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Physics - Ultrasound Case Review with Dr. Mahesh (4-28-25)

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0:02

Hello and welcome to Case Crunch, rapid case review

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for the core exam hosted by modality.

0:07

In this rapid fire format,

0:09

faculty will show key images along

0:11

with a multiple choice question,

0:13

and you'll respond with your best answer via

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the live polling feature.

0:16

After a quick answer explanation, it's onto the next case.

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You'll be able to access the recording

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of today's case review

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and previous case reviews

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by creating a free account using the

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link provided in the chat.

0:28

Today we're honored to welcome back Dr.

0:30

Mahesh for a physics board review in ultrasound. Dr.

0:33

Mahesh is a professor of radiology

0:35

and cardiology at Johns Hopkins School

0:37

of Medicine in Baltimore, Maryland.

0:40

Additionally, he is chair

0:41

of the Radiation Control Committee, president

0:43

of A A PM Board, member of a CR subject matter expert

0:47

for N-I-A-E-A and an elected member of NCRP

0:51

and ICRP.

0:53

Questions will be covered at the end if time allows,

0:55

so please remember to use that q

0:57

and a feature to submit your question.

1:00

With that, we're ready to begin today's board review. Dr.

1:02

Mahesh, please take it from here.

1:05

Hi, good evening. Um, I'm happy to talk about the

1:09

physics of AL ultrasound.

1:13

So you wanna set up the first question.

1:18

Wonderful. Um, I know many of you're preparing

1:22

for the board exam

1:24

and this is the right, um, one

1:25

of the topic which we talk heavily.

1:28

So let me go through a couple of some of the basics, uh, um,

1:32

with the question and followed by some of the understanding

1:34

of why that question is done.

1:37

So let me start off with a very fundamental question.

1:41

Question number one, the wavelength

1:43

of three megahertz sound beam is sharpest in

1:48

which tissue

1:55

and the answer is between A and bone.

1:58

We have only few people responded,

2:00

we have 35 people attending.

2:03

And, uh, is there any problem with the response?

2:05

Please let us know. The answer is a,

2:10

because here is a formula, the velocity

2:14

of sound waves is equal to a product of frequency

2:17

and wavelength or wavelength is equal

2:20

to velocity development.

2:22

The frequency. So given here, the megahertz three megahertz

2:26

as a constant frequency, the EF factor is being the same.

2:30

If you look down on this table of velocity

2:32

for different material, the smallest,

2:35

the shortest velocity is in air.

2:38

That's about 330 meters per second.

2:41

Therefore, the vallen is proportional to um, velocity.

2:46

Therefore, the sharpest, the valent

2:48

of three megahertz is sharpest in air

2:51

because that's correspond to the velocity you can see here.

2:55

Um, bone has, uh,

2:56

higher velocity sound wave travels higher in, in bone metal,

3:01

um, is 44,000.

3:03

And in soft tissue,

3:05

the approximate is about 1540 meters per second.

3:08

And here's the following, um, there's also discussion

3:11

that the SAR tissue is 1540 meter per second.

3:14

Um, so in a is 330 meters per second is what you need

3:18

to remember, and that is the answer.

3:20

So now let me go down a little that level.

3:24

Question number two, why is gel applied to skin

3:27

during ultrasound imaging?

3:35

And the answer is to remove air.

3:37

That's correct, because gel is applied to the skin so

3:42

that you don't leave any gap

3:43

between the transducer and the skin.

3:47

That way the sound wave travel faster

3:49

through the soft tissue.

3:51

If there's air, as you saw that the

3:54

velocity is small there in the air,

3:56

therefore that can diminish the transmission

3:59

of the sound wave.

4:00

Therefore, to get clear image, you you prefer

4:04

to put the gel on the skin.

4:07

It fundamentally, the basic principle

4:09

of the pre high principle is, uh, it acts

4:12

as a coupling agent between the surface and the skin surface

4:16

and the transducer eliminating any air pockets, um,

4:20

between the ultrasound probe, I call it a transducer,

4:24

a probe in the skin because

4:26

otherwise that will interfere with the sound wave, create,

4:29

reflection, reflection, all those other things.

4:33

What does the Q factor of an ultrasound transducer describe?

4:44

The answer is, um, is all over the area here.

4:48

The correct answer is frequency response of crystal.

4:53

So what is Q factor?

4:56

Q factor is called, also called a quality factor

4:58

for ultrasound trans user.

5:00

It tells how efficiently it can

5:04

transmit and receive the signal.

5:06

That's, that's important.

5:07

That's a characteristic of a cure

5:09

of an ultrasound transducer probe.

5:12

It also require relates to bandwidth of frequencies.

