Welcome to the 15th lecture in the course Engineering Electromagnetics. In this lecture also we continue with our discussion on wave propagation. The aspects that we consider in today's lecture are the following. We first consider the power flow in terms of the pointing vector and then go on to consider complex pointing vector along the lines of complex power flow and then we go on to discussing the wave propagation in conducting media and start with deriving the wave equation for conducting media. Taking up the first topic the power flow, you would recall that in the previous lecture we introduced the concept of pointing vector and we said that the pointing vector represented by P and given as the cross product of the electric field vector E and the magnetic field vector H is a measure of the power flow per unit area. Now this concept of expressing the power flow in terms of the field vectors is new to us. We are more familiar with power being described in terms of the product of voltage in current and therefore it will be interesting to see how this new concept of expressing power in terms of the product of the field vectors correspond to or is consistent with the other descriptions that we are familiar with. So for this purpose let's first take the example of a uniform plane wave and we try to determine the power flow associated with the uniform plane wave per unit area through some alternative means and then see how that corresponds to the statement of the pointing theorem that the pointing vector P equal to E cross H is the measure of the power flow per unit area. So let's say that there is a uniform plane wave with associated fields E and H propagating in some direction along one of the axis of the Cartesian coordinate system. Now how can we arrive at a description of the power flow? So for that purpose we write the power flow per unit area is equal to let's consider a unit volume and consider the energy stored in that unit volume which will be the energy stored per unit volume or the energy density. Now if we consider the speed at which this energy stored in a unit volume crosses the cross section of that unit volume that will give us the power flow per unit area like we have been doing the sums in mathematics finding out the volume of water flowing out of a pipe given the cross section of the pipe and the velocity of water etc. So similarly we can write here power flow per unit area is the energy density multiplied by the velocity which should give us in magnitude and direction since we are using velocity the power flow per unit area. Now as far as the first term on the right hand side is concerned the energy density that we know what is the energy density associated with the electric field and what is the energy density associated with the magnetic field. So using that we write half epsilon e square plus mu h square which is a scalar quantity this we multiply by the vector v not representing the velocity of the wave that should be the power flow per unit area. Then we manipulated in simple manner to see how it corresponds to the pointing vector. We are aware that for a uniform plane wave E and H are related through the intrinsic impedance of the medium. Overall electric field and the overall magnetic field are related in this manner E by H is equal to the intrinsic impedance eta of the medium. So we use that relation and replace E in the first term by eta H and H in the second term by E by eta. So that we get half and then epsilon or epsilon eta E H on one hand and mu by eta E H on the other hand multiplied by the velocity vector. We further realize that since eta is equal to square root of mu by epsilon for a perfect dielectric having no conductivity. These terms both of these the factors multiplying E H they are equal and they are equal to half square root of mu epsilon E H plus square root of mu epsilon E H times v not or it is E H by v not times v not recognizing that for a uniform plane wave v not is 1 by square root of mu epsilon mu and epsilon being the permeability and the permittivity of the medium alright. But therefore this is equal to E H times a unit vector in the direction of the movement of the wave the direction in which the wave is propagating. And we have already derived a relation for uniform plane waves that it is the cross product of E and H which is in the direction of the propagation of the wave and also for a plane wave uniform plane wave E and H are mutually perpendicular. Using these two results this is simply E cross H in magnitude and direction. So what we have done is that for a uniform plane wave starting with some description of the power flow per unit area we have reached a result that it is equal to the pointing vector E cross H and therefore this new notion that we have introduced is quite consistent with the alternative descriptions of power flow. The example that we have taken involved fields waves in infinite media or in free space are described in terms of fields and therefore that the power flow is coming out in terms of fields is perhaps quite alright. But we have stated earlier that the fields description is a more accurate description is a more general description and voltage and current descriptions are special cases of the fields description. So is it possible to see some in some situation where the power flow is given in terms of the voltage and current product how that corresponds to the pointing vector E cross H that should be even more interesting and for that purpose we consider the example of let us say a coaxial cable. We consider the usual coaxial cable with the with an inner and outer conductor in this manner and we consider that there is a voltage that is applied between the inner and the outer conductor. The inner and the outer conductors are connected through some resistance R and a current I flows in this direction in the inner conductor and an equivalent opposite current I flows in the outer conductor. We know that the power flow in this assuming that this is a DC situation there is no time variation is going to be the product of the potential difference between the two conductors and the current that is flowing in one of the conductors that is VI. We want to see how it corresponds to the pointing vector description for the power flow. So we need to evaluate the electric and the magnetic field associated with the system and if we redraw the cross section let us say this is the x and the y axis and this is the radial direction and this is the angle theta so that theta cap is in a direction normal to the radial direction. Let the radii of the inner and outer conductors be A and B and let this be the z direction coming out of the plane of the blackboard. Now what is the magnetic field between the two conductors in the space between the two conductors? It will be I by 2 pi R in the direction theta cap as I methodally oriented symmetric with respect to theta same value at all values of theta since it is a symmetric structure but varying with R. Strongest close to the inner conductor and weakest close to the outer conductor. What is the electric field? This we have derived earlier we can use the expression straight away it is V upon R natural log of B by A and if the inner conductor is at a greater potential then it is the radial direction in which the electric field lines would be there. Now we find out the pointing vector P which will be E cross H which will be V i upon 2 pi R squared natural log of B by A in what direction? R cap cross theta cap therefore that will be the z cap direction. What is the interpretation of the pointing vector that we have been giving? We have said that it is a measure of the power flow per unit area. So for total power flow associated with the system we need to integrate it we need to perform an area integral over the space where the fields are non zero. So that is the space between the two conductors and if we consider some element of area which is concentric with the system and has a thickness which is dr and has a radius R then the power flow through this area will be the pointing vector times the area of this element which will be V i by natural log of B by A then into 2 pi R squared times the area of this element which will be 2 pi R dr. What we are doing is we are writing P dot da which is equal to this and if we integrate this over the surface over which the fields are non zero we will get the total power flow so integrating from A to B. So the total power flow is going to be V i by log B by A and integral of dr by R from A to B now the integral is exactly equal to the term in the denominator and therefore this is equal to V i the power flow. So it shows very clearly that the concept that we have stated now that the pointing vector equal to E cross H is a measure of the power flow per unit area is completely consistent with any other alternative description of the power flow as we saw for the uniform plane wave and as we have seen for the coaxial cable. Now one thing is very noteworthy here what was the area of integration for determining the total power flow the area of integration was the entire region where the fields were non zero that was the space between the two conductors in the coaxial cable and it excluded the conducting regions. So from this point of view where is the power flowing it is flowing in the non conducting region in the region between the two conductors and therefore this is at some variance with our