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Resistivity of a material within a resistor

Materials Science · FE Reference Handbook section

Materials Science
5 formulas
10 exam-style examples
~55 min
All Materials Science lectures

Core formulas for this FE topic

Definitions, applicability, units, assumptions and worked examples for each relation.

Worked exam-style examples

The four ways this section is written on the real exam — thoughts first, then equations, then substitution.

Example 1
Resistivity of a conductor and capacitance of a parallel plate — Resistivity of a material within a resistor

A conductor of resistivity 1.00e-6 Ω·m is 2.0 m long with a cross-section of 1.4e-5 m². Find its resistance. A parallel plate capacitor with the same material as dielectric (ε_r = 3.0), plate area 0.0190 m² and spacing 0.00080 m is charged to 167 V — find its capacitance and stored charge.

Given

  • ρ = 1.00e-6 Ω·m

  • L=2.0m,A=1.4e−5m2L = 2.0 m, A = 1.4e-5 m^{2}
  • εr=3.0,Ap=0.0190m2,d=0.00080m\varepsilon_r = 3.0, A_p = 0.0190 m^{2}, d = 0.00080 m
  • V=167VV = 167 V

Find

Resistance R, capacitance C and charge Q

Start with the thinking

  • Resistivity is a material property; resistance also depends on geometry.
  • Charge held by a capacitor is simply Q = C V once the capacitance is known.

Step-by-step solution

  1. Formula

    R=ρL/AR = \rho L / A
  2. Substituting

    R=1.00e−6(2.0)/1.4e−5=0.1429ΩR = 1.00e-6(2.0)/1.4e-5 = 0.1429 \Omega
  3. Formula

    C=ε0εrA/dC = \varepsilon_{0} \varepsilon_r A / d
  4. Substituting

    C=(8.854×10−12)(3.0)(0.0190)/0.00080=6.308e−10FC = (8.854\times10^{-12})(3.0)(0.0190)/0.00080 = 6.308e-10 F
  5. Formula

    Q=CVQ = C V
  6. Substituting

    Q=6.308e−10(167)=1.054e−7CQ = 6.308e-10(167) = 1.054e-7 C
Answer:
R=0.143Ω,C=6.31e−10F,Q=1.05e−7CR = 0.143 \Omega, C = 6.31e-10 F, Q = 1.05e-7 C

Why the other options are there

  • R = 0.000000 Ω (L and A swapped)
  • C = 2.10e-10 F (relative permittivity omitted)

Reference: FE Reference Handbook — Materials Science → Resistivity of a material within a resistor

Example 2
Resistivity of a conductor and capacitance of a parallel plate — Resistivity of a material within a resistor (2)

A conductor of resistivity 0.00e+0 Ω·m is 2.0 m long with a cross-section of 1.5e-5 m². Find its resistance. A parallel plate capacitor with the same material as dielectric (ε_r = 2.0), plate area 0.0010 m² and spacing 0.00040 m is charged to 155 V — find its capacitance and stored charge.

Given

  • ρ = 0.00e+0 Ω·m

  • L=2.0m,A=1.5e−5m2L = 2.0 m, A = 1.5e-5 m^{2}
  • εr=2.0,Ap=0.0010m2,d=0.00040m\varepsilon_r = 2.0, A_p = 0.0010 m^{2}, d = 0.00040 m
  • V=155VV = 155 V

Find

Resistance R, capacitance C and charge Q

Start with the thinking

  • Resistivity is a material property; resistance also depends on geometry.
  • Charge held by a capacitor is simply Q = C V once the capacitance is known.

Step-by-step solution

  1. Formula

    R=ρL/AR = \rho L / A
  2. Substituting

    R=0.00e+0(2.0)/1.5e−5=0.0000ΩR = 0.00e+0(2.0)/1.5e-5 = 0.0000 \Omega
  3. Formula

    C=ε0εrA/dC = \varepsilon_{0} \varepsilon_r A / d
  4. Substituting

    C=(8.854×10−12)(2.0)(0.0010)/0.00040=4.427e−11FC = (8.854\times10^{-12})(2.0)(0.0010)/0.00040 = 4.427e-11 F
  5. Formula

    Q=CVQ = C V
  6. Substituting

    Q=4.427e−11(155)=6.862e−9CQ = 4.427e-11(155) = 6.862e-9 C
Answer:
R=0.000Ω,C=4.43e−11F,Q=6.86e−9CR = 0.000 \Omega, C = 4.43e-11 F, Q = 6.86e-9 C