5:16

So you can see here this is a typical, uh, uh,

5:19

ultrasound transducer.

5:21

You have a pizo electric effect element,

5:23

that's the one which produces, um, uh, sound base

5:27

and return back and connects it.

5:29

There is a caustic absorb that is sound base absorbed.

5:33

And there's also, this is actually a correction, is a

5:36

transmit receiver, um, cable which collects,

5:39

which we transmit the sound base

5:41

and also receive the sound base in a echo forum.

5:44

So here is a different scenario.

5:47

If it is a high queue, means it has longer spatial pulse,

5:52

pulse length as you can see, a longer pulse length.

5:55

Whereas a heavy damping means a very low queue,

5:59

means the sound is very short will,

6:01

and they won't transmit much.

6:03

And this is the broad bandwidth,

6:05

whereas this one is a narrow bandwidth so that it'll,

6:09

it'll penetrate through the material much more

6:11

longer 'cause of the iq.

6:13

So that's why the frequency response of a crystal is

6:18

what Q factor tells us.

6:23

Question number four, what is the attenuation?

6:26

If an ultrasound beam is attenuated by 99%,

6:36

the answer again is variable.

6:38

The correct answer is minus 20. So how, what is tonation?

6:44

Tonation means it's stopping of anything

6:47

in x-ray, we saw x-ray.

6:48

Tonation is the stopping power of a material

6:51

to block x-ray here, tonation is the stopping power

6:55

of the material to block us on wave.

6:57

So if an tonation ultrasound is alternated

7:01

by 99% means only 1% has passed through the material.

7:06

So we call it, we have a formula call

7:09

relative sound intensity.

7:11

This is expressed in desi bells.

7:13

That's the unit of relative sound intensity.

7:15

That's what we are, we are all these, uh, headphones are,

7:19

uh, when they see the power of the headphone,

7:21

the loud noise they express in decimal.

7:24

And that is also called

7:25

as like the decibel level reaches

7:27

more than a hundred decibel.

7:29

It is kind of like harmful the year and all those things.

7:32

Anyway. So here's the formula.

7:34

10 times 10 times longer than longer than week of base 10

7:39

to the ratio of these two i is the word a measured intensity

7:44

and inot is the internet original intensity.

7:47

So I means it ated by 99% means that trans

7:52

measured intensity is one,

7:53

whereas the version intensity is a hundred.

7:56

So if you put this into formula log

7:59

of 0.01 is minus two, minus two times 10 is minus 20.

8:04

Therefore, if a particular tissue has a negative decimal

8:08

value, it means it is attenuating the sound

8:11

waste very fast one.

8:13

If it is a positive decibel means it amplifies the sound.

8:17

For example, in a metal, if you click on one end,

8:21

the sound transmit and enhances that has a positive decibel.

8:25

Whereas in a soft tissue, another thing it get absorbed.

8:29

So if you have this ratio

8:32

of 0.1%

8:34

or 1% transmission, that's equal to a decimal of minus 20.

8:39

And if least 10% is minus 10 and 50 is minus three.

8:42

Again, it goes back to this, this formula

8:45

of log themic scale to 10 is in a calculated I by inot,

8:51

which of the following has the highest acoustic impedance?

9:01

Okay, the current answer is bone.

9:04

As you can see, caustic impedance means the, the stopping

9:08

or the resistance offered

9:10

by a particular tissue for the sound waste.

9:13

And you see that bone has one of the highest

9:16

caustic impedance, 7.8 kilogram per meter

9:19

square, uh, per second.

9:21

And you can see here air has the least

9:24

acoustic impotence and you can hear that.

9:27

And then the fatty tissue

9:29

and other tissues that the following, um, metal has the, one

9:33

of the even higher one, it's about 30.

9:35

So among the choices we are asked at the bone,

9:37

and that's the correct answer, which

9:42

of the two images was acquired with a sound

9:46

at shortest wavelength?

9:50

So image A is obtained at six megahertz,

9:53

image B is obtained at three megahertz.

10:02

The answer is, uh, a image and, and the, and the image a

10:07

and that is correct.

10:09

Why? Because you have the formula velocity called

10:12

to frequency time ent.

10:14

Therefore, if this is sick bag heart, uh,

10:18

and uh, with the shortest valent means

10:21

this should be the shortest

10:23

because the velocity of velocity of the subway tra

10:27

transport traveling through these two tissues the same.

10:30

So therefore the six megahertz will have the shortest well

10:34

compared to three megahertz will have a longer variant.

10:36

That's the, and that that comes out from this formulation

10:39

of weak equal frequency time lambda.