somewhat mistaken notion that the power flows in conductors and the greater the power flow the thicker the conductors. Actually conductors only provide a means for conducting current and to guide the wave associated with the power flow or the for the transfer of power flow. And their thickness is decided from the consideration of keeping the losses as low as possible and from the point of view of providing sufficient mechanical strength. So that is the advantage of the fields point of view we get a clearer picture of the phenomenon of power flow and the transfer of power. From this point onwards we now shift to the second topic that we will state for today and that is the complex pointing vector. You would recall that we use the concept of complex power at low frequencies. So we draw upon the same notion here and introduce the notion of complex pointing vector through the notion of complex power and we consider a situation where we have voltage in current phasors which are let us say like this with respect to some reference the voltage phasor let us say is like this. It has a magnitude V and it makes an angle theta V with respect to the reference and as time advances it rotates that is the concept of the phasor representation. Let us say the associated current phasor is like this with an associated magnitude I and an angle theta I. So that the angle between these two phasors theta V minus theta I is theta. Now we try to go back to the time varying voltage and current from these phasors so that the time varying voltage is going to be real of the voltage phasor V times e to the power j omega t which becomes magnitude of V and then cosine of omega t minus theta V that one can see here straight forward manner. Similarly the time varying current is going to be magnitude of it is going to be real of I times e to the power j omega t and through similar considerations it is going to be magnitude of I times cosine of omega t minus theta I. That is all right you are right omega t plus theta V and omega t plus theta I there is no reason for it to be negate. Now let us consider the instantaneous power flow instantaneous power flow we represent this as W is going to be the product of time varying V and I and therefore it is going to be magnitude of V times magnitude of I and then cosine of omega t plus theta V and cosine of omega t minus theta I which can be expressed as a sum and difference of these two angles thank you so that it is magnitude V times magnitude I by 2 and then we have cosine of theta V minus theta I plus cosine of 2 omega t plus theta V plus theta I. Now if we consider the average power averaged over a period of sinusoidal time variation then the second term is going to average to 0. This has an average value which is 0 and as far as the average power is concerned it is only the first term that will remain and we obtain W average equal to half magnitude of V magnitude of I times cosine of theta V minus theta I. Continuing on the other side we rewrite this as the average power equal to half magnitude V magnitude I into cosine of theta where theta is the difference between the phasor angles of the voltage phasor and the current phasor. Corresponding to this one also sometimes talks of the reactive power which is written as half magnitude V magnitude I times sin theta and cos theta is known as the power factor in power system terminology. Now let us introduce the notion of complex power and we say that let complex power W be half V I star where star stands for the complex conjugate of the current phasor which one can see is going to be half magnitude of V magnitude of I and then e to the power j theta V minus theta I or half magnitude of V magnitude of I e to the power j theta which is W average plus j W reactive and therefore we are in a position to say that the average power flow is equal to half real of V I star where V and I are the voltage and the current phasors. So, here we have introduced the instantaneous power, the average power and the complex power and how the average power can be calculated when we have phasor quantities available. W average is half real of V I star. So, following this same notation we are now in a position to write that the instantaneous power flow or the instantaneous pointing vector and designating it like this is going to be e cross h and the complex pointing vector is going to be what? It will be P equal to half e cross h star writing exactly corresponding relations to what we wrote for the voltage and current description. So, that the average pointing vector P average becomes half real of e cross h star. For sinusoidal time varying signals e and h phasors would be available to us and this is how we can calculate the average power flow per unit area or the average pointing vector. Continuing further if we want to specialize this to the case of a uniform plane wave propagating in the z direction then what would be the power flow in the z direction per unit area that we can work out for a z directed uniform plane wave. We will have x and y electric and magnetic field components and the cross product in such a case can be written easily and we will have P z in such a case power flow in the z direction per unit area equal to half real of e x h y star minus e y h x star which of course could be converted to uniform plane waves propagating in other directions through a similar procedure. Next we like to apply this to some specific cases and see what is the effect of polarization on the power flow description and some important differences in the case of the linearly polarized waves and those of the circularly polarized waves would emerge. We apply this to uniform plane waves and we first consider the case of linear polarization. Sir, this expression for P z is itself real e x h y star. Not necessarily. Sir, e x can be written in terms of h y h y star is mod f i 4. We need to apply it to different cases. For uniform plane waves. Yeah, for uniform plane waves for example for the elliptically polarized waves it may not come out real. There can be situations where this may not be real. That is why that is put. For the linearly polarized uniform plane wave what kind of electric field expression can be right? We consider that the wave is propagating in the z direction therefore what can be right for the electric field vector? For the wave to be propagating in the z direction we can have x and y components of the electric field vector. That is one thing. Second thing is for it to be linearly polarized they must be in phase. Both x and y field components must be in phase. That is the most general description of a linearly polarized wave. One or the other field component x or y may be absent. That is a special case. And therefore we write e equal to let us say a x cap plus b y cap. And of course in phasor notation factor e to the power minus j beta z for a wave propagating in the z direction. Now how do we obtain the magnetic field intensity vector? We recall the relations between the electric and the magnetic field components in terms of the intrinsic impedance. And for this case they will become e x by h y equal to eta and e y by h x equal to minus eta. So that h x is equal to minus e y by eta and h y is equal to e x by eta. And therefore here we will have 1 by eta on one hand. And the x component is minus b by eta x cap and the y component is a by eta. Eta is already taken out common. So we do not need to write it here minus b plus a y cap and of course e to the power minus j beta z. And now we apply the formula that we have derived for a wave propagating in the z direction in terms of the products of the various components and taking the complex conjugate. And in that case we get real of e x times h y star that gives us a square. These two factors cancel out because of the product of the quantity with the complex conjugate. And similarly the other term gives us plus b square applying minus e y times h x star. Assuming that a and b are real this is simply going to be e square by 2 eta or alternatively it will be half eta h squared h squared standing for the square of the magnitude of the magnetic field intensity. Now the appearance of the factor half can be related to the sinusoidally time varying field quantities. We are considering a linearly polarized wave and in the x y plane depending on the ratio of a and b the field vector electric field vector is oscillating along this direction is having different magnitudes. But the orientation remains unchanged and it is varying sinusoidally with time and therefore on an average the power flow becomes half e squared by eta or similarly half eta times h squared quite reasonable. If we consider a circularly polarized wave let us see what happens. How will we construct a circularly polarized wave? Here we stick to z directed plane wave that is all right. So, we will have x and y components. But for the wave to be circularly polarized the magnitudes of these two components must be identical and there must be a phase difference of 90 degrees. So, let us say we write it as x cap plus j y cap times e naught and e to the power minus j beta say which is a circularly polarized wave. If we look at it carefully it will be a left circularly polarized wave. This describes the phase shift in the wave as the wave propagates in the positive z direction. Now, the magnetic field description can be obtained in a similar manner using these relations and we are going to get h equal to 1 by eta and then h x is minus e y by eta. Therefore, it will be minus j times x cap and h y is e x by eta. So, that it is simply plus y cap and e naught e to the power minus j beta z. And now we apply this relation that we have written for a uniform plane wave propagating in the z direction and the real power flow per unit area given by these terms. This is e y and this is h x star. So, what do we get?  