Dimension of resistance `R` in terms of `mu_0 & epsilon_(0)` are
Dimension of resistance `R` in terms of `mu_0 & epsilon_(0)` are
A
`sqrt((mu_(0))/(epsilon_(0)))`
B
`sqrt((epsilon_(0))/(mu_(0)))`
C
`(epsilon_(0))/(mu_(0))`
D
`(mu_(0))/(epsilon_(0))`
Text Solution
AI Generated Solution
The correct Answer is:
To find the dimension of resistance \( R \) in terms of \( \mu_0 \) (the permeability of free space) and \( \epsilon_0 \) (the permittivity of free space), we can follow these steps:
### Step 1: Start with the formula relating power, current, and resistance
We know from electrical theory that:
\[
I^2 R = P
\]
where \( P \) is the power, \( I \) is the current, and \( R \) is the resistance.
### Step 2: Express power in terms of fundamental quantities
Power \( P \) can be expressed as:
\[
P = \frac{\text{Work}}{\text{Time}} = \frac{\text{Force} \times \text{Displacement}}{\text{Time}}
\]
The unit of work is Joules (J), which can be expressed as:
\[
\text{J} = \text{N} \cdot \text{m} = \text{kg} \cdot \text{m}^2/\text{s}^2
\]
Thus, we can write:
\[
P = \frac{\text{kg} \cdot \text{m}^2}{\text{s}^3}
\]
### Step 3: Substitute for \( P \) in the power equation
Substituting this into the equation \( I^2 R = P \):
\[
I^2 R = \frac{\text{kg} \cdot \text{m}^2}{\text{s}^3}
\]
### Step 4: Express current \( I \) in terms of its dimensions
Current \( I \) has the dimension of:
\[
I = \text{A} = \text{C/s}
\]
where \( \text{C} \) is the unit of charge (Coulombs).
### Step 5: Substitute the expression for \( I \) into the equation
Substituting \( I \) into the equation gives:
\[
(\text{C/s})^2 R = \frac{\text{kg} \cdot \text{m}^2}{\text{s}^3}
\]
This simplifies to:
\[
\frac{\text{C}^2}{\text{s}^2} R = \frac{\text{kg} \cdot \text{m}^2}{\text{s}^3}
\]
### Step 6: Solve for \( R \)
Rearranging gives:
\[
R = \frac{\text{kg} \cdot \text{m}^2}{\text{s}^3} \cdot \frac{\text{s}^2}{\text{C}^2} = \frac{\text{kg} \cdot \text{m}^2}{\text{s}^1 \cdot \text{C}^2}
\]
### Step 7: Find the dimensions of \( \mu_0 \) and \( \epsilon_0 \)
The dimensions of \( \mu_0 \) and \( \epsilon_0 \) are:
- \( \mu_0 \) (permeability of free space) has the dimension:
\[
\mu_0 = \frac{\text{N}}{\text{A}^2} = \frac{\text{kg} \cdot \text{m/s}^2}{\text{C}^2/\text{s}^2} = \frac{\text{kg} \cdot \text{m}^2}{\text{s}^2 \cdot \text{C}^2}
\]
- \( \epsilon_0 \) (permittivity of free space) has the dimension:
\[
\epsilon_0 = \frac{\text{C}^2}{\text{N} \cdot \text{m}^2} = \frac{\text{C}^2}{\text{kg} \cdot \text{m/s}^2 \cdot \text{m}^2} = \frac{\text{C}^2 \cdot \text{s}^2}{\text{kg} \cdot \text{m}^3}
\]
### Step 8: Find the ratio \( \frac{\epsilon_0}{\mu_0} \)
Now, we can find the ratio:
\[
\frac{\epsilon_0}{\mu_0} = \frac{\frac{\text{C}^2 \cdot \text{s}^2}{\text{kg} \cdot \text{m}^3}}{\frac{\text{kg} \cdot \text{m}^2}{\text{s}^2 \cdot \text{C}^2}} = \frac{\text{C}^4 \cdot \text{s}^4}{\text{kg}^2 \cdot \text{m}^5}
\]
### Step 9: Relate \( R \) to \( \mu_0 \) and \( \epsilon_0 \)
From the derived dimensions, we can express resistance \( R \) in terms of \( \mu_0 \) and \( \epsilon_0 \):
\[
R = \sqrt{\frac{\mu_0}{\epsilon_0}}
\]
### Conclusion
Thus, the dimension of resistance \( R \) in terms of \( \mu_0 \) and \( \epsilon_0 \) is:
\[
R = \sqrt{\frac{\mu_0}{\epsilon_0}}
\]
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