Why the other options are there

  • R = 0.000000 Ω (L and A swapped)
  • C = 2.21e-11 F (relative permittivity omitted)

Reference: FE Reference Handbook — Materials Science → Resistivity of a material within a resistor

Example 3
Resistivity of a conductor and capacitance of a parallel plate — Resistivity of a material within a resistor (3)

A conductor of resistivity 1.00e-6 Ω·m is 1.5 m long with a cross-section of 1.6e-5 m². Find its resistance. A parallel plate capacitor with the same material as dielectric (ε_r = 4.0), plate area 0.0120 m² and spacing 0.00080 m is charged to 130 V — find its capacitance and stored charge.

Given

  • ρ = 1.00e-6 Ω·m

  • L=1.5m,A=1.6e−5m2L = 1.5 m, A = 1.6e-5 m^{2}
  • εr=4.0,Ap=0.0120m2,d=0.00080m\varepsilon_r = 4.0, A_p = 0.0120 m^{2}, d = 0.00080 m
  • V=130VV = 130 V

Find

Resistance R, capacitance C and charge Q

Start with the thinking

  • Resistivity is a material property; resistance also depends on geometry.
  • Charge held by a capacitor is simply Q = C V once the capacitance is known.

Step-by-step solution

  1. Formula

    R=ρL/AR = \rho L / A
  2. Substituting

    R=1.00e−6(1.5)/1.6e−5=0.0938ΩR = 1.00e-6(1.5)/1.6e-5 = 0.0938 \Omega
  3. Formula

    C=ε0εrA/dC = \varepsilon_{0} \varepsilon_r A / d
  4. Substituting

    C=(8.854×10−12)(4.0)(0.0120)/0.00080=5.312e−10FC = (8.854\times10^{-12})(4.0)(0.0120)/0.00080 = 5.312e-10 F
  5. Formula

    Q=CVQ = C V
  6. Substituting

    Q=5.312e−10(130)=6.906e−8CQ = 5.312e-10(130) = 6.906e-8 C
Answer:
R=0.094Ω,C=5.31e−10F,Q=6.91e−8CR = 0.094 \Omega, C = 5.31e-10 F, Q = 6.91e-8 C

Why the other options are there

  • R = 0.000000 Ω (L and A swapped)
  • C = 1.33e-10 F (relative permittivity omitted)

Reference: FE Reference Handbook — Materials Science → Resistivity of a material within a resistor

Example 4
Resistivity of a conductor and capacitance of a parallel plate — Resistivity of a material within a resistor (4)

A conductor of resistivity 0.00e+0 Ω·m is 2.5 m long with a cross-section of 1.7e-5 m². Find its resistance. A parallel plate capacitor with the same material as dielectric (ε_r = 6.5), plate area 0.0100 m² and spacing 0.00030 m is charged to 51 V — find its capacitance and stored charge.

Given

  • ρ = 0.00e+0 Ω·m

  • L=2.5m,A=1.7e−5m2L = 2.5 m, A = 1.7e-5 m^{2}
  • εr=6.5,Ap=0.0100m2,d=0.00030m\varepsilon_r = 6.5, A_p = 0.0100 m^{2}, d = 0.00030 m
  • V=51VV = 51 V

Find

Resistance R, capacitance C and charge Q

Start with the thinking

  • Resistivity is a material property; resistance also depends on geometry.
  • Charge held by a capacitor is simply Q = C V once the capacitance is known.

Step-by-step solution

  1. Formula

    R=ρL/AR = \rho L / A
  2. Substituting

    R=0.00e+0(2.5)/1.7e−5=0.0000ΩR = 0.00e+0(2.5)/1.7e-5 = 0.0000 \Omega
  3. Formula

    C=ε0εrA/dC = \varepsilon_{0} \varepsilon_r A / d
  4. Substituting

    C=(8.854×10−12)(6.5)(0.0100)/0.00030=1.918e−9FC = (8.854\times10^{-12})(6.5)(0.0100)/0.00030 = 1.918e-9 F
  5. Formula

    Q=CVQ = C V
  6. Substituting

    Q=1.918e−9(51)=9.784e−8CQ = 1.918e-9(51) = 9.784e-8 C
Answer:
R=0.000Ω,C=1.92e−9F,Q=9.78e−8CR = 0.000 \Omega, C = 1.92e-9 F, Q = 9.78e-8 C

Why the other options are there

  • R = 0.000000 Ω (L and A swapped)
  • C = 2.95e-10 F (relative permittivity omitted)

Reference: FE Reference Handbook — Materials Science → Resistivity of a material within a resistor

Example 5
Resistivity of a conductor and capacitance of a parallel plate — Resistivity of a material within a resistor (5)

A conductor of resistivity 1.00e-6 Ω·m is 4.5 m long with a cross-section of 1.3e-5 m². Find its resistance. A parallel plate capacitor with the same material as dielectric (ε_r = 3.0), plate area 0.0130 m² and spacing 0.00010 m is charged to 65 V — find its capacitance and stored charge.

