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b) Three impedances are connected in parallel. \( Z_{1}=2 j+5, Z_{2}=3-j, Z_{3}=4 j \). Find the equivalent admittance \( Y \) where \[ Y=\frac{1}{Z_{1}}+\frac{1}{Z_{2}}+\frac{1}{Z_{3}} \] Express the admittance in both rectangular and polar forms. Rectangular form Polar form

Ask by Ellis Beck. in the United Kingdom
Feb 18,2025

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The equivalent admittance \( Y \) is: - **Rectangular Form**: \( Y = 0.472 - j0.219 \) - **Polar Form**: \( Y \approx 0.521 \angle -25^\circ \)

Solution

We are given three impedances in parallel:   Z₁ = 5 + 2j   Z₂ = 3 − j   Z₃ = 4j The equivalent admittance is the sum of the reciprocals:   Y = 1/Z₁ + 1/Z₂ + 1/Z₃ We will find Y in both rectangular and polar forms. ───────────────────────────── Step 1. Compute the reciprocal of each impedance: 1. For Z₁ = 5 + 2j, its reciprocal is   1/Z₁ = 1/(5+2j). Multiply numerator and denominator by the complex conjugate (5 − 2j):   1/Z₁ = (5 − 2j) / [(5)² + (2)²] = (5 − 2j) / (25+4) = (5 − 2j) / 29. 2. For Z₂ = 3 − j,   1/Z₂ = 1/(3 − j). Multiply by the conjugate (3 + j):   1/Z₂ = (3 + j) / [(3)² + (1)²] = (3 + j) / (9+1) = (3 + j) / 10. 3. For Z₃ = 4j,   1/Z₃ = 1/(4j). Recall that 1/j = –j so that:   1/Z₃ = 1/(4j) = (1/4) (1/j) = –j/4. ───────────────────────────── Step 2. Sum the reciprocals: Write each term in rectangular form:   1/Z₁ = (5/29) – (2/29)j   1/Z₂ = (3/10) + (1/10)j   1/Z₃ = 0 – (1/4)j Now, add the real parts:   Real(Y) = (5/29) + (3/10). Find a common denominator (the least common denominator of 29 and 10 is 290):   5/29 = (5×10)/290 = 50/290   3/10 = (3×29)/290 = 87/290 So, Real(Y) = (50 + 87)/290 = 137/290. Next, add the imaginary parts:   Imag(Y) = –(2/29) + (1/10) – (1/4). Again, using a common denominator of 290 (or 580; here we use 580 for clarity):   Convert each term:    –2/29 = –(2×20)/580 = –40/580    1/10 = (1×58)/580 = 58/580    –1/4 = –(1×145)/580 = –145/580 Then,   Imag(Y) = (–40 + 58 – 145)/580 = –127/580. Thus, the equivalent admittance in rectangular form is:   Y = (137/290) – j(127/580). To give approximate decimal values:   137/290 ≈ 0.4724, 127/580 ≈ 0.21897, so   Y ≈ 0.4724 – j0.2190. ───────────────────────────── Step 3. Express Y in polar form a) Compute the magnitude |Y|:   |Y| = √[(Real(Y))² + (Imag(Y))²]    = √[(0.4724)² + (–0.2190)²]    ≈ √[0.2232 + 0.0480]    ≈ √0.2712    ≈ 0.5208. b) Compute the phase angle θ (in degrees):   θ = arctan(Imag(Y) / Real(Y))    = arctan(–0.2190 / 0.4724)    ≈ arctan(–0.4638)    ≈ –25°. ───────────────────────────── Answer Summary Rectangular form:   Y = (137/290) – j(127/580)   or approximately  0.472 – j0.219 Polar form:   Y ≈ 0.521∠–25° Either form, with appropriate rounding, is acceptable.

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To find the equivalent admittance \( Y \), we first need to compute the individual admittances of each impedance: 1. For \( Z_{1} = 2j + 5 \): \[ Y_{1} = \frac{1}{Z_{1}} = \frac{1}{5 + 2j} \] Multiply numerator and denominator by the conjugate: \[ Y_{1} = \frac{5 - 2j}{(5)^{2} + (2)^{2}} = \frac{5 - 2j}{29} = \frac{5}{29} - \frac{2}{29}j \] 2. For \( Z_{2} = 3 - j \): \[ Y_{2} = \frac{1}{Z_{2}} = \frac{1}{3 - j} \] Multiply numerator and denominator by the conjugate: \[ Y_{2} = \frac{3 + j}{(3)^{2} + (1)^{2}} = \frac{3 + j}{10} = \frac{3}{10} + \frac{1}{10}j \] 3. For \( Z_{3} = 4j \): \[ Y_{3} = \frac{1}{Z_{3}} = \frac{1}{4j} = -\frac{j}{4} \] Now we add the individual admittances: \[ Y = Y_{1} + Y_{2} + Y_{3} = \left( \frac{5}{29} - \frac{2}{29}j \right) + \left( \frac{3}{10} + \frac{1}{10}j \right) + \left( 0 - \frac{1}{4}j \right) \] To combine, we need a common denominator. The least common multiple of \( 29, 10, \) and \( 4 \) is \( 580 \). Converting each term: - \( Y_{1} = \frac{5}{29} - \frac{2}{29}j = \frac{100}{580} - \frac{40}{580}j \) - \( Y_{2} = \frac{3}{10} + \frac{1}{10}j = \frac{174}{580} + \frac{58}{580}j \) - \( Y_{3} = 0 - \frac{1}{4}j = 0 - \frac{145}{580}j \) Now, let's sum the real and imaginary parts: Real part: \[ \frac{100}{580} + \frac{174}{580} = \frac{274}{580} \] Imaginary part: \[ -\frac{40}{580} + \frac{58}{580} - \frac{145}{580} = -\frac{127}{580} \] So the equivalent admittance in rectangular form is: \[ Y = \frac{274}{580} - \frac{127}{580}j \] Now, we can convert this to polar form: 1. Find the magnitude: \[ |Y| = \sqrt{\left( \frac{274}{580} \right)^{2} + \left( -\frac{127}{580} \right)^{2}} = \sqrt{\frac{75076 + 16129}{336400}} = \sqrt{\frac{91105}{336400}} \approx 0.494 \] 2. Find the phase angle: \[ \theta = \tan^{-1} \left( \frac{-127/580}{274/580} \right) = \tan^{-1} \left( -\frac{127}{274} \right) \] Calculating \( \theta \): \[ \theta \approx -0.433 \text{ radians} \approx -24.8^\circ \] So the equivalent admittance in polar form is: \[ Y \approx 0.494 \angle -24.8^\circ \] In conclusion, the equivalent admittance is: - Rectangular form: \( Y \approx \frac{137}{290} - \frac{127}{580}j \) - Polar form: \( Y \approx 0.494 \angle -24.8^\circ \)

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