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1 State Coulomb's Law. 7.2 Draw a labelled free-body diagram for sphere P. 7.3.1 Calculate the magnitude of the electrostatic force between sphere P and sphere Q.

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Question 7

7.1 Coulomb's Law states that the electrostatic force between two point charges is directly proportional to the product of the magnitudes of the charges and inversely proportional to the square of the distance between their centers.

7.2
A labelled free-body diagram for sphere P:

  • Weight (FgF_g or mgmg): Acting vertically downwards.
  • Normal force (FNF_N): Acting vertically upwards from the stand.
  • Electrostatic force (FeF_e): Acting horizontally to the left, due to repulsion from sphere Q.

7.3.1

  1. Identify the given values and Coulomb's Law formula.

    The charges are qP=−30×10−6 Cq_P = -30 \times 10^{-6} \text{ C} and qQ=−20×10−6 Cq_Q = -20 \times 10^{-6} \text{ C}.
    The distance between them is r=80 cm=0.80 mr = 80 \text{ cm} = 0.80 \text{ m}.
    Coulomb's constant is k=9×109 N⋅m2/C2k = 9 \times 10^9 \text{ N} \cdot \text{m}^2/\text{C}^2.
    The formula for electrostatic force is Fe=k∣qPqQ∣r2F_e = k \frac{|q_P q_Q|}{r^2}.

  2. Substitute the values into the formula and calculate the force.

    Fe=(9×109 N⋅m2/C2)∣(−30×10−6 C)(−20×10−6 C)∣(0.80 m)2F_e = (9 \times 10^9 \text{ N} \cdot \text{m}^2/\text{C}^2) \frac{|(-30 \times 10^{-6} \text{ C})(-20 \times 10^{-6} \text{ C})|}{(0.80 \text{ m})^2} Fe=(9×109)(600×10−12)0.64F_e = (9 \times 10^9) \frac{(600 \times 10^{-12})}{0.64} Fe=(9×109)(9.375×10−10)F_e = (9 \times 10^9) (9.375 \times 10^{-10}) Fe=8.4375 NF_e = 8.4375 \text{ N}

    The magnitude of the electrostatic force is 8.44 N\boxed{\text{}8.44 \text{ N}\text{}}.

    7.3.2

  3. Calculate the weight of sphere Q.

    The mass of sphere Q is m=90 g=0.090 kgm = 90 \text{ g} = 0.090 \text{ kg}.
    The acceleration due to gravity is g=9.8 m/s2g = 9.8 \text{ m/s}^2.

    Fg=mg=(0.090 kg)(9.8 m/s2)=0.882 NF_g = mg = (0.090 \text{ kg})(9.8 \text{ m/s}^2) = 0.882 \text{ N}
  4. Use the equilibrium conditions for sphere Q.

    Sphere Q is in equilibrium, so the net force in both horizontal and vertical directions is zero.
    From the free-body diagram for Q (not P, as asked in 7.2, but implied for 7.3.2/7.3.3):

    • Horizontal forces: Tsin⁡θ=FeT \sin \theta = F_e
    • Vertical forces: Tcos⁡θ=FgT \cos \theta = F_g We have Fe=8.4375 NF_e = 8.4375 \text{ N} and Fg=0.882 NF_g = 0.882 \text{ N}.
  5. Calculate the angle θ\theta.

    Divide the horizontal equilibrium equation by the vertical equilibrium equation:

    Tsin⁡θTcos⁡θ=FeFg\frac{T \sin \theta}{T \cos \theta} = \frac{F_e}{F_g} tan⁡θ=8.4375 N0.882 N\tan \theta = \frac{8.4375 \text{ N}}{0.882 \text{ N}} tan⁡θ=9.5663\tan \theta = 9.5663 θ=arctan⁡(9.5663)=84.04∘\theta = \arctan(9.5663) = 84.04^\circ
  6. Calculate the tension T.

    Using the vertical equilibrium equation:

    Tcos⁡θ=FgT \cos \theta = F_g T=Fgcos⁡θ=0.882 Ncos⁡(84.04∘)T = \frac{F_g}{\cos \theta} = \frac{0.882 \text{ N}}{\cos(84.04^\circ)} T=0.882 N0.1038T = \frac{0.882 \text{ N}}{0.1038} T=8.497 NT = 8.497 \text{ N}

    The tension T in the string is 8.50 N\boxed{\text{}8.50 \text{ N}\text{}}.