So, this is plus 1 and here one can see that if the phase difference were not 90 degrees one would not get a quantity which is already real. Then the real part will have to be considered which is simply eta also comes here which is simply e naught squared by eta the factor 2 in the denominator goes away or e squared by eta or alternatively eta times h squared. Now one can understand the difference between this final result for the circular polarization and this result for linear polarization in two different ways. One could either consider that the circularly polarized wave is a superposition of two linearly polarized waves each one having the same amplitude. So, each one will have a result like this and therefore, the total power associated with the circularly polarized wave is twice that. So, it is e squared by eta or else one could consider the behavior of the circularly polarized wave electric field vector. And what does it look like? It is an electric field vector with magnitude e naught rotating in the x y plane in this case in this direction. So, as a function of time is the electric field vector magnitude changing it is not changing. And therefore, from the point of view of mathematics a factor half is not required when we consider the average power whichever root appeals to you this is the result for circularly polarized waves and this is the result for linearly polarized waves. This small difference one should keep in mind. Also many times the RMS values are specified corresponding to phasor quantities and if they are given then one can see that this is going to be 1 by eta times e RMS squared or alternatively eta times h RMS squared which extension is quite straight forward. While we are discussing the polarization and the power flow associated with waves of different polarizations one important character of polarization must be mentioned. Supposing an antenna is transmitting a wave which is x polarized linearly polarized wave and the electric field vector is oriented in the x direction. Now if this signal is to be received the receiving antenna must be able to respond to this x directed polarization. If it is so oriented if the receiving antenna is so oriented that it responds to y directed polarization not to x directed polarization the signal received at the receiver will be nil. In such a case we would say that the receiving antenna is oriented for a polarization which is orthogonal to the polarization transmitted by the transmitting antenna. This is the reason why our radio and TV receptions improve when we maneuver the antennas and when they correspond when their orientation corresponds to the polarization of the incident wave then we get a strong signal and not otherwise. It is very easy to see that if it is a linearly polarized wave then what would be the orthogonal polarization?  So this kind of orthogonal polarization can be utilized to increase the information handling capability capacity of communication systems. They could be operated transmitting two different signals in two different in two orthogonal polarizations which would be non interfering with each other. Now just as for linear polarization one can identify an appropriate orthogonal polarization is the same thing possible for circularly polarized signals. The answer is yes and one can show this using the following example. We have just seen that this is one kind of circularly polarized wave left circularly polarized wave. So let one wave be represented as e 1 equal to x cap plus j y cap let us say e 1 and e to the power minus j beta z. And let us consider another wave e 2 which is right circularly polarized all we need to do is to change the 90 degree phase difference. If this is ahead in phase by 90 degrees if we retard this in phase by 90 degrees it becomes a right circularly polarized wave. So we write e 2 equal to x cap minus j y cap say e 2 e to the power minus j beta z both travelling in the positive z direction. The corresponding components time varying components can be obtained by multiplying by e to the power j omega t and taking the real part. So here we will get e x 1 the time varying part equal to e 1 cosine omega t cosine of omega t minus beta z actually but then we can consider the behavior at z equal to 0. Similarly what will be the time varying e y 1 realizing that there is a factor j here this will be minus e 1 sin omega t again at z equal to 0. Similarly we can put down the time varying field components here e x 2 at z equal to 0 will be e 2 cos omega t and e y 2 will be e 2 sin omega t. Now let us take a dot product of the time varying electric field vectors that is e 1 dot e 2. So that the corresponding components get multiplied and get added that is how the dot product is going to be taken. So we get this as e 1 e 2 which comes out as a common factor and we have cos squared omega t minus sin squared omega t or it is e 1 e 2 times cosine of 2 omega t and if we consider the average value of this quantity that is going to be 0 over a period of sinusoidal time variation. So from this point of view these two polarizations are orthogonal to each other and antenna oriented or designed to receive right circularly polarized wave will receive on an average a 0 signal if a left circularly polarized wave is incident on it. So for circularly polarized waves also the concept of orthogonal polarization is possible and many times when we need to increase the capacity of communication systems which are using circular polarization we can use this concept. We could transmit signals in right circularly polarized manner for one signal and using the left circularly polarized wave for the other signal and these would not interfere. If there are any questions up to this point we can try those out now. Otherwise we go on to considering the third topic for the day and that is the consideration of wave propagation in conducting medium. Now do we expect any difference in the behavior of a propagating wave in a conducting medium compared to that in free space or in a perfect electric. It is for the latter situations that we have got all the results. Now we want to consider if there are any differences that arise when we allow the medium to be conducting that is the medium is not a perfect electric. Where would a difference occur? We go back to the Maxwell's equations and we see that the first equation del cross h equal to epsilon del e by del t. This is what we wrote when we considered a perfect electric medium or free space. Of course we made the simplifying assumptions of the medium being homogeneous and isotropic and further source free. When the medium is conducting there will be a conduction current associated with the electric field. So a conduction current term must appear here when we want to consider wave propagation in conducting medium. This is where a difference would occur. Of course where j is equal to sigma times e sigma being the conductivity of the medium. Of course if sigma is 0 then we go back to the perfect electric situation. We write the other Maxwell's equations that is del cross e equal to minus mu del h by del t del dot e equal to 0 and del dot h also equal to 0. So we are still considering a source free region in which we will consider the behavior of either the electric field alone or the magnetic field alone. And this conduction current term which is appearing is because of the finite conductivity of the medium not because of any source being present in the region of consideration. The procedure is going to be similar to what we did earlier for perfect dielectric. We number these equations say 1, 2, 3 and 4 then from equation 2 if we take the curl on both sides we get del cross del cross e equal to minus mu curl of del h by del t. Then the curl of curl of e can be written as del of del dot e gradient of divergence minus del square e the Naplesian operation on the electric field vector. And on the right hand side we interchange the time derivative and the space derivative these being linear operations so minus mu del by del t of del cross h. And now from equations 3 and 1 equation 3 will allow us to see that the first term on the left hand side is 0 and equation 1 will allow us to replace del cross h in terms of the right hand side. And therefore, we get minus del square e equal to minus mu del by del t of epsilon del e by del t plus j or which is sigma e. And therefore, we get del 2 e minus mu epsilon del 2 e by del t square minus mu sigma del e by del t equal to 0 which is the wave equation for the electric field in an infinite conducting medium. And of course, if sigma goes to 0 we get back the wave equation for perfect dielectric meeting. This is where we stop today. Today in this lecture we have given examples of power flow in different situations and shown how the concept of power flow in terms of pointing vector is consistent with these different descriptions. We introduce the notion of complex pointing vector and then we have gone on to introduce the wave equation in conducting media. Thank you.


