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1. One brass plate is inserted between 2 charges. What will happen to the force of interaction between them? 2.Three charges Q ,2Q ,8Q are to be placed on a line of length R metre. Find the the positions where these should be placed so that the potential energy of the system is minimum. 3.A solid non-conducting sphere of radius R has charge density p=pox , x is the distance from the centre of the sphere. What is the self energy of the sphere? 4.Find the equivalent capacitance between the points m and n. All capacitors are of capacitance Co. 5.Two capacitors of capacitance 1 micro-farad and 4 micro-farad are charged to 60 V by connecting them across a battery. Now the battery is disconnected and the capacitors are connected to each other with terminals of unlike polarity together. Find the final voltage across them. 6.If a,b,c are three vectors such that a+b+c=0 then a x b=? Submit your detailed Question here...

Bibhudatta Barik , 12 Years ago
Grade 12th Pass
anser 1 Answers
Askiitians Tutor Team

Let's tackle your questions one by one, diving into the concepts and calculations involved. Each question touches on fundamental principles in electrostatics and vector mathematics, so we'll break them down for clarity.

1. Effect of a Brass Plate Between Two Charges

When a brass plate is inserted between two charges, it acts as a conductor. This conductor will redistribute its charges in response to the electric field created by the two charges. As a result, the electric field between the two charges is altered, which affects the force of interaction between them.

Initially, the force between two point charges is given by Coulomb's law:

  • F = k * |q1 * q2| / r²

Where k is Coulomb's constant, q1 and q2 are the magnitudes of the charges, and r is the distance between them. When the brass plate is inserted, it reduces the effective electric field between the charges, leading to a decrease in the force of interaction. The charges on the plate will create an opposing electric field that partially cancels the field due to the charges, thus reducing the force.

2. Positioning Charges for Minimum Potential Energy

To minimize the potential energy of a system of charges, we need to consider the interactions between them. The potential energy (U) between two point charges is given by:

  • U = k * q1 * q2 / r

For three charges Q, 2Q, and 8Q, we want to find positions along a line of length R. Let's denote the positions of the charges as:

  • Q at position x1
  • 2Q at position x2
  • 8Q at position x3

To minimize potential energy, we can use the principle of symmetry and the fact that like charges repel. A good approach is to place the charges in a way that the distances between them are proportional to their magnitudes. A possible arrangement could be:

  • Place Q at 0
  • Place 2Q at R/3
  • Place 8Q at R

This arrangement balances the repulsive forces and minimizes the overall potential energy of the system.

3. Self-Energy of a Non-Conducting Sphere

For a solid non-conducting sphere with a charge density that varies linearly with distance from the center (p = p0 * x), we can calculate the self-energy by integrating the energy contributions from each infinitesimal charge element within the sphere.

The self-energy (U) can be expressed as:

  • U = (1/2) * ∫(ρ * V) dV

Where ρ is the charge density and V is the electric potential. By substituting the charge density into the integral and evaluating it over the volume of the sphere, we can find the total self-energy. The integration will involve spherical coordinates and will yield a result dependent on the radius R and the charge density p0.

4. Equivalent Capacitance Calculation

To find the equivalent capacitance between two points (m and n) with multiple capacitors of capacitance C0, we need to know how these capacitors are arranged—whether in series or parallel. The formulas are:

  • For capacitors in series: 1/C_eq = 1/C1 + 1/C2 + ...
  • For capacitors in parallel: C_eq = C1 + C2 + ...

Once we know the configuration, we can apply the appropriate formula to find the equivalent capacitance between points m and n.

5. Final Voltage Across Two Capacitors

When two capacitors (1 µF and 4 µF) charged to 60 V are connected with unlike terminals together, charge redistribution occurs. The total charge before connection is:

  • Q1 = C1 * V1 = 1 µF * 60 V = 60 µC
  • Q2 = C2 * V2 = 4 µF * 60 V = 240 µC

After connecting, the total charge is conserved, and the final voltage (V_f) across the combined capacitors can be calculated using:

  • Q_total = C_eq * V_f

Where C_eq is the equivalent capacitance of the two capacitors in series. This will yield the final voltage across them after charge redistribution.

6. Cross Product of Vectors

Given three vectors a, b, and c such that a + b + c = 0, we can express c as c = - (a + b). The cross product a x b can be evaluated using the properties of cross products:

  • a x b = - (b x a)

Since the cross product is anti-commutative, the result will depend on the magnitudes and the angle between the vectors a and b. If a and b are not parallel, the magnitude of a x b will be non-zero, and we can find its direction using the right-hand rule.

Each of these concepts is foundational in physics and mathematics, and understanding them will greatly enhance your grasp of the subject. If you have further questions or need clarification on any point, feel free to ask!

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