10:42

The wave length,

10:47

which of the following will

10:49

directly affect the frame rate in ultrasound?

10:53

Is it line density frequency selection, speckle reduction,

10:57

or harmonic imaging?

11:05

The answer is between these two

11:07

and the right answer is line density.

11:10

Sorry, because line density means it's the number

11:14

of scanned lines

11:15

or beams, which is used to create an image

11:18

within an angular width.

11:20

How many ways it to send and create pattern?

11:22

So higher provide better image resolution,

11:26

but will reduce frame rate because you, so

11:29

therefore the line density, um, will directly affect, uh,

11:33

which of the following will directly affect the frame

11:35

density is the line there.

11:36

Frame rate is the line density.

11:38

So if the higher level provides better image resolution,

11:42

but if, sorry, uh, lemme see.

11:46

But this will reduce the frame rate.

11:48

So the line density is inverse, is mostly affects the,

11:52

um, the frame rate.

11:57

Which of the following, um, transmit

12:02

setting will result in the best axial resolution?

12:12

So now here is again as a variable answer here,

12:16

the correct answer is four

12:19

transmit cycles at eight megahertz.

12:22

Why? Because for a, for a given transmit frequency,

12:27

XI resolution, um,

12:29

really degrade if there are greater number

12:32

of transit cycles are used.

12:34

Therefore, in order to have the best XI resolution, you want

12:38

to have a minimum number of transit cycle.

12:40

But for a given number of transit cycle,

12:44

axi resolution will improve if the transit

12:46

frequency is increased.

12:48

Therefore, between these two choices, the four,

12:51

the lower the transmit cycle is better

12:53

and higher, the frequency is better

12:56

to get the axi resolution.

12:58

Therefore, the choice was, uh,

13:00

four cycles at eight hertz is the right answer.

13:05

I think this is a, it's an error.

13:07

It should be C and uh, that's a type of error.

13:11

What is the axial resolution of an ultrasound beam

13:16

transmitting four cycles at one megahertz in soft tissue.

13:26

Again, this is a bit of a calculation.

13:29

I am hoping these type of

13:31

detailed calculations are not given,

13:32

but this is a little bit more complicated than the other

13:35

calculation, but other calculations you need to know.

13:38

But what is the right answer?

13:39

The right answer is three millimeter.

13:42

So what is, what is axial resolution?

13:45

Axial resolution is the ability of the, of the,

13:49

of the system to resolve object in the line of the beam.

13:54

This is the line of the beam.

13:56

So ability to down along the axis of the beam propagation,

14:01

also known as the depth is, uh, is one,

14:04

this is axi resolution is independent of the depth,

14:07

how depth, how many, it doesn't matter how deep they are,

14:10

it can resolve here.

14:11

So here for example, there is a, there is a, there is a,

14:15

there is a tradeoff.

14:16

Increasing transmit frequency will improve axial resolution,

14:20

but ation increases and so forth.

14:22

So let me show you the calculation.

14:24

This is a little bit more calculation.

14:25

I wanna go step by step.

14:27

So the axi resolution is calculated as form.

14:32

Axial resolution is one half of the spatial pulse length

14:36

because you are, you are in ultrasound,

14:39

we tra we transmit the sound wave

14:42

and wait for it to come back.

14:44

You collect the echo, that's the receiver.

14:46

So the total time of the travel,

14:48

you have to account both of them.

14:50

Therefore, axi resolution is half

14:53

of the spatial pulse length.

14:55

So at one megahertz of ultrasound, the len,

14:59

the wavelength is 1540, sorry 50, uh, I'm sorry,

15:05

1540 P millisecond one by one hertz

15:07

because we are using soft tissue, speed of length, speed

15:11

of velocity of sound in soft tissue is about

15:14

1540 meters per second.

15:16

And you divide that by the frequency one megahertz.

15:19

So you get at one megahertz, the wavelength is 1.54 you

15:25

now, now the spatial pulse length is what the, is the number

15:29

of cycles, times the wave length, that's about 6.16

15:34

and the axi resolution is one half of that.

15:37

That's why it's approximately three millimeter.

15:40

Now the science behind it is important

15:42

for a given frequency.

15:45

Um, you want to see axi resolution will degrade

15:49

if we have more transit cycles are used

15:52

because more transit cycle you incur use it,

15:56

that will increase the spatial pulse

15:58

length longer and longer.

15:59

Therefore the XI resolution will go down for a given number

16:03

of transit cycle.

16:04

If there are four transit cycle

16:06

or two transit cycle, the XI resolution will improve.

16:10

If the frequency is increased, like as you can see,

16:13

the frequencies increased, the variant will decrease

16:16

and that therefore the spa pulse plan is also decreases and

16:20

therefore there is a trade off

16:22

of increasing the transmit frequency.

