The formula for resistivity is given by:
\(\rho = R \frac{\pi r^2}{l}\)
The relative error in resistivity is given by:
\(\frac{\Delta \rho}{\rho} = \frac{\Delta R}{R} + 2 \frac{\Delta r}{r} + \frac{\Delta l}{l}\)
Substituting the given values:
\(\frac{\Delta \rho}{\rho} = \frac{10}{100} + 2 \times \frac{0.05}{0.35} + \frac{0.2}{15}\)
Calculating each term:
\(\frac{\Delta \rho}{\rho} = 0.1 + 2 \times 0.1429 + 0.0133\)
\(\frac{\Delta \rho}{\rho} \approx 0.1 + 0.2858 + 0.0133 = 0.3991 \approx 39.9\%\)
The problem requires us to calculate the percentage error in the resistivity of a metal wire, given the measured values and their associated errors for the wire's radius, length, and resistance.
1. Formula for Resistivity: The resistance \(R\) of a wire is related to its resistivity \(\rho\), length \(l\), and cross-sectional area \(A\) by the formula:
\[ R = \rho \frac{l}{A} \]
For a wire with a circular cross-section of radius \(r\), the area is \(A = \pi r^2\). Substituting this into the resistance formula and solving for resistivity \(\rho\), we get:
\[ \rho = \frac{R (\pi r^2)}{l} \]
2. Propagation of Errors: For a quantity \(Z\) calculated from measured quantities \(X\), \(Y\), and \(W\) using a formula of the form \(Z = k \cdot X^a \cdot Y^b \cdot W^c\), where \(k\) is a constant, the fractional error in \(Z\) is given by the sum of the fractional errors in the measured quantities, each multiplied by the magnitude of its power:
\[ \frac{\Delta Z}{Z} = a \frac{\Delta X}{X} + b \frac{\Delta Y}{Y} + c \frac{\Delta W}{W} \]
The percentage error is then \( \left( \frac{\Delta Z}{Z} \right) \times 100\% \).
Step 1: List the given measurements and their absolute errors.
Radius, \(r = 0.35 \, \text{cm}\) with absolute error \(\Delta r = 0.05 \, \text{cm}\).
Resistance, \(R = 100 \, \text{ohm}\) with absolute error \(\Delta R = 10 \, \text{ohm}\).
Length, \(l = 15 \, \text{cm}\) with absolute error \(\Delta l = 0.2 \, \text{cm}\).
Step 2: Write the formula for resistivity and derive the expression for its fractional error.
The formula for resistivity is \(\rho = \frac{R \pi r^2}{l}\). Applying the rule for propagation of errors (note that the constant \(\pi\) has no error associated with it):
\[ \frac{\Delta \rho}{\rho} = \frac{\Delta R}{R} + 2 \left( \frac{\Delta r}{r} \right) + \frac{\Delta l}{l} \]
This equation gives the total fractional error in resistivity.
Step 3: Calculate the individual fractional errors for \(R\), \(r\), and \(l\).
Fractional error in resistance:
\[ \frac{\Delta R}{R} = \frac{10}{100} = 0.1 \]
Fractional error in radius:
\[ \frac{\Delta r}{r} = \frac{0.05}{0.35} = \frac{5}{35} = \frac{1}{7} \]
Fractional error in length:
\[ \frac{\Delta l}{l} = \frac{0.2}{15} = \frac{2}{150} = \frac{1}{75} \]
Step 4: Substitute these fractional errors into the formula for the total fractional error in resistivity.
\[ \frac{\Delta \rho}{\rho} = 0.1 + 2 \left( \frac{1}{7} \right) + \frac{1}{75} \]
Step 5: Compute the numerical value of the total fractional error.
\[ \frac{\Delta \rho}{\rho} \approx 0.1 + 2(0.1428) + 0.0133 \] \[ \frac{\Delta \rho}{\rho} \approx 0.1 + 0.2857 + 0.0133 \] \[ \frac{\Delta \rho}{\rho} \approx 0.399 \]
Step 6: Convert the fractional error to a percentage error by multiplying by 100.
\[ \text{Percentage Error in } \rho = \left( \frac{\Delta \rho}{\rho} \right) \times 100\% \] \[ \text{Percentage Error} \approx 0.399 \times 100\% = 39.9\% \]
Rounding to the nearest whole number, the percentage error is approximately 39.9%.
Therefore, the percentage error in the resistivity of the material is 39.9%.
Inductance of a coil with \(10^4\) turns is \(10\,\text{mH}\) and it is connected to a DC source of \(10\,\text{V}\) with internal resistance \(10\,\Omega\). The energy density in the inductor when the current reaches \( \left(\frac{1}{e}\right) \) of its maximum value is \[ \alpha \pi \times \frac{1}{e^2}\ \text{J m}^{-3}. \] The value of \( \alpha \) is _________.
\[ (\mu_0 = 4\pi \times 10^{-7}\ \text{TmA}^{-1}) \]
A small block of mass \(m\) slides down from the top of a frictionless inclined surface, while the inclined plane is moving towards left with constant acceleration \(a_0\). The angle between the inclined plane and ground is \(\theta\) and its base length is \(L\). Assuming that initially the small block is at the top of the inclined plane, the time it takes to reach the lowest point of the inclined plane is _______. 