Physics

Electric Field and Force Analysis of an Electric Dipole System

  • Dipole Configuration Setup:

    • Two source charges of equal magnitude QQ and opposite signs are positioned symmetrically along the x-axis at distance aa from the origin:

    • Charge +Q+Q is located at position (a,0)(a, 0).

    • Charge Q-Q is located at position (a,0)(-a, 0).

    • Target evaluation point PP is located on the y-axis at height bb, with coordinates (0,b)(0, b).

  • Displacement Vectors to Point P:

    • Displacement vector dˉ1\bar{d}_1 from source charge +Q(a,0)+Q(a, 0) to point P(0,b)P(0, b):     dˉ1=(0a,b0)=(a,b)\bar{d}_1 = (0 - a, b - 0) = (-a, b)

    • Displacement vector dˉ2\bar{d}_2 from source charge Q(a,0)-Q(-a, 0) to point P(0,b)P(0, b):     dˉ2=(0(a),b0)=(a,b)\bar{d}_2 = (0 - (-a), b - 0) = (a, b)

  • Distances and Unit Vectors:

    • By the Pythagorean theorem, distance d1d_1 and distance d2d_2 are equal:     d1=d2=a2+b2d_1 = d_2 = \sqrt{a^2 + b^2}

    • Squared distance terms:     d12=d22=a2+b2d_1^2 = d_2^2 = a^2 + b^2

    • Unit direction vector d^1\hat{d}_1 pointing from +Q+Q to PP:     d^1=(a,b)a2+b2\hat{d}_1 = \frac{(-a, b)}{\sqrt{a^2 + b^2}}

    • Unit direction vector d^2\hat{d}_2 pointing from Q-Q to PP:     d^2=(a,b)a2+b2\hat{d}_2 = \frac{(a, b)}{\sqrt{a^2 + b^2}}

  • Coulombic Force on a Test Charge:

    • Place a test charge qq at point P(0,b)P(0, b).

    • By the principle of superposition, total Coulombic force Fˉ\bar{F} on test charge qq is:     Fˉ=Fˉ+Q+FˉQ\bar{F} = \bar{F}_{+Q} + \bar{F}_{-Q}     Fˉ=KeQqd12d^1+Ke(Q)qd22d^2\bar{F} = K_e \frac{Q q}{d_1^2} \hat{d}_1 + K_e \frac{(-Q) q}{d_2^2} \hat{d}_2

    • Substituting distances and unit vectors:     Fˉ=KeQqa2+b2((a,b)a2+b2)+Ke(Q)qa2+b2((a,b)a2+b2)\bar{F} = K_e \frac{Q q}{a^2 + b^2} \left( \frac{(-a, b)}{\sqrt{a^2 + b^2}} \right) + K_e \frac{(-Q) q}{a^2 + b^2} \left( \frac{(a, b)}{\sqrt{a^2 + b^2}} \right)

    • Factoring out common numerical terms and combining fractional powers using exponent rules (n1×n1/2=n3/2n^1 \times n^{1/2} = n^{3/2}):     Fˉ=KeQq(a2+b2)3/2(a,b)KeQq(a2+b2)3/2(a,b)\bar{F} = \frac{K_e Q q}{(a^2 + b^2)^{3/2}} (-a, b) - \frac{K_e Q q}{(a^2 + b^2)^{3/2}} (a, b)

    • Vector arithmetic evaluation:

    • x-component: aa=2a-a - a = -2a

    • y-component: bb=0b - b = 0     Fˉ=q×KeQ(a2+b2)3/2(2a,0)\bar{F} = q \times \frac{K_e Q}{(a^2 + b^2)^{3/2}} (-2a, 0)

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