16:25

Um, is increased ation, the ultrasound beam

16:28

and uh, generally this is not, it's independent of the depth

16:33

or depending no matter how deep the objects are,

16:36

that is doesn't matter for the actual resolution.

16:39

For axial resolution, it is important on the

16:41

transmit frequency and also the um, the spatial pulse length

16:46

of the beam and the,

16:48

and the frequency of the transducer

16:52

in real time be mode ultrasound,

16:56

the lateral resolution is improved with increased What

17:06

the answer is scan line line density.

17:10

So in a real mode,

17:12

real time V mode ultrasound higher line density

17:17

generates better lateral spatial resolution.

17:20

On the other hand, if you have more line lines are used,

17:24

the frame rate must be it is

17:25

because it needs some time to correct the it,

17:27

that's why the lateral resolution is increased

17:30

by increased scan length line density.

17:35

Question number 11, which performance parameters related

17:39

to ultrasound equipment's ability to resolve

17:42

in plain objects along the propagation axis

17:46

of an ultrasound B?

17:54

That's correct because we are talking about resolve in plain

17:59

object along the propagation axis of ultrasound beam

18:02

and that's, uh, that's, uh, axi resolution.

18:06

Next question, question number 12.

18:09

Lateral resolution in ultrasound is best achieved when the

18:13

objects are at above focus zone at focus zone

18:19

or below focus zone

18:27

at focus zone is correct.

18:29

And here's the thing, when you say lateral resolution,

18:33

you're talking about in this direction perpendicular to the,

18:36

uh, propagation.

18:38

So in the longitudal, uh,

18:39

axial resolution you're talking about object in this line.

18:42

Now the lateral resolution is object line across the beam.

18:46

So the lateral resolution is defined as the ability

18:50

of the ultrasound beam to resolve object on,

18:54

on particular direction to the people.

18:56

And this is depend on the width of the focal zone

18:59

and on the depth focal zone is if you, this is a

19:03

curve curl curve transducer

19:06

because it is a curve, curve career curve object.

19:09

You see the, say the beam focuses at this

19:12

is called the focal zone.

19:14

And the focal zone, it has the best resolution.

19:17

If the object were away from the focal zone,

19:20

you can see here it is almost joining together.

19:23

And if it is away from the focal zone,

19:25

again the resolution is very poor.

19:27

That's why it is it.

19:29

But another thing is this is depends on the width

19:32

of the focal zone and on the depth also.

19:36

So here the depth is much longer, whereas inal resolution,

19:40

it is independent of the depth in the,

19:43

in the depth beam direction, whereas lateral resolution, um,

19:47

it is dependent on the width and on on the depth.

19:53

So which of the following control provides greater depth

19:56

of visualization?

19:58

On the top image on the, on the depth

20:01

of top image is 124.7 millimeter.

20:05

And the bottom one is a hundred point 101 millimeter.

20:09

So the one is this is this is the, uh,

20:12

the phantom which we use as a medical physicist

20:15

to do the quality control.

20:17

And you can see here on the we, we can,

20:20

we can see different period point, sorry,

20:23

the correct answer is, uh, greater transmit power.

20:27

And I'm sorry, with the mouse modeling this a something

20:30

which I'm messing up with the, going back on the slide,

20:33

I apologize, but here the right answer is transmit power

20:36

created transmit power.

20:38

What I wanna show you in this particular phantom is

20:41

these phantom is commonly we use it here.

20:44

For example, if we see a line in this direction,

20:48

we can see the capacity of the axial resolution

20:51

and how far the deep it can go.

20:54

As you can see here, the resol axial resolution is same no

20:58

matter how deep the objects are here.

21:00

This one will measure the lateral resolution, how

21:04

how good the object,

21:05

the transducer can resolve object in the lateral plane.

21:09

And we count this and we can measure.

21:11

Then there are other things which we measure is like, um,

21:14

low, uh, high echoic point and low e echoic point

21:17

and also the uh, the distance measurement and so forth.

21:21

So there are a number of uc tests which we do on,

21:24

on a phantom, which is embedded by all sort

21:27

of these object inside it.

21:31

Which performance parameter related

21:34

to ultrasound equipment's ability

21:37

to resolve in plain objects perpendicular to access

21:41

of ultrasound being

21:49

I think this was an easy one.

21:50

It's a lateral resolution because we have seen that.

21:54

But in the,

21:55

in the PM direction is axial resolution perpendicular

21:58

to the axis of the resolution is a lateral resolution.

