Frequency of circuit with purely real impedance

[leroyjenkens]

Homework Statement

Two resistors, a capacitor, and an inductor are connected as shown. What is the frequency at which the impedance is purely real?

Diagram below

Homework Equations

Inductor: Z = jwL
Capacitor: Z = \frac{1}{jwL}=\frac{-j}{wC}
Resistor Z = R

The Attempt at a Solution

I added all the components, but I don't see how I can get very far without any values of them.

\frac{1}{\frac{1}{R}+\frac{1}{L}}+\frac{1}{\frac{1}{R}+jwC}

I'm not sure if the capacitor was added correctly, but that's just taken from my notes.

So is that equation I found equal to Z?

I need to set Im[Z] = 0, which is the imaginary part of the impedance, and then solve for w. Did I find Z correctly? And how do I know the imaginary part of Z?

 

[gneill]

Homework Statement

Two resistors, a capacitor, and an inductor are connected as shown. What is the frequency at which the impedance is purely real?

Diagram below

Homework Equations

Inductor: Z = jwL
Capacitor: Z = \frac{1}{jwL}=\frac{-j}{wC}
Resistor Z = R

The Attempt at a Solution

I added all the components, but I don't see how I can get very far without any values of them.

\frac{1}{\frac{1}{R}+\frac{1}{L}}+\frac{1}{\frac{1}{R}+jwC}

I'm not sure if the capacitor was added correctly, but that's just taken from my notes.

So is that equation I found equal to Z?

The impedance of the inductor should involve jω. Your equation shows only L. Otherwise it looks okay.

I need to set Im[Z] = 0, which is the imaginary part of the impedance, and then solve for w. Did I find Z correctly? And how do I know the imaginary part of Z?

You will need to separate the expression into real and imaginary parts (algebraically).

 

[leroyjenkens]

Ok so I have \frac{1}{\frac{1}{R}+\frac{1}{jwL}}+\frac{1}{\frac{1}{R}+jwC}

So now I need to separate the imaginary parts, which are j. I need to have the equation set equal to something for me to be able to do that, right? Since that equation is the Z_{eq}, then I set it equal to that? And then solve for j?

 

[gneill]

Ok so I have \frac{1}{\frac{1}{R}+\frac{1}{jwL}}+\frac{1}{\frac{1}{R}+jwC}

So now I need to separate the imaginary parts, which are j. I need to have the equation set equal to something for me to be able to do that, right? Since that equation is the Z_{eq}, then I set it equal to that? And then solve for j?

Yes, that's an expression for $Z_{eq}$. It's not j that you want to solve for. You want to rearrange the expression so that it is put into the form $Z_{eq} = A + jB$, where A and B are real expressions. In other words, separate the impedance expression into separate real and imaginary parts. Then work out what value of ω will make the imaginary part zero.

 

[leroyjenkens]

So the real parts would be the resistance.

So Z_{eq}=\frac{2}{R}+\frac{jwL}{1+j^2w^2LC}

Well a value of 0 would make the imaginary part 0, wouldn't it?

 

[gneill]

So the real parts would be the resistance.

So Z_{eq}=\frac{2}{R}+\frac{jwL}{1+j^2w^2LC}

Well a value of 0 would make the imaginary part 0, wouldn't it?

Can you expand upon how you arrived at that expression for the impedance?

 

[leroyjenkens]

Yeah, I'm not even sure if I can do that. I inverted both sides of the equation to get rid of the numerator on the right, then I combined the resistance terms, and then flipped it again to get rid of the numerator on the left.

After thinking about it, there's no way that's right, is it?

 

[gneill]

Yeah, I'm not even sure if I can do that. I inverted both sides of the equation to get rid of the numerator on the right, then I combined the resistance terms, and then flipped it again to get rid of the numerator on the left.

After thinking about it, there's no way that's right, is it?

It looks like the way you performed the inversion was not correct.

Invert the two principal terms separately and massage them into canonical form (a + jb) before attempting to add them (or extracting their imaginary parts for addition).

 

[leroyjenkens]

Ok what I'm doing right now on paper is turning into a giant mess.
I multiplied both sides by the denominators, then I tried getting rid of some of the R's by multiplying both sides by R, but now this looks like I have no where else to go. I have Z's, j's, L's, and w's everywhere.

This isn't the way this problem is supposed to be solved, is it?