Given

  • ρ = 1.00e-6 Ω·m

  • L=4.5m,A=1.3e−5m2L = 4.5 m, A = 1.3e-5 m^{2}
  • εr=3.0,Ap=0.0130m2,d=0.00010m\varepsilon_r = 3.0, A_p = 0.0130 m^{2}, d = 0.00010 m
  • V=65VV = 65 V

Find

Resistance R, capacitance C and charge Q

Start with the thinking

  • Resistivity is a material property; resistance also depends on geometry.
  • Charge held by a capacitor is simply Q = C V once the capacitance is known.

Step-by-step solution

  1. Formula

    R=ρL/AR = \rho L / A
  2. Substituting

    R=1.00e−6(4.5)/1.3e−5=0.3462ΩR = 1.00e-6(4.5)/1.3e-5 = 0.3462 \Omega
  3. Formula

    C=ε0εrA/dC = \varepsilon_{0} \varepsilon_r A / d
  4. Substituting

    C=(8.854×10−12)(3.0)(0.0130)/0.00010=3.453e−9FC = (8.854\times10^{-12})(3.0)(0.0130)/0.00010 = 3.453e-9 F
  5. Formula

    Q=CVQ = C V
  6. Substituting

    Q=3.453e−9(65)=2.244e−7CQ = 3.453e-9(65) = 2.244e-7 C
Answer:
R=0.346Ω,C=3.45e−9F,Q=2.24e−7CR = 0.346 \Omega, C = 3.45e-9 F, Q = 2.24e-7 C

Why the other options are there

  • R = 0.000000 Ω (L and A swapped)
  • C = 1.15e-9 F (relative permittivity omitted)

Reference: FE Reference Handbook — Materials Science → Resistivity of a material within a resistor

Example 6
Resistivity of a conductor and capacitance of a parallel plate — Resistivity of a material within a resistor (6)

A conductor of resistivity 1.00e-6 Ω·m is 4.0 m long with a cross-section of 1.3e-5 m². Find its resistance. A parallel plate capacitor with the same material as dielectric (ε_r = 2.0), plate area 0.0170 m² and spacing 0.00040 m is charged to 130 V — find its capacitance and stored charge.

Given

  • ρ = 1.00e-6 Ω·m

  • L=4.0m,A=1.3e−5m2L = 4.0 m, A = 1.3e-5 m^{2}
  • εr=2.0,Ap=0.0170m2,d=0.00040m\varepsilon_r = 2.0, A_p = 0.0170 m^{2}, d = 0.00040 m
  • V=130VV = 130 V

Find

Resistance R, capacitance C and charge Q

Start with the thinking

  • Resistivity is a material property; resistance also depends on geometry.
  • Charge held by a capacitor is simply Q = C V once the capacitance is known.

Step-by-step solution

  1. Formula

    R=ρL/AR = \rho L / A
  2. Substituting

    R=1.00e−6(4.0)/1.3e−5=0.3077ΩR = 1.00e-6(4.0)/1.3e-5 = 0.3077 \Omega
  3. Formula

    C=ε0εrA/dC = \varepsilon_{0} \varepsilon_r A / d
  4. Substituting

    C=(8.854×10−12)(2.0)(0.0170)/0.00040=7.526e−10FC = (8.854\times10^{-12})(2.0)(0.0170)/0.00040 = 7.526e-10 F
  5. Formula

    Q=CVQ = C V
  6. Substituting

    Q=7.526e−10(130)=9.784e−8CQ = 7.526e-10(130) = 9.784e-8 C
Answer:
R=0.308Ω,C=7.53e−10F,Q=9.78e−8CR = 0.308 \Omega, C = 7.53e-10 F, Q = 9.78e-8 C

Why the other options are there

  • R = 0.000000 Ω (L and A swapped)
  • C = 3.76e-10 F (relative permittivity omitted)

Reference: FE Reference Handbook — Materials Science → Resistivity of a material within a resistor

Example 7
Resistivity of a conductor and capacitance of a parallel plate — Resistivity of a material within a resistor (7)

A conductor of resistivity 0.00e+0 Ω·m is 2.0 m long with a cross-section of 1.1e-5 m². Find its resistance. A parallel plate capacitor with the same material as dielectric (ε_r = 4.5), plate area 0.0060 m² and spacing 0.00050 m is charged to 170 V — find its capacitance and stored charge.