Wazel, Wazel, Wazel. Top of the morning to you from Stevenville, Newfoundland. We're here in Stevenville, trying to figure out what's going on. I just woke up about 30 seconds ago. Morning, how are you? Diesel, how are you today? You've probably been up way longer than me. He's always a creeper in the morning. I always wake up and he's just sitting there staring at me. And then as soon as he knows I'm awake, I've got to be very careful if I wake up and I don't want to get up yet. As soon as he knows I'm awake, he like starts dancing and whining. He's so excited that I'm awake and he wants to go outside. Oh, then he's got to wait for me to get dressed and wait for me to get everything cleaned up. And oh, there's torture for the poor fella. Anyway guys, we're across the street from Walmart. We got to run in there again because my phone charger died throughout the night. I don't know, it's just not working. So I got to go get a new one. I guess there's so many phone chargers, it's frustrating. Just want a good one that's going to last a while. Cause this is what everyone loves to do first thing in the morning, go for an ice long freezing cold walk. Wicks, yep, pretty quick, that's for sure. All right, so we got the new charger. Chargers aren't cheap, did you know that? Chargers are not cheap. And mine keep burning out or stopping. And they don't charge anymore, that's no fun. I need to charge my phones. Oh well, so we got that done. Oh, just ran in, ran out. Still trying to wake up here.  We'll be off to the ferry. So we got to hurry up and wait. That right there is the Atlantic Ocean. So we're just about in Porto Basque. I just got to do some work here yet before we get to the ferry. Got to get everything ready for when I get to the mainland. I'll quickly take care of all of that and then we'll be off and get in line for the ferry. In the meantime, I thought I'd stop and have this magnificent view in front of me. We are on the west side of the island. So on the other side of this ocean is actually, we're facing Canada right now. We're in Canada, but we're facing the mainland. You go straight across this ocean right there and you'd probably end up in Labrador or Quebec. Quebec. So they got some like chairs up there on the hill. You see that there? Just behind us, we have this. Amazing, eh? Beautiful Newfoundland. What'd you think, Diesel? What'd you think? You even got a paved trail here, man. Where do you think it goes? Where do you think the trail goes, man? It's not okay, man. I don't want the trail. I want the grass. Way as well. Explored just a little bit, just for a little while. I am king of this mountain. What'd you think, man? That's a cliff, man. Never seen a cliff before, have you? We're from Manitoba. That's the ocean. And that's a cliff. Neither of which are anywhere near Manitoba. Anyone up for a stroll on the beach? Careful, buddy. Now speak for yourself, man. I got four-wheel drive. So he does. Four-wheel drive is always better than two-wheel drive. Tell you what. Ha, ha, ha, ha, ha. Okay, we'll go this way. This way it looks a little safer. Don't go in the ocean without me, Diesel. Wait for me. Careful, Diesel.  Diesel, have you ever even seen the ocean before, man? I think this is Diesel's first experience with any ocean. Be very careful where you step here. Very rocky. Look at that. Hurry, Diesel, you wanna go swim in the ocean? Not me.    Look at that, eh? Look at that, what's that, Diesel? Look at that water right there. Go check it out. Be very careful. Don't go too close, buddy. Paranoid parent here. Whoa, that's a big one. That was a big one. Freaks him out. Look at him. Talk to that ocean, man. Look, here comes a big one. Here comes a big one. Oh, he's gonna get wet. He's gonna get wet. Look at a laugh of that. What's going on, man? What is that, man? Here comes a big one. Here comes a big one. Here comes a big one. Here comes another big one. Hehehehe. What is it, man? That's the ocean, Diesel. Look at that. Wow. He loves it. Diesel, don't go too far, man. Come on. Come here, bud. Careful. Look at that big one. Hehehehe. They're getting bigger, I think. What's going on, man? You like it? That's my rock. Get your own rock, man. Smells like seaweed here. I guess we could have gone over there. There's smaller rocks over there. Oh, look at him, look at him. Don't drink that, Diesel. Hehehe, silly boy. You've never seen the ocean. You can't drink the ocean water, man. Hehehehe. Yeah, I figured we'd come show Diesel the ocean once he's never seen it before, so I'll cross that off the bucket list for him. He loves it. He loves the waves, but he's scared of them. It's hilarious. You see him over there? Hehehehe. Oh, Diesel, come here. Don't go so far away, man. Apparently I'm not a parent. How am I supposed to get over there real quick if something goes wrong? Okay, so now, that was a nice little stroll on the beach. We hung out here just for a little bit. We don't have a lot of time. Where'd he go? Oh, he's over there. Diesel, come here. He's coming slowly. So how many of you guys live on the beach like this at the ocean? Diesel, that's not even fair, man. So there's four-wheel drive showing off. Okay, well, me and my two-wheel drive need to get back up this hill. Without embarrassing ourselves.   I'm lost over there. Diesel, come here. Man, I don't know what's over there. Come here. Crazy boy. I just wanna run, man. Look at all the grass. Good boy. Show off. Yeah, that was the ocean, guys. I don't have any more time to show you anything more. Gotta keep going, but. See, atlantic. Oh, he sat up on top with a tunnel there, man. That'd be a good picture. Well, Diesel, we made it. We're here waiting for the ferry. So, once the ferry gets here, it looks like we'll be boarding probably around 9.30, 10 o'clock tonight because the ferry leaves at 11.45. So I'll be on the ocean over tonight again, which means that I can't really vlog on the ship again, which sort of sucks, but I have past videos of the Newfoundland ferry where you can go and see its exact same boat again. And so it's nothing you guys haven't seen already or that I haven't filmed already. But anyways, we're gonna sit back here, relax, we haven't watched our Transformers movie yet, so we're gonna do that. Well, Transformers was amazing. Michael Bay and Steven Spielberg gone out, did themselves again. Amazing movie. A long movie. It's about two and three-quarter hour long, but like every Transformer movie, it was just packed full of awesomeness. Great scene, great work, great music, great actors. All the actors are new in this one. All new actors. And wow, what a plot and a storyline. I think this one was better than the last one. And no offense to the last actors. I like these actors better. It's just my own opinion. Other people might think differently, but these actors, who was it? You got, isn't that Mr. Born Identity guy? Mark Wahlberg, great actor. Any movie he's in is usually a great action movie. And who's the check? Doesn't say on here who the chick is? Oh, come on, you gotta tell me your name, man. Anyways, that's the chick there. It focuses. And then that's her Irish boyfriend, who's also a special driver. I won't spoil it for you. Yeah. Doesn't say her name on here. Dang it. I have to research what her name is. Well, I would definitely recommend that Transformers Age of Extinction and I have the entire set now. Guys, so like usual, my nap turned into more like sleep as long as you can. Kind of nap. That's usually why I don't nap. Because if I nap, I'm just gonna keep sleeping till the next day. But I'm up now. There's some commotion going on around me. People are turning their lights on. There's vehicles moving. Dark outside, so the ferry's here. They just finished unloading everything, or they finished a while ago, unloading everything, probably one hour. And now they've been loading empty semi-trailers in there first, that's what they do. A lot of people from the island here bring their trailers to the dock and just drop it. And then they have shunt trucks that bring those trailers. I don't know if they're empty or not, they could be loaded. They bring those trailers, just the trailer, onto the ship first, right? And then pack them away into the corner because they don't got trucks on them.  And it's coming very close to that time where we're gonna be boarding the ferry.