I'm not even sure what this thing would look like if it was in A + jB form. The A term is supposed to be just the resistance? What is the B term? Everything stuck to the j's? I'm so confused. I wish books actually explained stuff instead of just mentioning stuff.

 

[gneill]

Ok what I'm doing right now on paper is turning into a giant mess.
I multiplied both sides by the denominators, then I tried getting rid of some of the R's by multiplying both sides by R, but now this looks like I have no where else to go. I have Z's, j's, L's, and w's everywhere.

This isn't the way this problem is supposed to be solved, is it?

I'm not even sure what this thing would look like if it was in A + jB form. The A term is supposed to be just the resistance? What is the B term? Everything stuck to the j's? I'm so confused. I wish books actually explained stuff instead of just mentioning stuff.

Yeah, it can get a bit messy and tedious working with complex algebra. But it's what has to be done here.

Start with just one of the main terms, say the inductor in parallel with the resistor and see if you can simplify it into the normalized form. You can use the "two resistor expression" for parallel resistors to begin if you wish:
$$z1 = \frac{R \cdot jωL}{R + jωL}$$
Clear the imaginary from the denominator.

Then do the same thing for the other, capacitor term.

 

[leroyjenkens]

Just so I'm clear, the imaginary part is the j, right? Well in my notes I found something that might be useful. This is from a parallel RLC circuit:

Z_{eff}=\frac{1}{\frac{1}{R}+\frac{1}{jwL}+jwc}

Then the next line

=\frac{1}{\frac{1}{R}+j(wc-\frac{1}{wL})}

How did that j get factored out? In one term it's in the numerator and the other it's in the denominator.

But then the absolute value of Z_{eff} is given:

|Z_{eff}|=\frac{1}{\sqrt{(\frac{1}{R})^2+(wc-\frac{1}{wL})^2}}

Where did the j go in this last one? It just disappeared.

But to do what you asked, I multiplied both sides by the denominator and then did a little rearranging to get only the j's on the right side and I got:

Z_1=RjwL+(jwL)^2-\frac{Z_1jwL}{R}

I'm kinda confused on which letters are considered imaginary and which ones aren't, because if it's just the j that's considered imaginary, then I can't isolate it from the rest of the variables.

 

[gneill]

Yes, the terms with j multiplying them are imaginary. j is the variable name associated with $\sqrt{-1}$. j can "disappear" if it is multiplied by j (so it's squared) as j² = -1.

It sounds like you should take a few minutes to review the properties and basic manipulations of imaginary numbers.

 

[leroyjenkens]

But in that last expression, everything was raised to the second power? Well, the reason I said it disappeared was because the + sign in front of it stayed +. If j just turned into a -1, then that + would turn into a -, right?

I also don't understand how that j was factored out in the 1st one.

 

[gneill]

But in that last expression, everything was raised to the second power? Well, the reason I said it disappeared was because the + sign in front of it stayed +. If j just turned into a -1, then that + would turn into a -, right?

The last expression is finding the magnitude of the complex expression. The real and imaginary parts add in quadrature (square root of sum of squares). This is a property of imaginary numbers that you need to know.

I also don't understand how that j was factored out in the 1st one.

Multiply the numerator and denomination of the 1/(jωL) term by j.

 

[ehild]

Ok so I have \frac{1}{\frac{1}{R}+\frac{1}{jwL}}+\frac{1}{\frac{1}{R}+jwC}

So now I need to separate the imaginary parts, which are j. I need to have the equation set equal to something for me to be able to do that, right? Since that equation is the Z_{eq}, then I set it equal to that? And then solve for j?

The calculation is simpler if you make the denominators real, by multiplying both the numerator and the denominator by the complex conjugate of the denominator.
The RL part becomes
Z_{RL}= \frac {1}{\frac{1}{R}+ \frac{1}{jwL} }=\frac{\frac{1}{R}-\frac{1}{jwL}}{(\frac{1}{R}+\frac{1}{jwL})(\frac{1}{R}-\frac{1}{jwL})}=\frac{\frac{1}{R}-\frac{1}{jwL}}{(\frac{1}{R})^2+(\frac{1}{wL})^2}

Decomposing into real and imaginary terms, the RL term of the impedance is

Z_{RL}=\frac{\frac{1}{R}}{(\frac{1}{R})^2+(\frac{1}{wL})^2}+j\frac{\frac{1}{wL}}{(\frac{1}{R})^2 + ( \frac{1}{wL} )^2 }


Do the same with the capacitor term. Simplify, add the imaginary parts and make the sum zero.

ehild