To solve this problem, we need to find the error in the measured current using the given voltage-current relation of the diode: I = \left( e^{1000V/T} - 1 \right) \, \text{mA} where the voltage V is in volts and the temperature T is in kelvin.
We are given:
We apply Taylor series expansion for small changes in voltage:
\delta I = \left( \frac{dI}{dV} \right) \delta V
From the formula I = \left( e^{1000V/T} - 1 \right) \, \text{mA}, the derivative \frac{dI}{dV} can be computed as:
\frac{dI}{dV} = \frac{1000}{T} \cdot e^{1000V/T} \, \text{mA/V}
It's given that the current is measured as I = 0.2 \, \text{mA}.
At this current, set:
0.2 = e^{1000V/T} - 1
Resulting in:
e^{1000V/T} = 1.2
So, \frac{dI}{dV} = \frac{1000}{T} \times 1.2 \, \text{mA/V}
Now, using \delta I = \left( \frac{1000}{T} \times 1.2 \right) \delta V \, \text{mA/V} and given \delta V = 0.01 \, \text{V}, the error in current becomes:
\delta I = \left( \frac{1000}{T} \times 1.2 \right) \times 0.01 \, \text{mA}
The distinctive property of exponential growth provides a high rise for small angular changes, likely increasing the sensitivity values at small errors near 0.2 \, \text{mA} thereby resulting closest plausible significant error to approximately 0.2 \, \text{mA}.
Thus, the correct error is option: 0.2 mA.
If the uncertainty in velocity and position of a minute particle in space are, \(2.4 × 10^{–26}\) \((m s^{–1)}\) and \(10^{–7} (m)\), respectively. The mass of the particle in g is _____ . (Nearest integer)
(Given : \(h = 6.626 × 10^{–34} Js\))