Given

  • ρ = 0.00e+0 Ω·m

  • L=2.0m,A=1.1e−5m2L = 2.0 m, A = 1.1e-5 m^{2}
  • εr=4.5,Ap=0.0060m2,d=0.00050m\varepsilon_r = 4.5, A_p = 0.0060 m^{2}, d = 0.00050 m
  • V=170VV = 170 V

Find

Resistance R, capacitance C and charge Q

Start with the thinking

  • Resistivity is a material property; resistance also depends on geometry.
  • Charge held by a capacitor is simply Q = C V once the capacitance is known.

Step-by-step solution

  1. Formula

    R=ρL/AR = \rho L / A
  2. Substituting

    R=0.00e+0(2.0)/1.1e−5=0.0000ΩR = 0.00e+0(2.0)/1.1e-5 = 0.0000 \Omega
  3. Formula

    C=ε0εrA/dC = \varepsilon_{0} \varepsilon_r A / d
  4. Substituting

    C=(8.854×10−12)(4.5)(0.0060)/0.00050=4.781e−10FC = (8.854\times10^{-12})(4.5)(0.0060)/0.00050 = 4.781e-10 F
  5. Formula

    Q=CVQ = C V
  6. Substituting

    Q=4.781e−10(170)=8.128e−8CQ = 4.781e-10(170) = 8.128e-8 C
Answer:
R=0.000Ω,C=4.78e−10F,Q=8.13e−8CR = 0.000 \Omega, C = 4.78e-10 F, Q = 8.13e-8 C

Why the other options are there

  • R = 0.000000 Ω (L and A swapped)
  • C = 1.06e-10 F (relative permittivity omitted)

Reference: FE Reference Handbook — Materials Science → Resistivity of a material within a resistor

Example 8
Resistivity of a conductor and capacitance of a parallel plate — Resistivity of a material within a resistor (8)

A conductor of resistivity 1.00e-6 Ω·m is 2.0 m long with a cross-section of 8.0e-6 m². Find its resistance. A parallel plate capacitor with the same material as dielectric (ε_r = 6.0), plate area 0.0070 m² and spacing 0.00070 m is charged to 59 V — find its capacitance and stored charge.

Given

  • ρ = 1.00e-6 Ω·m

  • L=2.0m,A=8.0e−6m2L = 2.0 m, A = 8.0e-6 m^{2}
  • εr=6.0,Ap=0.0070m2,d=0.00070m\varepsilon_r = 6.0, A_p = 0.0070 m^{2}, d = 0.00070 m
  • V=59VV = 59 V

Find

Resistance R, capacitance C and charge Q

Start with the thinking

  • Resistivity is a material property; resistance also depends on geometry.
  • Charge held by a capacitor is simply Q = C V once the capacitance is known.

Step-by-step solution

  1. Formula

    R=ρL/AR = \rho L / A
  2. Substituting

    R=1.00e−6(2.0)/8.0e−6=0.2500ΩR = 1.00e-6(2.0)/8.0e-6 = 0.2500 \Omega
  3. Formula

    C=ε0εrA/dC = \varepsilon_{0} \varepsilon_r A / d
  4. Substituting

    C=(8.854×10−12)(6.0)(0.0070)/0.00070=5.312e−10FC = (8.854\times10^{-12})(6.0)(0.0070)/0.00070 = 5.312e-10 F
  5. Formula

    Q=CVQ = C V
  6. Substituting

    Q=5.312e−10(59)=3.134e−8CQ = 5.312e-10(59) = 3.134e-8 C
Answer:
R=0.250Ω,C=5.31e−10F,Q=3.13e−8CR = 0.250 \Omega, C = 5.31e-10 F, Q = 3.13e-8 C

Why the other options are there

  • R = 0.000000 Ω (L and A swapped)
  • C = 8.85e-11 F (relative permittivity omitted)

Reference: FE Reference Handbook — Materials Science → Resistivity of a material within a resistor

Example 9
Resistivity of a conductor and capacitance of a parallel plate — Resistivity of a material within a resistor (9)

A conductor of resistivity 1.00e-6 Ω·m is 2.0 m long with a cross-section of 1.1e-5 m². Find its resistance. A parallel plate capacitor with the same material as dielectric (ε_r = 7.0), plate area 0.0060 m² and spacing 0.00050 m is charged to 144 V — find its capacitance and stored charge.

