For the CE-transistor amplifier, the audio signal voltage across the collected resistance of 3 kΩ is 3V. Assume the current amplification factor of the transistor is 50, and find the input voltage and base current, if the resistance is 1 k Ω ?
This problem focuses on a Common Emitter (CE) transistor amplifier and requires us to determine two crucial parameters: the input voltage and the base current. We are provided with several key details about the amplifier's operation, including the voltage across the collector resistance, the value of the collector resistance, the transistor's current amplification factor, and the input resistance (which is essentially the base resistance).
To begin our analysis, let's organize the specific values provided in the question:
| Parameter | Symbol | Value |
|---|---|---|
| Collector Resistance | \(R_C\) | \(3 \, \text{k}\Omega = 3 \times 10^3 \, \Omega\) |
| Audio Signal Voltage across Collector Resistance | \(V_C\) | \(3 \, \text{V}\) |
| Current Amplification Factor (beta) | \(\beta\) | \(50\) |
| Input Resistance (Base Resistance) | \(R_{in}\) | \(1 \, \text{k}\Omega = 1 \times 10^3 \, \Omega\) |
Solving this problem relies on understanding fundamental principles of transistor operation and applying basic circuit laws:
We will calculate the required values in a sequential manner, starting with the collector current.
First, we need to find the collector current (\(I_C\)). We can do this by using the given audio signal voltage across the collector resistance (\(V_C\)) and the collector resistance (\(R_C\)). According to Ohm's Law:
\(V_C = I_C \times R_C\)
To find \(I_C\), we rearrange the formula:
\(I_C = \frac{V_C}{R_C}\)
Now, substituting the provided values:
\(I_C = \frac{3 \, \text{V}}{3 \times 10^3 \, \Omega} = 1 \times 10^{-3} \, \text{A} = 1 \, \text{mA}\)
Next, we can calculate the base current (\(I_B\)) using the calculated collector current (\(I_C\)) and the given current amplification factor (\(\beta\)). The relationship is defined by the beta value:
\(\beta = \frac{I_C}{I_B}\)
Rearranging the formula to solve for \(I_B\):
\(I_B = \frac{I_C}{\beta}\)
Substituting the values we have:
\(I_B = \frac{1 \times 10^{-3} \, \text{A}}{50} = 0.02 \times 10^{-3} \, \text{A} = 20 \times 10^{-6} \, \text{A} = 20 \, \mu\text{A}\)
Finally, we determine the input voltage (\(V_{in}\)). This is the voltage drop across the input resistance (\(R_{in}\)) due to the flow of the base current (\(I_B\)). We again apply Ohm's Law:
\(V_{in} = I_B \times R_{in}\)
Substitute the calculated \(I_B\) and the given \(R_{in}\):
\(V_{in} = (20 \times 10^{-6} \, \text{A}) \times (1 \times 10^3 \, \Omega)\)
\(V_{in} = 20 \times 10^{-3} \, \text{V} = 0.02 \, \text{V}\)
Based on our detailed calculations, the determined values are:
These values provide a comprehensive solution to the problem.
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