And I and I'm gonna be honest. I'm happy Why is Chacoby playing Madden right now? Like what is he doing right now? His Seahawks traded every player in their universe He's a gamer and somehow he's playing mutt head-to-head in March on a random Wednesday night I don't you know what I'm saying like through the Seahawks went out bad Chacoby is not lurking me. Chacoby hasn't beat me and I don't think in his whole life I never lost to Chacoby.  He's got to love that situation, right boys. I hope I can sack on my Bobby Wagner That would make my day if somehow Bobby Wagner gets us gets a sack. Oh, he's gonna roll out on me This is where I need Luke Keekley, honestly, honestly, I need the audible down here This is fun boys. I'm just letting just make sure you guys know how much fun I'm having right now It's great throw by Chacoby there. Got Jack young blood in the game Not saying I love that but you know This is what it is. I mean, this is one where it's like I'm gonna even like Spy, you know, but it's not even Russian. I'm like, all he's gonna do is roll out But I don't think he'll ever I don't think he'll ever stand still in the pocket here. Oh What else is new wheel route? I'm honestly gonna run cover for like this and just the contains actually kind of work in 35 wide Because I don't think you can double team them there.  It's fine It's good defense. Of course, he's no huddling Cuz I don't have my my D linemen in the game here. Gotta go to running back here somehow See, I'm not mad at this. I'm not really not mad at this defense the whole game What do you guys think this is what goes to my head when I play like, okay? This is what I'm gonna run. Is anybody like mad at playing defense like I called around defense that wouldn't hurt Man, just gotta be in the right defense, bro. I just didn't call the right I just didn't call it right defense. I didn't call it right defense there. Yeah, I know I'm aware he's running corner routes. I see it.  Nice That's why we got Patterson, right boys He might do the contains on where he gets like the contain blitz the loop. I think he's going to that And I'm just like stuck right now nice Dude the running back just bailed at the last second like he was set to block that and the running back Just like went bit just running back just bailed on me the level of luck on that is just astronomical Of course, I get intentional grounding there, too Gotta love it. You just gotta love it, right boys Just seven people in the flat and we get intentional grounding dude. I'm just I'm having a blast today already.  Let's just like Honestly feel like my chilies look I see Patterson already breaking tackles All right, we got a big drive right here. It's a whole game man. I milked so much. Honestly. He's in good position, but This is how we're gonna live this drive here boys. You guys ready? We will cover the corner out every single play. All right. Are we with it? I don't know how else to cover that I don't think cover four is gonna cover it. Give me some defensive coordinate I'm asking you guys. We're in March. I'm dealing with these snap roll-out guys. I can you can't even come close to containing What are my options here? Let's try cover four first. Let's just try it now I don't think you can blitz a corner. He runs right by him Like he like the corner takes a dumb angle and runs right by him if that makes any sense Like I keep calling the wrong defense. That's one thing.  He had that double wheel route play. I'm gonna hard flat Calvin over there or who's my running my tight end? It's got to be corner out to the left I think I should really use her out here and see which way he goes. Yep.  Oh my goodness, man I think I I think I want to try Zero purples and put them out there. I think I really want to try that like no troll.  I was just I Know it was a corner out. I should have had better. I should have had better user I should have covered the corner out. That was just like I didn't even cover the corner out I feel like in Chicago you run the same No, I covered to is what I tried on that guy last night and honestly it was not good Yeah, I know that was a missile That was not a missile Just run flood bro, just run flood every play dude run flood every play every play is flood against him Every single play nothing else He's in fool, man Like my man's not even try. I don't I don't know what's going on with my contain I really have no idea like I have no idea what's happening to him like he's not even like getting black He's not even he's like going to the egg at spider detack. Oh, did he tackle would have been there? I just can't cover the corner out.  You lost Corner out it's open. I just got to figure out how to how to there's gotta be a way to contain this The worst part is like I can't run dollar. That's what's that because they're running big big I tied I tied like it's worse worse playing about the game It's a little worse thing about the game is in weak box. It is the worst feature about the whole game is weak box, dude The worst feature and I'm nobody telling that people don't talk about weak box enough I mean he has to get my running back here Tackle Patterson is the best. Oh, I can't believe I do that sleep pic though I did it cuz I wasted a time out cuz I wasn't on two clock rough rough rough rough We get a stop though boys. I think I got I think I got a philosophy or an audible down though Oh, I know what we can actually do to run chicopee.  What defense am I in? Why did this happen? I have no idea why that just happened like why did that just happen that I went from He no huddled and I was in a different defense Thank you, bro. You're not good So what happened when you don't try to roll out he stayed in a pocket one time He was back there cuz he tried to like pass you ever see somebody like try to pass and you're like, oh Tell you man, it's just this These under center dudes, bro And I need to get a good defense for the under center guys. There's like some way to really stop it I don't really know it for sure yet boys But just be I just be take your patience with me. All right boys. Just take some patience with it with the kid All right That was just open that was just like come on now that can't happen. They literally can't it just can't happen I think he was on the tight end. I think he was on a tight end. Am I tripping? I swear he was on the tight end. He was not in his own Maybe he was and he was on like a five-yard zone, but I thought he was on a tight end swear to God I did It's like I'm just amazed at like how like oh, how do you not match to that? Am I like it's just really the best play in the game I'm really getting milked right now. Like this is like a noxious dude. They just start chasing them. Oh my god, dude That's zero yard flats right here. Let's see what happens boys I want the flat to just go get him when he rolls out. It's just like those don't matter I mean this guy hasn't scored 20 points on me in his whole life like that like really hasn't It's never scored 20 points on me in his entire life now I just can't stop him and you cannot blitz the corner, dude He runs today. It's the easiest the worst idea in the world It's the first brain that I deal with that people think of blitz the corner It's really the first it's the first brain that thing that they think of and it's not the move Promise you guys with everything in my heart. It's not the move I thought the move really would be play match To match the corner out, but it's just not it's not working I mean, it's only so many times you