Step 1: Power in terms of voltage and resistance
The formula for power is given by:
\( P = \frac{V^2}{2} \)
We are given that the power \( P = 500 \) W, so:
\( 500 = \frac{100^2}{R} \)
Solving for \( R \), we get:
\( R = 20 \, \Omega \)
Step 2: Current calculation
Using Ohm's law across the resistor, we know:
\( P = I_{\text{rms}} \times V_{\text{rms}} \)
Given that \( P = 500 \) W and \( V_{\text{rms}} = 100 \) V, we can calculate the current \( I_{\text{rms}} \):
\[
500 = I_{\text{rms}} \times 100
\]
Solving for \( I_{\text{rms}} \), we get:
\( I_{\text{rms}} = 5 \, \text{A} \)
Step 3: Voltage and real power comparison
The RMS voltage across the resistance is given as \( V_{\text{rms}} = 200 \) V.
The real voltage (effective voltage) is 100 V, so the ratio is:
\( \frac{V_{\text{rms}}}{\text{real}} = 100 \, \text{V} \)
Step 4: Calculating the phase angle \( \varphi \)
The power factor \( \cos \varphi \) is the ratio of the real voltage to the RMS voltage:
\( \cos \varphi = \frac{100}{200} = \frac{1}{2} \)
Thus, the phase angle \( \varphi \) is:
\( \varphi = 60^\circ \)
Step 5: Calculate the reactance \( X_C \) and capacitance \( C \)
The relationship between reactance \( X_C \), resistance \( R \), and the phase angle \( \varphi \) is given by:
\( \tan \varphi = \frac{X_C}{R} = \frac{1}{\omega R C} \)
Using the value of \( \tan 60^\circ = \sqrt{3} \), we have:
\[
\sqrt{3} = \frac{1}{100\pi(20)C}
\]
Solving for \( C \), we get:
\[
C = \frac{1}{20\pi\sqrt{3} \times 100}
\]
Simplifying further:
\[
C = 10^{-4} \, \text{F}
\]
Final Answer:
The capacitance \( C \) is \( 10^{-4} \, \text{F} = 100 \, \mu\text{F} \).
Step 1: Power in terms of voltage and resistance
The formula for power is given by:
\( P = \frac{V^2}{2} \)
We are given that the power \( P = 500 \) W, so:
\( 500 = \frac{100^2}{R} \)
Solving for \( R \), we get:
\( R = 20 \, \Omega \)
Step 2: Current calculation
Using Ohm's law across the resistor, we know:
\( P = I_{\text{rms}} \times V_{\text{rms}} \)
Given that \( P = 500 \) W and \( V_{\text{rms}} = 100 \) V, we can calculate the current \( I_{\text{rms}} \):
\( 500 = I_{\text{rms}} \times 100 \)
Solving for \( I_{\text{rms}} \), we get:
\( I_{\text{rms}} = 5 \, \text{A} \)
Step 3: Voltage and real power comparison
The RMS voltage across the resistance is given as \( V_{\text{rms}} = 200 \) V.
The real voltage (effective voltage) is 100 V, so the ratio is:
\( \frac{V_{\text{rms}}}{\text{real}} = 100 \, \text{V} \)
Step 4: Calculating the phase angle \( \varphi \)
The power factor \( \cos \varphi \) is the ratio of the real voltage to the RMS voltage:
\( \cos \varphi = \frac{100}{200} = \frac{1}{2} \)
Thus, the phase angle \( \varphi \) is:
\( \varphi = 60^\circ \)
Final Answer:
The phase angle \( \varphi \) is \( 60^\circ \).
Let $ a_0, a_1, ..., a_{23} $ be real numbers such that $$ \left(1 + \frac{2}{5}x \right)^{23} = \sum_{i=0}^{23} a_i x^i $$ for every real number $ x $. Let $ a_r $ be the largest among the numbers $ a_j $ for $ 0 \leq j \leq 23 $. Then the value of $ r $ is ________.
Let $ y(x) $ be the solution of the differential equation $$ x^2 \frac{dy}{dx} + xy = x^2 + y^2, \quad x > \frac{1}{e}, $$ satisfying $ y(1) = 0 $. Then the value of $ 2 \cdot \frac{(y(e))^2}{y(e^2)} $ is ________.
The left and right compartments of a thermally isolated container of length $L$ are separated by a thermally conducting, movable piston of area $A$. The left and right compartments are filled with $\frac{3}{2}$ and 1 moles of an ideal gas, respectively. In the left compartment the piston is attached by a spring with spring constant $k$ and natural length $\frac{2L}{5}$. In thermodynamic equilibrium, the piston is at a distance $\frac{L}{2}$ from the left and right edges of the container as shown in the figure. Under the above conditions, if the pressure in the right compartment is $P = \frac{kL}{A} \alpha$, then the value of $\alpha$ is ____