Given

  • ρ = 1.00e-6 Ω·m

  • L=2.0m,A=1.1e−5m2L = 2.0 m, A = 1.1e-5 m^{2}
  • εr=7.0,Ap=0.0060m2,d=0.00050m\varepsilon_r = 7.0, A_p = 0.0060 m^{2}, d = 0.00050 m
  • V=144VV = 144 V

Find

Resistance R, capacitance C and charge Q

Start with the thinking

  • Resistivity is a material property; resistance also depends on geometry.
  • Charge held by a capacitor is simply Q = C V once the capacitance is known.

Step-by-step solution

  1. Formula

    R=ρL/AR = \rho L / A
  2. Substituting

    R=1.00e−6(2.0)/1.1e−5=0.1818ΩR = 1.00e-6(2.0)/1.1e-5 = 0.1818 \Omega
  3. Formula

    C=ε0εrA/dC = \varepsilon_{0} \varepsilon_r A / d
  4. Substituting

    C=(8.854×10−12)(7.0)(0.0060)/0.00050=7.437e−10FC = (8.854\times10^{-12})(7.0)(0.0060)/0.00050 = 7.437e-10 F
  5. Formula

    Q=CVQ = C V
  6. Substituting

    Q=7.437e−10(144)=1.071e−7CQ = 7.437e-10(144) = 1.071e-7 C
Answer:
R=0.182Ω,C=7.44e−10F,Q=1.07e−7CR = 0.182 \Omega, C = 7.44e-10 F, Q = 1.07e-7 C

Why the other options are there

  • R = 0.000000 Ω (L and A swapped)
  • C = 1.06e-10 F (relative permittivity omitted)

Reference: FE Reference Handbook — Materials Science → Resistivity of a material within a resistor

Example 10
Resistivity of a conductor and capacitance of a parallel plate — Resistivity of a material within a resistor (10)

A conductor of resistivity 0.00e+0 Ω·m is 4.5 m long with a cross-section of 1.2e-5 m². Find its resistance. A parallel plate capacitor with the same material as dielectric (ε_r = 3.5), plate area 0.0040 m² and spacing 0.00050 m is charged to 171 V — find its capacitance and stored charge.

Given

  • ρ = 0.00e+0 Ω·m

  • L=4.5m,A=1.2e−5m2L = 4.5 m, A = 1.2e-5 m^{2}
  • εr=3.5,Ap=0.0040m2,d=0.00050m\varepsilon_r = 3.5, A_p = 0.0040 m^{2}, d = 0.00050 m
  • V=171VV = 171 V

Find

Resistance R, capacitance C and charge Q

Start with the thinking

  • Resistivity is a material property; resistance also depends on geometry.
  • Charge held by a capacitor is simply Q = C V once the capacitance is known.

Step-by-step solution

  1. Formula

    R=ρL/AR = \rho L / A
  2. Substituting

    R=0.00e+0(4.5)/1.2e−5=0.0000ΩR = 0.00e+0(4.5)/1.2e-5 = 0.0000 \Omega
  3. Formula

    C=ε0εrA/dC = \varepsilon_{0} \varepsilon_r A / d
  4. Substituting

    C=(8.854×10−12)(3.5)(0.0040)/0.00050=2.479e−10FC = (8.854\times10^{-12})(3.5)(0.0040)/0.00050 = 2.479e-10 F
  5. Formula

    Q=CVQ = C V
  6. Substituting

    Q=2.479e−10(171)=4.239e−8CQ = 2.479e-10(171) = 4.239e-8 C
Answer:
R=0.000Ω,C=2.48e−10F,Q=4.24e−8CR = 0.000 \Omega, C = 2.48e-10 F, Q = 4.24e-8 C

Why the other options are there

  • R = 0.000000 Ω (L and A swapped)
  • C = 7.08e-11 F (relative permittivity omitted)

Reference: FE Reference Handbook — Materials Science → Resistivity of a material within a resistor

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