A Dipole in an Electric Field β€” Question 1

Section 22-8 Β· Physics pages 3612–3613

Question 1 A uniform field exerts a couple on a neutral rigid dipole A rigid dipole consists of charges βˆ’q and +q separated by vector d directed from negative to positive, so p = qd. The external field is uniform. All torques are about the midpoint. βˆ’q +q βˆ’qE qE p Schematic; labels, not drawing lengths, specify the data. (a) Derive the net force and vector torque from the two individual forces. (b) For p = (2.00, 3.00, 0) Γ— 10βˆ’9 C m and E = (400, 0, 0) N/C, find the torque and its rotational sense as viewed from positive z.
Show solutionHide solution
Question 1 - Solution A uniform field exerts a couple on a neutral rigid dipole βˆ’q +q βˆ’qE qE p (a) Method and calculation F+ = qE, Fβˆ’= βˆ’qE, Fnet = 0. Ο„ = d 2 Γ— qE + ( βˆ’d 2 ) Γ— (βˆ’qE) = p Γ— E. (b) Interpretation and further calculation Ο„z = pxEy βˆ’pyEx = βˆ’(3.00 Γ— 10βˆ’9)(400). Ο„ = βˆ’1.20 Γ— 10βˆ’6Λ†z N m. The negative-z torque is clockwise when viewed from positive z toward the origin. It tends to align the moment with the field. Physical check Zero net force permits a nonzero torque because the equal and opposite forces act on different lines.

Question 1

A uniform field exerts a couple on a neutral rigid dipole

A rigid dipole consists of charges βˆ’q-q and +q+q separated by vector 𝒅\mathbf d directed from negative to positive, so 𝒑=q𝒅\mathbf p=q\mathbf d. The external field is uniform. All torques are about the midpoint.

Diagram shown in the original SVG worksheet.

  1. Derive the net force and vector torque from the two individual forces.

  2. For 𝒑=(2.00,3.00,0)Γ—10βˆ’9\mathbf p=(2.00,3.00,0)\times10^{-9} C m and 𝑬=(400,0,0)\mathbf E=(400,0,0) N/C, find the torque and its rotational sense as viewed from positive z.

Question 1 - Solution

A uniform field exerts a couple on a neutral rigid dipole

Diagram shown in the original SVG worksheet.

(a) Method and calculation

𝑭+=q𝑬,π‘­βˆ’=βˆ’q𝑬,𝑭net=𝟎.\mathbf F_+=q\mathbf E,\quad\mathbf F_-=-q\mathbf E,\quad\mathbf F_{\mathrm{net}}=\mathbf0.𝝉=𝒅2Γ—q𝑬+(βˆ’π’…2)Γ—(βˆ’q𝑬)=𝒑×𝑬.\boldsymbol\tau=\frac{\mathbf d}{2}\times q\mathbf E+\left(-\frac{\mathbf d}{2}\right)\times(-q\mathbf E)=\mathbf p\times\mathbf E.

(b) Interpretation and further calculation

Ο„z=pxEyβˆ’pyEx=βˆ’(3.00Γ—10βˆ’9)(400).\tau_z=p_xE_y-p_yE_x=-(3.00\times10^{-9})(400).𝝉=βˆ’1.20Γ—10βˆ’6𝒛̂Nm.\boldsymbol\tau=-1.20\times10^{-6}\hat{\mathbf z}\,\mathrm{N\,m}.The negative-z torque is clockwise when viewed from positive z toward the origin. It tends to align the moment with the field.

Physical check

Zero net force permits a nonzero torque because the equal and opposite forces act on different lines.