying the Forces**: - Each charge experiences a force due to the other three charges. We need to find the net force acting on one of the charges (let's say charge at corner A). 3. **Calculating the Forces**: - The force between two point charges is given by Coulomb's law: \[ F = k \frac{|Q_1 Q_2|}{r^2} \] where \( k = 8.99 \times 10^9 \, N m^2/C^2 \) is Coulomb's constant, \( Q_1 \) and \( Q_2 \) are the magnitudes of the charges, and \( r \) is the distance between them. 4. **Distance Between Charges**: - The distance between adjacent charges (e.g., A and B) is \( a = 0.4 \, m \). - The distance between diagonal charges (e.g., A and C) can be calculated using the Pythagorean theorem: \[ r_{AC} = \sqrt{a^2 + a^2} = \sqrt{2a^2} = a\sqrt{2} = 0.4\sqrt{2} \, m \] 5. **Calculating the Forces on Charge A**: - The force due to charge B (adjacent): \[ F_{AB} = k \frac{Q^2}{a^2} = 8.99 \times 10^9 \frac{(16 \times 10^{-6})^2}{(0.4)^2} \] - The force due to charge D (adjacent): \[ F_{AD} = k \frac{Q^2}{a^2} = F_{AB} \] - The force due to charge C (diagonal): \[ F_{AC} = k \frac{Q^2}{(0.4\sqrt{2})^2} = k \frac{Q^2}{0.32} \] 6. **Direction of Forces**: - The forces \( F_{AB} \) and \( F_{AD} \) will act along the sides of the square, while \( F_{AC} \) will act diagonally towards charge C. 7. **Setting Up the Equations**: - For the net force on charge A to be zero, the horizontal and vertical components of the forces must balance out. - The horizontal components of \( F_{AB} \) and \( F_{AD} \) must equal the horizontal component of \( F_{AC} \). 8. **Finding the Relationship**: - By symmetry and the requirement for equilibrium, we can derive that for the net force to be zero, the charge \( q \) placed at the center of the square must satisfy: \[ F_{AB} + F_{AD} = 2 F_{AC} \] - This leads to a relationship between \( Q \) and \( q \). 9. **Conclusion**: - The relationship can be derived from the balance of forces, leading to the conclusion that \( q \) must be such that it counteracts the resultant force from the four corner charges.

To solve the problem, we need to analyze the forces acting on the charges placed at the corners of the square. ### Step-by-Step Solution: 1. **Understanding the Setup**: - We have four equal charges \( Q = 16 \, \mu C \) placed at the corners of a square with side length \( a = 0.4 \, m \). 2. **Identifying the Forces**: ...
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Knowledge Check

  • Four equal charges q each are placed at four corners of a square of side a each. Work done in carrying a charge -q from its centre to infinity is

    A
    zero
    B
    `(sqrt2q^(2))/(pi in_(0)a)`
    C
    `(sqrt2q)/(pi in_(0)a)`
    D
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  • Four equal charges Q are placed at the four corners of a square of each side is 'a'. Work done in removing a charge -Q from its centre to infinity is

    A
    `0`
    B
    `(sqrt(2)Q^(2))/(4pi epsilon_(0)a)`
    C
    `(sqrt(2)Q^(2))/(pi epsilon_(0)a)`
    D
    `(Q^(2))/(2pi epsilon_(0)a)`
  • Equal charges q are placed at the three corners B, C, D of a square ABCD of side a. The potential at A is

    A
    `1/(4 pi epsi_(0))q/a`
    B
    `(3q)/(4 pi epsi_(0))`
    C
    `q/(4 pi epsi_(0)a)[2+1/sqrt2]`
    D
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