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 $ \mathbb{R} $ denote the set of all real numbers. Then the area of the region $$ \left\{ (x, y) \in \mathbb{R} \times \mathbb{R} : x > 0, y > \frac{1}{x},\ 5x - 4y - 1 > 0,\ 4x + 4y - 17 < 0 \right\} $$ is
The center of a disk of radius $ r $ and mass $ m $ is attached to a spring of spring constant $ k $, inside a ring of radius $ R>r $ as shown in the figure. The other end of the spring is attached on the periphery of the ring. Both the ring and the disk are in the same vertical plane. The disk can only roll along the inside periphery of the ring, without slipping. The spring can only be stretched or compressed along the periphery of the ring, following Hooke’s law. In equilibrium, the disk is at the bottom of the ring. Assuming small displacement of the disc, the time period of oscillation of center of mass of the disk is written as $ T = \frac{2\pi}{\omega} $. The correct expression for $ \omega $ is ( $ g $ is the acceleration due to gravity): 