    7.3.3
    The angle θ\theta was calculated in Step 3 of 7.3.2.

    θ=arctan⁡(FeFg)\theta = \arctan\left(\frac{F_e}{F_g}\right) θ=arctan⁡(8.4375 N0.882 N)\theta = \arctan\left(\frac{8.4375 \text{ N}}{0.882 \text{ N}}\right) θ=arctan⁡(9.5663)\theta = \arctan(9.5663) θ=84.04∘\theta = 84.04^\circ

    The angle θ\theta is 84.0∘\boxed{\text{}84.0^\circ\text{}}.


    Question 8

    8.1 The electric field at a point is defined as the electrostatic force experienced per unit positive test charge placed at that point.

    8.2
    The electric field pattern between spheres A (+5 nC) and B (-4 nC) would show:

    • Field lines originating from sphere A (positive charge).
    • Field lines terminating on sphere B (negative charge).
    • Arrows on the field lines pointing away from A and towards B.
    • The lines would be denser closer to the charges, especially near A due to its larger magnitude of charge compared to B.
    • The lines would not cross each other.

    8.3

  7. Identify the given values and distances.

    qA=+5 nC=+5×10−9 Cq_A = +5 \text{ nC} = +5 \times 10^{-9} \text{ C}
    qB=−4 nC=−4×10−9 Cq_B = -4 \text{ nC} = -4 \times 10^{-9} \text{ C}
    k=9×109 N⋅m2/C2k = 9 \times 10^9 \text{ N} \cdot \text{m}^2/\text{C}^2
    Distance from X to A is rA=rr_A = r.
    Distance from X to B is rB=r+3r=4rr_B = r + 3r = 4r.
    Net electric field at X is Enet=4128 N⋅C−1E_{net} = 4128 \text{ N} \cdot \text{C}^{-1} West.

  8. Determine the direction of electric fields due to A and B at point X.

    • For qAq_A (positive), the electric field EAE_A at X points away from A. Since X is to the left of A, EAE_A points to the left (West).
    • For qBq_B (negative), the electric field EBE_B at X points towards B. Since X is to the left of B, EBE_B points to the right (East).
  9. Write the expressions for EAE_A and EBE_B.

    EA=k∣qA∣rA2=(9×109)5×10−9r2=45r2 (West)E_A = k \frac{|q_A|}{r_A^2} = (9 \times 10^9) \frac{5 \times 10^{-9}}{r^2} = \frac{45}{r^2} \text{ (West)} EB=k∣qB∣rB2=(9×109)4×10−9(4r)2=(9×109)4×10−916r2=3616r2=94r2 (East)E_B = k \frac{|q_B|}{r_B^2} = (9 \times 10^9) \frac{4 \times 10^{-9}}{(4r)^2} = (9 \times 10^9) \frac{4 \times 10^{-9}}{16r^2} = \frac{36}{16r^2} = \frac{9}{4r^2} \text{ (East)}
  10. Calculate the net electric field at X.

    Since EnetE_{net} is West, EAE_A (West) must be greater than EBE_B (East).

    Enet=EA−EBE_{net} = E_A - E_B 4128=45r2−94r24128 = \frac{45}{r^2} - \frac{9}{4r^2} 4128=4×45−94r24128 = \frac{4 \times 45 - 9}{4r^2} 4128=180−94r24128 = \frac{180 - 9}{4r^2} 4128=1714r24128 = \frac{171}{4r^2}
  11. Solve for rr.

    4r2=17141284r^2 = \frac{171}{4128} 4r2=0.04142444r^2 = 0.0414244 r2=0.04142444r^2 = \frac{0.0414244}{4} r2=0.0103561r^2 = 0.0103561 r=0.0103561r = \sqrt{0.0103561} r=0.10176 mr = 0.10176 \text{ m}

    The value of r is 0.102 m\boxed{\text{}0.102 \text{ m}\text{}}.

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