22:02

Again, the same figure I wanna show you,

22:04

the best resolution is obtained

22:06

and the focus zone of the particular transducer, um,

22:10

and away from it is more away from it has

22:13

all this other situation.

22:16

How long is the echo written time

22:19

for an interface at one centimeter depth

22:28

as I, as I mentioned, oh, this is six,

22:30

six microsecond and so forth.

22:33

The answer is 13 microsecond. Why? Here's the formula.

22:38

It is based on the range equation we have the time,

22:42

the echo time equal to two times the depth divided by the c,

22:47

c is the velocity we are assuming it's in soft tissue.

22:50

So it's therefore it's 1,540 meters per second

22:55

or 1.54 meter per microsecond.

22:59

The distance is calculated as C times G divided by two.

23:04

This is the depth at which the echo signal is formed.

23:07

That's the depth. So depth is calculated by the velocity

23:11

of the sound in a particular tissue

23:13

or in a multiplied by the time delay,

23:17

which include both the time for the fault to travel

23:20

and also refer back.

23:21

So time and divided by the two

23:23

because we, we always count time as the amount,

23:26

the time it took to transmit to particular region

23:29

and the reflection is held back, the echo is hard back.

23:32

So using this formula D equal CT by two, we are trying

23:36

to calculate what T is.

23:38

So if we interpose all these things, you get 2D divided

23:41

by C, therefore this comes out to 13th microsecond.

23:45

So this is another one of those things.

23:47

You just need to remember if the depth is equal

23:50

to the velocity times the time delay divided by two

23:55

because the time delays always takes into account twice the,

23:58

it is already taken into twice the time to go

24:01

and come back to, to transmit and HiTA interface

24:05

and reflect back, which is scattered by the transmitter.

24:08

And that's how it's calculating

24:14

which interaction of ultrasound wave

24:17

can result in artifacts marked by lateral displacement

24:22

of object in an ultrasound image relative

24:26

to their original locations.

24:34

Correct? It's a refraction

24:36

because as you can see here, um, this basically,

24:41

um, the way, um, um, it, the beam seemed

24:45

to be not reflected but out.

24:49

And this is typical artifact

24:51

because the structure appears

24:53

to be not in the current location

24:55

and it appears in the wrong location due to the bending.

24:59

And this is a classic example of this like Phil drop coin,

25:02

the coin appears almost lightly out.

25:05

Actually that can cause that is

25:06

because of the lateral displacement due to fraction

25:10

reflection is basically, um,

25:12

is the sound way getting reflected in a

25:14

particular, uh, interface.

25:16

And that is what we do in the um, uh, ultrasound.

25:20

We collect the reflection and create the object wa

25:22

and the in interface surface transmission is passing through

25:28

refraction is the one which causes the object to be appeared

25:31

as if it is displayed from a particular location.

25:34

And this is the classically we've seen in the ultrasound.

25:39

So now what is the maximum pulse reputation

25:43

frequency to penetrate 20 centimeter

25:48

of tissue using a three megahertz trans transducer?

25:58

And the answer is, um, let me show you the answer

26:04

and the answer is four megahertz.

26:06

Now we need to know what is pulse reputation, frequency,

26:10

pulse reputation, frequency is given for the transducer.

26:13

How much of this, um, wave cells sent per unit time?

26:18

And that is divided by that, that is, uh, given

26:21

by the formula C times 2D as you can see again

26:26

twice the distance PRF is the frequency.

26:29

Again, you can call it frequency equal

26:32

to velocity divided by the vallen.

26:34

Vallen here is color two times the depth, that's

26:37

what this 20 centimeter, 20 centimeter is 200 millimeter

26:41

and the C is gives as us 1 54,

26:44

that is assuming it's a soft tissue 1, 5, 4 0 meter per

26:48

second or 1.54 meter per microsecond.

26:52

So if we put this into this formula here, again,

26:55

that comes up to 3.85 kilohertz at approximately,

27:00

um, approximately four hertz is, so

27:05

if we, if we divide this by microsecond

27:08

or op can number to four hertz.

27:13

So again, these formula seems daunting

27:16

but simply the same formula C equals len, the frequency,

27:20

once you remember that it can change these things around.

27:26

Now what is an M mode display present?

27:35

That's correct, that's moving anatomy, um,

27:39

as a function of time.

27:41

And here MM mode stand for motion, um,

27:45

where B mode is like a more static one.

27:47

So in MO what happens is

27:49

echo signal amplitudes are modulated to brightness level.

27:53

So the echo signal coming out is, it varies depending on,

27:57

depending on the amplitude is coming.

27:59

Each of these are given a different brightness signal.

28:03

Therefore, um, the, the flow is actually showing the,

28:07

like a color how it's in the color in the docker are

28:11

or in more display.

