GSO002 Problem 12
Problem Statement
Minimum Gap of a Movable Plate Against Non-Linear Electrostatic Force
Problem Statement
On a smooth horizontal insulating floor, two thin metal plates A and B of area S are placed facing each other vertically. Plate A is fixed to the floor. Plate B has mass m and is attached to one end of a light insulating spring (spring constant k) laid horizontally on the floor; the other end of the spring is fixed to a wall. Plate B can slide smoothly and without friction in the horizontal direction along the spring axis, always remaining parallel to plate A. When the spring is at its natural length, the distance between plates A and B is d0.
The permittivity of the medium between the plates is ε. Edge effects are negligible.
Plates A and B are connected in series with a switch and an ideal DC power supply of EMF V. The electrical resistance and self-inductance of the circuit are negligibly small, and no electromagnetic radiation or Joule heat is generated due to plate motion.
As the initial condition, plate B is held at the natural length position (plate separation d0) with the switch closed for a sufficiently long time.
Then, with the switch still closed, the hand is gently released from plate B. Plate B begins to move toward plate A due to the electrostatic attractive force. Let dmin be the plate separation when plate B is closest to plate A.
Find the value of dmin.
Constraints
- Initial plate separation: d0=1.7×10−2 m
- Spring constant: k=1.0×101 N/m
- Permittivity: ε=8.5×10−12 F/m
- Plate area: S=2.0 m2
- EMF of DC supply: V=4.0×102 V
- Mass of plate B: m=5.0×10−1 kg
Input Format
Find dmin in millimeters (mm) and give the numerical value as a positive integer.
Solution
1. Energy Conservation
When plate B is at position d (plate separation), the capacitance is C=dεS. Since the voltage is held at V, the charge changes and the battery does work.
Comparing the state when released (d=d0, velocity =0) with the closest approach (d=dmin, velocity =0):
Work by battery = change in spring energy + change in electrostatic energy:
(Cmin−C0)V2=21k(d0−dmin)2+21(Cmin−C0)V2Simplifying:
21k(d0−dmin)2=21(Cmin−C0)V22. Deriving the Quadratic Equation for dmin
Substituting C=dεS:
k(d0−dmin)2=εSV2(d0dmind0−dmin)Since dmin=d0, divide both sides by (d0−dmin):
k(d0−dmin)=d0dminεSV2Rearranging into a quadratic in dmin:
dmin2−d0dmin+kd0εSV2=0Using the quadratic formula, the two roots are:
d=2d0±d02−4kd0εSV2Since plate B starts at d0 and moves toward plate A, dmin is the first turning point — the larger root:
dmin=2d0+d02−4kd0εSV23. Numerical Calculation
εSV2=(8.5×10−12)×(2.0)×(4.0×102)2=2.72×10−6 J m kd0=(1.0×101)×(1.7×10−2)=0.17 N 4kd0εSV2=4×0.172.72×10−6=64×10−6=0.64×10−4 m2 d02=(1.7×10−2)2=2.89×10−4 m2 D=d02−4kd0εSV2=2.89×10−4−0.64×10−4=2.25×10−4 m2 D=1.5×10−2 m dmin=21.7×10−2+1.5×10−2=23.2×10−2=1.6×10−2 m=16 mmAnswer: 16