VIPSolutions logo ✨ VIPSolutions

Solve the question as stated with a graph and solve the question in 2 steps with examples and the final answer.Q. 1" find the magnitude of the curent ve a. 0056milv.s if (a) the drift vebcily is 1900 amb (b) He electric field intrity is 500 uvm (c) He sample is accube 3.5 mm on aside hanng a .304 - o. 5 mv bedwem opposike fros. d) the sample is cabe 3.6 mm on a side cerrying a total carrat of 800 mA - Find- (a) V at P:(b) Ent P:(c) Pvat P:(d) the equalion of the equintential sorface pasins invers. fi les the caution of the stresmites emons, in

Question:

Solve the question as stated with a graph and solve the question in 2 steps with examples and the final answer.Q. 1" find the magnitude of the curent ve a. 0056milv.s if (a) the drift vebcily is 1900 amb (b) He electric field intrity is 500 uvm (c) He sample is accube 3.5 mm on aside hanng a .304 - o. 5 mv bedwem opposike fros. d) the sample is cabe 3.6 mm on a side cerrying a total carrat of 800 mA - Find- (a) V at P:(b) Ent P:(c) Pvat P:(d) the equalion of the equintential sorface pasins invers. fi les the caution of the stresmites emons, in

This is AI generated Response.
Asked by: Mack
Created at: 2025-12-25 03:23:30

Final Answer:

Rendered Raw Text
Did you like this answer?
# Solution to the Question Let's clarify and break down your question step by step: You are given a **cube-shaped sample** with certain dimensions and electric properties. You are to find: - The **magnitude of current** given the drift velocity. - The **electric field intensity**. - The **potential at point P**. - The **electric field at point P**. - The **power at point P**. - The **equation of the equipotential surface passing through point P**. I'll answer each sub-question, with example values and steps. A graph will be included at the end. --- ## Step 1: Understand the Given Data Let’s extract the data from your question: - **Sample shape:** Cube - **Side length of cube (a):** - 3.5 mm (for part c) - 3.6 mm (for part d) - **Potential difference (V):** .304 V to .5 mV (exact value unclear, will use .304 V as example) - **Drift velocity ($v_d$):** 190 cm/s ($= 19$ m/s) - **Electric field intensity ($E$):** 500 μV/m = $5 \times 10^{-4}$ V/m - **Total current ($I$):** 800 mA = .8 A (for part d) --- ## Step 2: Solve Each Part ### (a) Magnitude of the Current, Given Drift Velocity **Formula:** \[ I = n e v_d A \] - $n$: number density of charge carriers - $e$: elementary charge ($1.6 \times 10^{-19}$ C) - $v_d$: drift velocity - $A$: cross-sectional area **Assuming** $n = 8.5 \times 10^{28} \mathrm{~m}^{-3}$ (typical for copper) Cube side $a = 3.5\,\text{mm} = 3.5 \times 10^{-3}\,\text{m}$ Area $A = a^2 = (3.5 \times 10^{-3})^2 = 1.225 \times 10^{-5}\,\text{m}^2$ Drift velocity $v_d = 19\,\text{m/s}$ **Calculation:** \[ I = n e v_d A = (8.5 \times 10^{28}) \times (1.6 \times 10^{-19}) \times 19 \times (1.225 \times 10^{-5}) \] \[ I \approx (8.5 \times 1.6 \times 19 \times 1.225) \times 10^{28-19-5} \] \[ I \approx (8.5 \times 1.6 = 13.6; 13.6 \times 19 = 258.4; 258.4 \times 1.225 \approx 316.54) \] \[ I \approx 316.54 \times 10^{28-19-5} = 316.54 \times 10^{4} \] \[ I \approx 3.165 \times 10^{6}\,\text{A} \] **Note:** This value is unphysically large for a small sample; the drift velocity or $n$ value may be off for the example. For principle, the _formula and steps_ are shown. --- **Example with smaller $n$ (e.g., $n = 8.5 \times 10^{22}$):** \[ I = (8.5 \times 10^{22}) \times (1.6 \times 10^{-19}) \times 19 \times (1.225 \times 10^{-5}) \] \[ = 3.165 \times 10^{} = 3.17\,\text{A} \] --- ### (b) Electric Field Intensity Given $E = 500\,\mu\text{V/m} = 5 \times 10^{-4}\,\text{V/m}$ --- ### (c) Potential at Point P If one face is at $V_1 = .304$ V and the opposite at $V_2 = $ V, and $P$ is $x$ mm from the $V_2$ face: \[ V(x) = V_2 + \frac{x}{a}(V_1 - V_2) \] - At $x=$: $V=\,\text{V}$ - At $x=a$: $V=.304\,\text{V}$ - At $x = a/2 = 1.75\,\text{mm}$: \[ V(a/2) = + \frac{1.75}{3.5}(.304) = .152\,\text{V} \] --- ### (d) Equation of Equipotential Surface For a cube aligned along $x$, equipotential surfaces are planes perpendicular to $x$: \[ V(x) = \text{constant} \] So, \[ x = k, \quad \text{where } k \text{ is a constant for a given potential} \] --- ### (e) Electric Field at P The electric field in a uniform cube: \[ E = -\frac{dV}{dx} = \frac{\Delta V}{\Delta x} \] \[ E = \frac{.304\,\text{V}}{3.5 \times 10^{-3}\,\text{m}} = 86.9\,\text{V/m} \] --- ### (f) Power at P Power at P (total power delivered): \[ P = I \cdot V \] \[ P = .8\,\text{A} \times .304\,\text{V} = .243\,\text{W} \] --- ## Example Summary Table | Quantity | Formula | Value (Example) | |-----------------|----------------------------------|--------------------------| | Current ($I$) | $n e v_d A$ | $3.17$ A (see above) | | Electric Field ($E$) | $\Delta V/\Delta x$ | $86.9$ V/m | | Potential at $a/2$ | $V(x) = \frac{x}{a} V_1$ | $.152$ V | | Power ($P$) | $I \cdot V$ | $.243$ W | | Equipotential | $x = \text{constant}$ | Plane at $x = k$ | --- ## Graph: Potential vs. Distance ```mermaid graph LR A[ mm, V] --|linear| B[1.75 mm, .152 V] --|linear| C[3.5 mm, .304 V] ``` **Alt text:** Linear graph of potential vs. distance across the cube, starting at V at mm and rising to .304 V at 3.5 mm. --- ## Final Answers (Examples) 1. **Current:** $I \approx 3.17$ A (with $n = 8.5 \times 10^{22} \mathrm{~m}^{-3}$) 2. **Electric field:** $E = 86.9$ V/m 3. **Potential at $x = a/2$:** $V = .152$ V 4. **Power:** $P = .243$ W 5. **Equipotential surface equation:** $x = \text{constant}$ --- **Note:** Adjust calculations if you have the actual value of $n$ or more precise values. Steps above show the general method.

📢 Instructions:

  • Ask anything relatd to above question only.
  • For new Question goto :

Study Help, Fast Answers

VIPSolutions focuses on clear, step‑by‑step explanations so you can learn quickly. Whether you need an AI‑generated walkthrough or a short hint to get unstuck, each solution is organized for fast reading and easy review later.

Search similar questions, compare approaches, and bookmark the best answers for revision. Our goal is simple: quick, reliable study help that feels natural—not noisy.