28:13

So here's what happens is like ultrasound beam is not swept

28:17

across the plane of interest.

28:18

Instead the beam is fixed

28:20

because you're only targeting anatomy or,

28:23

or an object which is flowing through the beam area.

28:26

So as it moves through the area,

28:29

you're collecting the reflection

28:30

and the reflection,

28:32

the amplitude goes into different direction.

28:34

So the beam is fixed in one position,

28:37

but observer observe over scanning time

28:40

to graph a motion of moving structure.

28:43

So you're basically keeping there,

28:45

the beam is position at the same level like a carotid artery

28:48

or any of these blood vessels you want to image kept there

28:52

and you hold it in the same position where

28:54

and correct the echo signals

28:56

and the echo signal collecting it.

28:58

The amplitude depends on the, uh, the flow direction

29:02

and also the uh, going in

29:04

or out, it is mapped into a color scale

29:07

and that's what you get this, all these colors.

29:10

So let me see here. Next question.

29:16

Which information does the color doppler provides?

29:25

It's a mean flow velocity, that's correct. Um, let me see.

29:32

It's, and probably you heard right now in a doppler effect,

29:36

uh, from my, my, from my sound system

29:39

because there's an ambulance to call from hospital

29:43

as it moved away you could hear the

29:45

waning sound of the scene.

29:46

That's, that's the phenomena of the do sound effect

29:50

and that's mapped into a color phenomena.

29:52

We call it color doppler and that's it

29:54

because the sound wave where is hearing?

29:56

So this is information which in the color,

30:00

color doppler is we want to call

30:02

for the mean flow velocity is what is uh, recorded.

30:08

Which type of artifact does the arrow in the image

30:11

of a kidney cyst indicate?

30:20

The answer is ation.

30:22

You are correct because if we look in here closely, sorry,

30:26

if you looking closely here, this is the cyst means it is,

30:30

it is a air pocket, so it is dark,

30:32

there's all the soft tissue in the kidney area.

30:35

Um, probably this is reflecting from the, uh, darker, um,

30:39

bone or some other, other, other tissue.

30:41

But here, if you look here, this is,

30:44

you can see here almost like a line artifacts

30:47

and a bunch of parallel lines here.

30:49

And that is like hitting back and,

30:52

and we call this like a, it's called ation artifact

30:56

because it has equally spaced echoes

30:59

with decreasing brightness and length.

31:02

It's very classically nice one.

31:04

So the bar, the first one is larger, it's also brighter,

31:08

but if you go down the list, it's almost equally spaced,

31:11

but you have different, um, um, brightness

31:13

and also decreasing length.

31:15

And there these are called river reservation artifact.

31:22

And, and you were as per us FDA, what is the upper limit

31:26

for mechanical index for general ultrasound scanning?

31:37

The answer is, um, the answer is 1.9

31:42

and this is a mechanical index.

31:45

A MI is a value of a negative pressure divided

31:49

by the squire root at the center frequency.

31:51

It is also used in terms of like some type

31:53

of a harm in the ultrasound safety aspect,

31:56

also the mechanical index

31:58

and that's allocated here, pressure divided

32:01

by the squire root of the center frequency.

32:03

Um, there is a question in the,

32:06

the take on question number 17.

32:08

I had that at 3.8 kilohertz.

32:11

Um, but how come my answer was four?

32:13

Actually I think it's a typo,

32:15

which I have done in the question.

32:16

It should be four kilohertz

32:18

because I run it off to, um, it should be in hertz, not, uh,

32:22

it should be in kilohertz, not just hertz.

32:25

Um, um, so higher frequency resulted better

32:29

and worse axle resolution.

32:30

We can come back to you, I'll come back later to show back,

32:34

go back to the axle resolution

32:35

and you can discuss this frequency component of it.

32:40

Next question. The following information can be obtained

32:43

from the spectral Doppler evaluation except the following

32:54

that correct because you can actually, um,

32:57

by the doppler we can actually get the, sorry.

33:04

So you can see the main idea

33:06

of the D evaluation is to see the direction.

33:08

You can get the direction of the flow.

33:09

That depends on the color, what you see on the,

33:12

on the arteries or veins, the blood flow in

33:15

or out of the, uh, trans area.

33:18

You can, you can also get the spectrum

33:19

of flow velocity mapped on

33:21

and you can also see what type of flow,

33:23

but we cannot see the depth of the vessel.

33:25

That's correct. Which type

33:29

of artifact does the arrow in the image

33:31

of a kidney cy indicate?

33:40

The current answer is, um, a um, is a twinkle

33:45

creating a twinkle twinkle artifact.