can try stuff. You just give it up touch. The Tampa 2 is not the move, dude Tampa 2 they can't contain they can't what why would Tampa 2 make that big of a difference, dude I don't want to play man covers. I think it's too hard. It's too hard to play man covers Dude, that's what I tried on the dude that last night. It's just too easy to play man coverage Come on Vic. Like come on Vic make a throw for me one time, man. I really just I really think you cannot contain them It's it's what I mean I don't know if it's wild to say that but I honestly feel like you can't Just got guard deep in the corner Like that's got to be an interception dude like there's no way you like do that pass with like intent. I Don't have a spy which could hurt me and somehow I don't have a man on the running back I have to go out the running back dude. I'm going deep here, dude No way like like oh my god Like he was right there bro. Like he was there. He was there. He was there, dude He just like he was there like I'll tell you man coverage is just not it boys. I'm WI. It's just not it It's just you can't like I like it's just what's crazy about the game is that I don't even want to rush anybody There's no point. I wish like but the game is so broken. You have to write the way He's playing the people rushing the quarterback are honestly a waste of players on my team Because they're so they did just get like stuck in the agap and he's all the way at the sideline Man coverage is just not the move dude. It's just not the move like in a perfect world It would be but it's just just simply not it against this It's just not man is only good with high speed corners. Yeah, you're right I got 95 if I had if I didn't have these 94 speeds out here. I'd have a chance dude facts G It's the 94 speed guys that are holding me back I mean truth be told this game is close cuz I do picks if I didn't throw picks We still win this game with one stop. It just wasn't matching for me. I wish cover six would match on that corner out I just I Really honestly don't know how to stop that corner up We win this month It's crazy cuz it's like, you know, it's nuts about it. It's like really no way to blitz, bro That's what's frustrating about it Now I got a plan I have a plan. There's my plan you guys ready. I'm definitely adjusting right here I don't really do anything like this, but just you can't cover these dudes, bro Where is my purple zone that I put on zero dude?  I really do I don't know like I Don't think there's a way I could stop it. I just I'm just thinking everything I know like he's just too fast on the center under center. He's just like Yeah, escape artist is OP but under center is just like a thousand times faster that makes it.  I like nothing I'm doing is just even coming close. Just don't have a spy. That's like It's like bro, like I just can't like The the zero-yard purple that I'm putting out here is like where is he I just need to put a spy I key I need to put a spy so I just can send that guy and the problem is there's so many people I'm afraid to send if that makes sense like I'm literally afraid to send somebody now I don't want to spy because I need to guard the running bag This is why man coverage is impossible, dude Man coverage is literally impossible to run because you need a spy. You need a deep blue in the middle of the field He just choked nice. This is a tough spot though. That's a tough spot, but I Gotta take my outrout since I gotta get into drill touchdown range. Honestly Four seconds to eight yards ain't really worth it.  He is pooping bricks right now. Be honest. I know this guy. I know she called me He is pooping bricks Honestly want to throw a couple outrouts to the end zone here. It wasn't worth it at the time. The time just wasn't worth it Oh my god being off sides like help like it was just like ah Wasn't worth I should just throw I should just ran with Vic got what I could bro It just really wasn't worth it right there that Switch it up for y'all. This is for people. This is for people. I'm saying some people that realize I'm the greatest ever do this play this game I got bad. God. He put a flat on the left side. Oh Man, I didn't think he'd take that chance. Ah Good call. Oh Man, dude, he's so bad man. I wanted to hit this corner out on the left. Ah Man, I wanted this corner right here probably low key could have hit the running back Probably low key could hit Patterson and I'm situation. I swear. God the running back is like always I really didn't think he'd put a I really didn't think he would put a cloud flat out there and just pray But he did good call if I put him on a post this touchdown, but I put him on I thought he'd I thought he'd go deep blue and like a purple or something like that.  Okay Good segue hum boys What do you mean like put the corner in the content I just feel like he's just too fast or he'll he'll just double team the end let the corner come free and just run around them Knockout is glitchy. This is a this is a game where I wish I could have what you're gonna call it Wish I could have what's that ability route tech? Come on defensive rally. I need you here, buddy. I mean Michael Parsons. Just was the one that routed me right there I'm not even on offense, bro Like I'm not even on are you alright Diego? Come on Simmons.  Mm-hmm. Mm-hmm Because this guy has post up on the center, right? So what we're gonna do is we're gonna drop our detack a lot in covers that way watch was post up blocks right here boys Watch who was posted how was post up blocks right here? This is called Nick. This is called a hurting an ability honestly. Look at that Look at that. I click somebody will get the quarterback, but nobody wants to I'm liking my defense right now boys. I really am what do you guys think? Gotta use your spy though. I really do. I mean one thing I hate about man coverage and zone coverage and dollar I feel like it's just such an easy tell and a lot of times I give kids too much credit that they know the tells like They know when it's manner zone. Oh that dude just fried So let's like this guy's gonna play a lot of man-to-man. So We'll see how it goes Well, he's baseline right now. What's this? Does he got past rush abilities?  That's always good When you get people to contain your past rushers you won already really. I mean that's just a precision pass boys. I Killa that was a whistle. That was just pretty That was pretty that I like I that was a pretty football right there, dude Yep, this is what happens dude is that the purple zone bumps into that guy I don't know why it happens. I Have no idea. I don't know how I can stop that from happening like I like it just it's infuriating It's literally infuriating when that happens This guy thinks he's dick-la-bow with these cover three adjustments out of cover two. He really does do no I'm dirty for overall There's probably a decent bootleg out probably Now this guy has gone to I'm gonna cover the deep middle myself Bro, they should be able to flex NBA games, dude Like when the team sucks like like we should that we should get more flexing in NBA games Like there's no way I'm watching the Lakers every single night, bro It's like it's just not an option for me, dude. That was a terrible pass. God I just I was half half looking at y'all half looking at the field.  Right doesn't he stand there perfectly for this guy?  Thank you Like this dude is just awful on defense bro I'm people say I got the middle to feel myself So you know way that there's no way that happened right there. There's just no way that like I'm getting trolled so crazy dude. I really am. I'm just getting trolled so crazy right now this game Just trolling me right now under pressure Just no way man. We've nobody gets home crawled like there's just no way. Oh my god in heaven, dude Dude, I can't lie. This guy has all day like these three people are getting actually railed right now Put your hands out. Huh? It's like put your hands out right there.  