3x Find the vector of the Force when the V = -ye³x + zsin(x) where V is the potential function. If x = t and y = 3t and z = 1 - t, find the moment as a function of time, M(t), and find the angular momentum, H(t), as function of time when the position is 7 = 3î - 2ĵ+ 5k.

Elements Of Electromagnetics
7th Edition
ISBN:9780190698614
Author:Sadiku, Matthew N. O.
Publisher:Sadiku, Matthew N. O.
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**Vector of the Force from Potential Function**

Given the potential function \( V = -ye^{3x} + z \sin(x) \), where \( V \) is the potential function, we aim to find the force vector \(\vec{F}\).

### Expression and Variables

If \( x = t \), \( y = 3t \), and \( z = 1 - t \):
1. **Position vector**:
   \[
   \vec{r} = 3t\hat{i} - 2t\hat{j} + 5\hat{k}
   \]

2. **Moment as a function of time** \( \vec{M}(t) \).
3. **Angular momentum as a function of time** \( \vec{H}(t) \).

### Analytical Steps

1. **Force Calculation**:
   The force \(\vec{F}\) is given by the negative gradient of the potential \( V \):
   \[
   \vec{F} = - \nabla V
   \]

   To compute this, find the partial derivatives of \( V \).

   For \( V = -ye^{3x} + z \sin(x) \):

   \[
   \frac{\partial V}{\partial x} = -3ye^{3x} + z \cos(x)
   \]

   \[
   \frac{\partial V}{\partial y} = -e^{3x}
   \]

   \[
   \frac{\partial V}{\partial z} = \sin(x)
   \]

   Therefore, the force vector is:
   \[
   \vec{F} = - \left( \frac{\partial V}{\partial x}\hat{i} + \frac{\partial V}{\partial y}\hat{j} + \frac{\partial V}{\partial z}\hat{k} \right) = \left( 3ye^{3x} - z \cos(x) \right)\hat{i} + e^{3x}\hat{j} - \sin(x)\hat{k}
   \]

2. **Moment Calculation** \( \vec{M}(t) \):
   \[
   \vec{M}(t) = \vec{r} \times \vec{F}
   \]

3. **Angular Momentum Calculation** \( \vec{H}(t)
Transcribed Image Text:**Vector of the Force from Potential Function** Given the potential function \( V = -ye^{3x} + z \sin(x) \), where \( V \) is the potential function, we aim to find the force vector \(\vec{F}\). ### Expression and Variables If \( x = t \), \( y = 3t \), and \( z = 1 - t \): 1. **Position vector**: \[ \vec{r} = 3t\hat{i} - 2t\hat{j} + 5\hat{k} \] 2. **Moment as a function of time** \( \vec{M}(t) \). 3. **Angular momentum as a function of time** \( \vec{H}(t) \). ### Analytical Steps 1. **Force Calculation**: The force \(\vec{F}\) is given by the negative gradient of the potential \( V \): \[ \vec{F} = - \nabla V \] To compute this, find the partial derivatives of \( V \). For \( V = -ye^{3x} + z \sin(x) \): \[ \frac{\partial V}{\partial x} = -3ye^{3x} + z \cos(x) \] \[ \frac{\partial V}{\partial y} = -e^{3x} \] \[ \frac{\partial V}{\partial z} = \sin(x) \] Therefore, the force vector is: \[ \vec{F} = - \left( \frac{\partial V}{\partial x}\hat{i} + \frac{\partial V}{\partial y}\hat{j} + \frac{\partial V}{\partial z}\hat{k} \right) = \left( 3ye^{3x} - z \cos(x) \right)\hat{i} + e^{3x}\hat{j} - \sin(x)\hat{k} \] 2. **Moment Calculation** \( \vec{M}(t) \): \[ \vec{M}(t) = \vec{r} \times \vec{F} \] 3. **Angular Momentum Calculation** \( \vec{H}(t)
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