33:48

This is because it's, it's characterized

33:51

by a mixture of colors.

33:53

And as you can see here, this is the probe going around the,

33:58

to the doppler doppler imaging.

34:01

You can see the scales here.

34:03

The, the red means it is indicating in your 15.4 centimeter

34:08

per second in one direction, minus 54 is a flow, uh,

34:12

in the opposite direction.

34:14

So that's how you can differentiate

34:16

the direction of the flow.

34:17

And uh, and here the artifact is actually caused, uh, sorry,

34:23

and this is because it is happened may probably,

34:26

there may be an object which reflect a very highly

34:29

reflective object and that signal gets signaled

34:32

and in this case, twinkle artifact is caused

34:34

by the kidney stone around it.

34:36

That's why we see the very brightness here.

34:38

That's the kidney stone is equal to calcium phosphate,

34:41

calcium equal like a bone.

34:43

So similar to bone, that's where they, it's the,

34:46

it's a loud signal you can,

34:47

because it is a maximum automation.

34:50

And when you have that reflection base mixed together,

34:53

you can have these type of, a combination of a mixture

34:57

of color and it's designed, it's called as, um, a twinkle,

35:01

uh, artifact based on the surface

35:06

reflection in the image.

35:08

Which two tissues have greatest impedance differences?

35:18

That's correct. The answer is, um, muscle, sorry,

35:22

muscle and bone.

35:24

And what, why this is here is what's shown

35:27

as the different tissues and this is the impedance

35:31

and the unit of influence is called als.

35:34

Time number six.

35:35

You can see here, lemme

35:37

see, you can see here.

35:43

Um, the bone has the highest impedance and muscle is less.

35:47

Therefore you can see, um,

35:50

the surface reflection in the image is so high

35:53

between the muscle

35:54

and the on the bone, which is the femur here in this case

35:59

compared to fluid and muscle.

36:03

Another question, the fetus of two image.

36:06

These are the images of fetus images, you can see the fetus,

36:10

um, forming here.

36:12

And you can see the idea here.

36:14

Caution is the fetus in these two images were exposed

36:18

to electromagnetic radiation, mechanical vibration,

36:22

ionizing radiation, uh, impedance oscillation.

36:31

The current answer is mechanical vibration.

36:34

And that's one of the reason why we, the,

36:38

we always warn about all these

36:41

boutique ultrasound centers trying to provide nice, uh, uh,

36:46

baby picture for the pregnant women.

36:48

Uh, especially in the malls.

36:50

You can, you might have seen this facility which advertise,

36:53

they can give you all these 3D images,

36:55

but every time you are doing it you can gonna create

36:58

mechanical vibrations that can harm the fetus of the baby.

37:03

And that's why we always caution as one of the, uh,

37:07

cautionary, uh, aspect we want, uh, not to lower

37:12

use ultrasound, pregnancy, use it only when essential not

37:16

for, uh, boutique factor.

37:19

The other one is like if there are any air cavity in the,

37:23

in the fetus area that can create what is called a say, uh,

37:26

like a temperature can increase in that area

37:29

because the reflection

37:30

that can also cause a little bit more harmful to the,

37:33

to the, to the fetus.

37:34

So all these things are part

37:36

of the ultrasound safety aspect.

37:40

So I have these, uh, these, I had these questions.

37:44

Let me see these,

37:45

the questions coming out on the under on the board.

37:48

So the second one I said, uh, I think it should be four, uh,

37:52

four kilowatts not, um, for hertz.

37:55

So that's fine. What is the image finding that shows

37:58

that there's more reflection between bone

38:00

and muscle on the period?

38:01

What is the imaging finding that part?

38:04

I don't know the answer. What is the, uh, finding,

38:08

I think you guys need to know.

38:09

I'm not a ultrasound radiologist.

38:11

So what is the, this is, I'm just talking about the, um,

38:15

reflection, but I don't wanna,

38:17

I don't know the answer to that one.

38:19

So the other question you had was

38:24

higher frequency results in better

38:27

or worse action resolution.

38:28

Let's go back to the, uh, axial resolution question.

38:37

So let me stop, let me, let me, let me here, come back here.

38:40

Let me go back to the axial part resolution.

38:43

So this is what we are talking about.

38:45

Um, let me see, where is there acceleration?

38:49

Uh, we can go back here to the next one.

38:53

Let me see.

38:59

So as we can see here, the

39:05

transmit the frequency will improve a acceleration

39:07

however tion increases

39:09

and also ability

39:10

to resolve on the axis along the depth

39:13

is independent of the depth.

39:14

Let me see what, what else?

39:15

Like, you know, you're talking about the frequency.

