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MYP · 15 · extended response

Finding the location where a field vanishes

Fields and gravity · Original GioPhysics question with a detailed, mark-by-mark answer guide.

Demand
discriminating
Marks
6
Topics
3
Answer
Complete
Explore the question data

Field of the left charge alone

Supplied question data. Read the labelled axes and use the observations to test the physical model.

Vertical axis (y): Field magnitude / N C⁻¹

Field of the left charge aloneSupplied question data. Read the labelled axes and use the observations to test the physical model. Horizontal axis: Distance from left charge / m. Vertical axis: Field magnitude / N C⁻¹. Exact values are available in the data table below.090018002700360000.0750.150.2250.3xy

Horizontal axis (x): Distance from left charge / m

Reading 1Distance from left charge / m: 0.1Field magnitude / N C⁻¹: 3600
Read the exact data as a table
Field of the left charge alone — supplied values
Distance from left charge / mField magnitude / N C⁻¹
0.13600
0.2900
0.3400

These are the supplied values, not a worked answer. No fitted trend is drawn.

extended response6 marks

Optional enrichment: this challenge may extend beyond the usual syllabus depth and assumes confidence with algebra and graph interpretation. Two fixed point charges lie on the x-axis: +4.0 nC at x = 0 and +1.0 nC at x = 0.30 m. Use k = 9.0×10⁹ N m² C⁻² and V = kQ/r with zero potential at infinity. The supplied graph gives the field magnitude of the +4.0 nC charge alone. Supplied model: For point charges use field magnitude E = k|Q|/r² and force F = qE, adding field vectors with directions. Supplied data (Distance from left charge / m; Field magnitude / N C⁻¹): (0.1, 3600), (0.2, 900), (0.3, 400).

  1. (a)

    Locate the zero-resultant-field point between the charges and find the electric potential there.

    3 marks
  2. (b)

    Find force on a −2.0 nC test charge at x = 0.10 m, and describe useful field-line features without treating them as literal objects.

    3 marks
Ready to self-mark?Reveal the detailed answer guide
Answer overview(a) Zero field at x = 0.20 m; potential there = +270 V. (b) Resultant field = 3375 N C⁻¹ east; force = 6.75×10⁻⁶ N west.
01

(a)

3 marks

Locate the zero-resultant-field point between the charges and find the electric potential there.

How to approach it

Build a chain of claim, evidence and physics reasoning. Address more than one relevant factor, identify a limitation or assumption, and finish with a conclusion that is conditional on the evidence rather than absolute.

  1. 1

    Between two positive charges their fields oppose. Equality requires 4/x² = 1/(0.30−x)², giving x/(0.30−x) = 2.

  2. 2

    Solve x = 0.20 m, with distances 0.20 and 0.10 m. Field directions, not just magnitudes, must be checked.

  3. 3

    Potential adds as a scalar: V = 9.0×10⁹[(4.0×10⁻⁹)/0.20+(1.0×10⁻⁹)/0.10] = 270 V. Zero field does not require zero potential.

02

(b)

3 marks

Find force on a −2.0 nC test charge at x = 0.10 m, and describe useful field-line features without treating them as literal objects.

How to approach it

Build a chain of claim, evidence and physics reasoning. Address more than one relevant factor, identify a limitation or assumption, and finish with a conclusion that is conditional on the evidence rather than absolute.

  1. 1

    At x = 0.10 m the left charge contributes +3600 N C⁻¹, while the right contributes −9.0/(0.20²) = −225 N C⁻¹.

  2. 2

    Net field is +3375 N C⁻¹. F = qE = (−2.0×10⁻⁹)(3375) = −6.75×10⁻⁶ N; a negative charge feels force opposite the field.

  3. 3

    Lines point away from positive charges, never cross and are denser where field is stronger in a consistent drawing. They represent a continuous vector field, not discrete channels carrying test charges.

Complete marking guidance

Use these worked steps alongside the part-by-part answers. They explain the method and mark allocation; they do not add extra marks.

  1. Between two positive charges their fields oppose. Equality requires 4/x² = 1/(0.30−x)², giving x/(0.30−x) = 2.
  2. Solve x = 0.20 m, with distances 0.20 and 0.10 m. Field directions, not just magnitudes, must be checked.
  3. Potential adds as a scalar: V = 9.0×10⁹[(4.0×10⁻⁹)/0.20+(1.0×10⁻⁹)/0.10] = 270 V. Zero field does not require zero potential.
  4. At x = 0.10 m the left charge contributes +3600 N C⁻¹, while the right contributes −9.0/(0.20²) = −225 N C⁻¹.
  5. Net field is +3375 N C⁻¹. F = qE = (−2.0×10⁻⁹)(3375) = −6.75×10⁻⁶ N; a negative charge feels force opposite the field.
  6. Lines point away from positive charges, never cross and are denser where field is stronger in a consistent drawing. They represent a continuous vector field, not discrete channels carrying test charges.

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