Like what a tackle man. Oh, this is like the most bird defense. I've ever played in my life It's just no way you're play defense like this I got out of balance and we win this game just I just oh My gosh, man. That's like this.  He's just absolutely having a blast. Oh man like We're really getting cooked by mean Joe Green. How did nobody get free there?   Let's go, baby and Aaron Donald scoops it. He's scoops Ken Aaron Donald by hottest. I don't even want to buy hot us. Let's go, man Just keep blitzing stop playing these kids like they're good Keep blitz. Oh my gosh. Just see us a safety.  Really This is low kid combo. Give me a first, please Fourth and inches nice.  I really feel like but I'm I gotta run full back dive against this Look like I have to nice Now we can milk the whole clock though. Let's go I would have ran I would have I would have played that fourth down like it was my life Cuz even if he gives up a touchdown like he has time to go score. I Got a kind of I gotta like low key be careful here because Time is going to like I only got one time out. So I got it. I like this combo right now I'd like this combo with the pulse route. I think the pulse routes won't be a touchdown I actually love this combo. I'm gonna take my time out Get in the end zone. There's no way. Oh My god, Cooper. There's no way. You don't get me. I let it up in everything.  Just like I that was ahead of me a three-wreck.  Like I've just never that was OP I mean boys if he stops like I like that was almost the worst Man, how did he stop my I'm so afraid cuz he stopped my slants so well Denny Bro, didn't he stop my slants so well right there. I'm scared. Hey good blitz.  There's two games. I don't clutch. Oh my god Back to back games. I don't clutch sad tonight. He got a perfect. I Wasn't ready for that play. I really wasn't doing I really wasn't that's my fault, dude I should have just went back to slants. Nobody stops slants. Nobody does Nobody stops slants, but he was stopping it That one play he was Victor do what go where yeah, I just I feel like I had dots I had dots dude. You're right. I wasn't prepared. I honestly I wasn't prepared that last play I wasn't prepared. I don't know what you want me to tell you speaking of prepared speaking of prepared. Hello fresh Check it out boys. That's the deal you get right there. Just cuz you know me Just cuz you guys know me right there Listen, it would cost you 50 bucks it would cost you 50 bucks, but because you guys know me only 24


you know one of the biggest flexes in life is to love yourself the way that you wish they would love you in other words be your own upgrade today don't wait for them you are who you have been waiting for go ahead and love you like you wanted them to love you that's the biggest flex upgrade yourself today


Some of it's going to be really difficult. We are going to have to not do things that we traditionally have done. I am Joanne Manning. I lead the global resources business now in Arab. I've always led businesses that are future-facing and led them in a future-facing way. As an example, when I looked at developing a resource and waste business in Australia, I very much said, well, we will do it only if we put waste as a resource at the centre of what we do, and therefore we refuse to do any new landfill development because that's managing waste as a waste rather than managing it as a resource. Stop thinking about it as waste. It's a resource and therefore it's something to be valued. It's something to be protected. It's something to be cherished. Do we need to transform our economy from being linear from this take, make, use and dispose to being circular? Where we value things, we keep everything in circulation and it's highest value. We actually look to design it out in the first place. We actually say to ourselves, well, can we refuse it? What can we do? Can we just do more with what we have? And then at the same time looking to regenerate our natural systems and increasing our natural capital, which we now recognise is fundamental to achieving sustainable development. A lot of people say, well, our system isn't broken because a linear economy has been really effective and it has delivered economic prosperity and actually human wellbeing like no other century and like no other economy has. But it is broken because that's come at a huge cost to our environment and our planet. So we only have a finite planet. We have ever-increasing demand on this ever-decreasing pool of finite resources that we have. It has to change. Managing waste as a resource is actually a fundamental part of sustainable development. My form of leadership is very much inclusive leadership or even servitude leadership to provide that direction and stewardship that people can get behind and people can understand. To lead in this space and to advocate for it is something I feel very privileged about. It's about being me, about being authentic. I believe that being true to what I believe in, true to my family, true to my communities, true to the people that I work with is fundamental to who I am. My key values for Arab is to have sustainable development at the heart of everything that we do and that's true to me as well and making sure that I walk the talk at all times in terms of how I am behaving and how I conduct myself. I'm a big believer in strong communications and listening holistically to different opinions. I feel stretched and outside my comfort zone at all times. Even most recently I've been appointed to the board, I think being a woman as well, straight away have the imposter syndrome. Why me? Why am I there? But realizing that I do have a really strong voice advocating for those priorities and challenging having that ability to stand up for what I believe in and actually being brave. And some of it's really hard. Some of it's going to be really difficult. We are going to have to not do things that we traditionally have done. Well, my first one was my original leader who I had in Dublin, a woman called Neva Sullivan who was just the most incredible woman. And when I joined Arab and I started working with Neva, she pushed us and she really challenged what we could do but very much gave us that belief. I mean, I've been very fortunate always to work with really, really strong people within Arab. I've also been very fortunate to have great clients that always led to a really great diversity of people to work with. And yeah, that's all shaped who I am. I've worked through the UK, through Ireland and now in Australia. So again, being exposed to lots of different cultures, different types of people in lots of different environments. You have to just strive to anything as possible, be inquisitive, take time to research and learn what it is you're trying to change. Don't just go, oh, I've got a barrier. That's it. I can't go any further. Stop, contemplate. There's always a workaround. Get sponsors, get allies. If you feel you're ever alone, you're not alone and you just need to find your crew and find out who else is battling the same things that you are. Of course, so it's just fantastic. I think the quality of the people that we were exposed to and the content was absolutely fantastic. But I think more than anything else, it gave me confidence. It made me realise that I'm not just a stalwart doing this alone. It's actually all these other people who are already doing it and already have had huge impact and huge influence. There was a lot of opportunity to learn on how to execute, which I thought was a critical part of the course. One of the things I obviously learned actually was really understanding these four key stakeholder groups. The community from academia, from industry and from government and then understanding what are those different perspectives and how does that influence my positioning and my decision making? What the course gave me in many ways was a pathway to achieve my ambition.