39:17

Um, let's say how do we calculate the frequency?

39:21

We are calculating the frequency, um, with it.

39:25

So this is the XI resolution was calculated as follows.

39:29

Let's say here, if we use this, this formulation

39:34

resolution is 3.02.

39:35

That is three millimeter XI resolution.

39:38

If you increase the frequency here,

39:41

the variant becomes smaller,

39:43

therefore the spatial LE length becomes smaller,

39:46

therefore the resolution can also become smaller.

39:50

So therefore increasing the frequency will actually improve

39:54

the spatial XI resolution.

39:56

A better when it transmit frequency

40:01

al re degrade or the more tracking is used.

40:04

But on the other end, if the a trade off is increasing,

40:07

is increasing imagination, but if the, um,

40:14

because of the spatial

40:15

and going smaller, the AL resolution is increased.

40:18

So I would say the XI resolution will improve

40:22

with the higher frequency of this one transfusion.

40:25

Let me see other questions you

40:27

have for the lab.

40:31

Is thematic radiation wrong?

40:32

Yes, because ultrasound is not part

40:35

of the electromatic spectrum.

40:36

Ultrasound is a differently

40:39

because thematic spectrum works under the principle

40:41

of e equals mc square, all of the spectrum

40:45

present in the electromatic.

40:47

Radiation is part of this, uh, travel with speed

40:51

of light C equals the three point,

40:53

three point 10 point of eight meters per second.

40:55

Whereas ultrasound is the sound where

40:57

therefore it's not electromatic radiation.

41:00

What is the relationship between pulse reputation,

41:03

frequency and frequency?

41:04

They're pretty much the, they're they're the same.

41:07

Um, can you review your variation versus the ring

41:10

down artifact please?

41:12

Uh, the ring down artifact, again, that depends on the,

41:17

uh, um, I'm not very familiar with one.

41:21

I, the answer I can convey is like revelation is like there

41:24

is a reflective, uh, surface

41:26

and that's causing this, uh, reservation

41:29

and that creating a artifact whereas a ring down artifact is

41:32

like, like the, the, the whole um,

41:38

I don't want to guess this

41:39

because I had

41:40

to think about ring down artifact I'm not very familiar with

41:44

because I've not heard so much about the ring artifact.

41:47

Um, uh, so you need to check on that in the,

41:49

in the textbook, uh, for the check it out on this one.

41:52

So I'm, I'm sorry about that.

41:53

I want to give wrong information.

41:56

Whereas ation artifact, as you can see here,

41:59

uh, we saw that one.

42:01

What's the reason is like, uh, let see,

42:08

see this is the equally spaced decreasing brightness

42:11

that is sent from the surface, but this is

42:13

because of the interface.

42:14

There is a very high reflection point causes this one

42:18

and that is causing this all this uh, uh, uh,

42:24

so I think we answered the question.

42:28

Any other question? So I got this one done

42:34

answer, so thank you very much

42:37

and I think two weeks from now I wanna talk about the final

42:40

set of these questions.

42:41

That, and that's on radiation protection,

42:43

which is again a major portion of the, um,

42:47

board exam will be taking a lot of questions about

42:49

radiation protection and limitations and so forth.

42:53

So I look forward to sharing that information.

42:56

Uh, two weeks from now is that May 12th, uh, Ashley May

42:59

12th. Yes,

43:00

May 12th. And they're

43:01

gonna announce it and we're gonna have it so on.

43:05

Yes. Thank you so much Dr.

43:07

Mahesh for this case review. Appreciate it. Sure,

43:09

Appreciate, thank you very much for joining.

43:12

Yes, thank you for everyone for participating.

43:14

You can access the replay of previous reviews

43:17

by creating a free account.

43:18

Be sure to join us next Monday, May 5th

43:20

with Dr. Francis Dang who will lead us in a rapid review

43:23

of neuro brain imaging board review cases.

43:26

And then May 12th is our final case crunch

43:29

for the year with Dr.

43:30

Mahesh on risk. You can register

43:32

for those at the link provided in the chat.

43:34

Follow us on social media for updates on future meetings.

43:37

Thanks again for learning with us and we'll see you soon.

Report

Faculty

Mahadevappa Mahesh, PhD, FACR, MS, FAAPM, FACMP, FSCCT, FIOMP

Professor of Radiology and Cardiology

Johns Hopkins University School of Medicine

Tags

Vascular Imaging

Pediatrics

Nuclear Medicine

Neuroradiology

Musculoskeletal (MSK)

Interventional

Head and Neck

Genitourinary (GU)

Gastrointestinal (GI)

Chest

Cardiac

Breast

Body