This is my mom. What? She made me a sandwich. Do you want one? I want a sandwich, I'm hungry. No, you cannot. Because I already ate it. Send me one via PayPal. No, it does not work like that. Okay, real talk, Brent. When's my pizza shot? What pizza shot? The one that you promised me. When did I promise you? You didn't promise me, but I'm gonna make it happen. Did you have it in writing or in video form? That I promised you otherwise it doesn't happen. You said you'd think about it on the stream. Do you have a clip of that that you can send me right now? No, but I can find it. Because I need it in like a hundred percent either video or written form with no forged signatures. Let me just... And I know I didn't write anything of it, so you might want to, you know, I'm not gonna find that clip because I do know I didn't write anything of that sort. What do you mean? What do you mean? When you want to say pizza shot, but your friend says no, what do you mean? Okay, you know what? I feel attacked, you don't want to shout me any pizzas. No, because I care about your health. I'll shout you a salad. I don't want a salad. From McDonald's. It's the worst kind of salad. I know because you could have got anything else. But no. McDonald's salad. McDonald's salad is the worst thing. You know what else is the worst thing in my life? Subway. Subway is nice, I like Subway.  Can we just talk about Subway for a spurt so you can hear? Subway sponsors us. Subway plus Subway. I love you for a long time. Subway, we will literally shout you out every single time. We do any kind of thing. I just want to like three foot long meatball subs every day. Wow, foot long, jeez. Do you want to get a six inch? No, I take a foot long as well.  You've got to love a foot long in your mouth, you know. Yeah, dude, every day of the week you got to hit this without for long. We're not doing anything, we're not talking about anything sexual here. We just like the box. Those saucy meatball ones. Meatball is honestly my favourite though. Like no joke, the best. Meatball subs are the best. I got it. Alright, let's go. Guard him. Guard him. Your mum, XD. What?  You get a foot long meatball sub. You put some cheese on that meatball sub. Can you think of anything better? Yeah, you put a bit of lettuce as well just to make sure you're healthy. But you always ask for just a tad bit. Just a bit because you don't want to be too healthy. Legitimately what I tell them, I don't want to be like too healthy, so just a bit please.  Putting a little bit of barbecue sauce just to spice it up a little bit. That's always surprises them. Did you see this dude? Look at this dude. Look at this dude. Why did you go first? Because I want to kill him. Yeah, but like I need to blade you and stuff. Oh no, look out, it's the actual emo boy. Oh yeah, look at him go. He is not very spicy at all. Not about that spicy. But he's pretty lit. That is true, he's pretty lit. Spicy wifey. You're my spicy wifey. Do you have a wifey spicy? One spicy meatball please. Do you have a spiky wifey? Spiky wifey? Yeah. I don't understand. That's unfortunate. Explan. That's unlucky, champ. It's really, really unlucky, you know. Please explain. I'm sorry, I cannot. I have an inability to explain. Okay. I'm just going to hit through the shield. Yeah, yeah, boy. Easy clap. Well, I'll put a blade on you just in case you do not kill. Yay.  I will definitely worry about shield, boy. I feel like you're killed by us, don't worry about it. If I could, easy clap. 40% come and clutch. Maybe. Right. Right. You should do right. It deepens. No. No crit. Well, that's an easy kill on the boss. Easy kill on the boss, boy, because he's bad. Yeah, that's what I thought. But this boy, he might take a bit of more encouragement, you see. Yeah. But I feel like I've got him. Oh, no, he doesn't. No, he does. I don't. He does. I don't have him. I don't quite have him. Do you have a leaf stew? I do have a leaf stew. Because I don't care. This is legit. Legitimately, just my farming day. Only 2% of the shield. Oh, he fizzled. No, it's not a shield. He's bad. He's bad. He's bad. What do you want? You want this? Okay, that's cool. I didn't understand what you were asking at the point at the time. So I didn't respond. Yeah, you want that. So, you know, you can have that. I'll give it to you, daddy. You know what I want? I'll give you my blade any day. You know what I want? What? I want you. I know. To love me. I want me too. Okay, humble. Humble bundle. Hashtag humble. Hashtag humble bundle. Hashtag humble brag. Hashtag Brent is good. Hashtag 24 hours stream. Hashtag Brent for Priz, 2020. What are you being the president of? Your mom. I mean, this is just classic comedy at this point. Brent is so funny, guys. Are you jealous? Brent is funny, guys. Are you jealous of me? I don't want to hear that anyone thinks Brent is not funny because he is the funniest man. I'm really unfunny. Anybody who says I'm funny is wrong. I think anyone who says you're funny, wow, now I don't have any hits. You can find it again, don't worry. What do you think happens when you fizzle? I don't know. Magically disappears forever? Yes. Same. Do you like these heels? Am I a pro life wizard?   Yeah, I did my job. I did my job, mommy. Mommy, look at me, mommy. Oh, yeah, mommy. Oh, yeah.  Gigi wins four days. Wow, that was so easy. And guess what? Guess who has a port to live in? Oh, that's right, me.