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#1 Re: Help Me ! » Geometry; similar shapes » Yesterday 06:49:45

Cheers, Bob.

I've now looked at the answer and Maths Genie agrees smile

#2 Re: Help Me ! » Geometry; similar shapes » 2025-07-16 04:51:47

Thanks, Bob.

“But that assumes that CD is parallel to BE.  It looks right but the question doesn't specifically say so.”
I’ve had another look; it doesn’t actually look parallel.

“A is obviously common but maybe angle ACD = AEB which still leads to similar triangles but with the second answer.”
So E would be the top of the triangle?
Do we rotate the small triangle anti-clockwise until its base is BA?

“My notation for this case is
ACD
AEB”

That makes me think we don’t rotate the small triangle anti-clockwise until its base is BA.
Maybe we flip AEB on its head, as it were, to put E at the top, with A still at the bottom left?
“Now I can pick out the alternative ratios
AC/ AE = AD/AB
and form a second equation for x.”

To find Scale Factor (SF):

(8+x)/(12) = (15)/(8) ?
8x=12
x=12/8
x=3/2
SF=3/2

**

15(3/2)=22.5
22.5-8=14.5
x=14.5 ?

#3 Re: Help Me ! » Geometry; similar shapes » 2025-07-15 05:50:45

Thank, Bob.

What's the difference between ADC and ACD?

I'm wondering why they aren't two ways of labelling the same thing, like we could call/label a square ABCD, going from, say, top left, clockwise through B,C and D. Or we could call/label the same square DCBA, going from bottom left, anti-clockwise through C,B and A. Is that correct?

What am I missing regards ADC v ACD

They look to me like the same shape, the same triangle, the former being labelled anti-clockwise, the latter clock-wise. But obviously I'm missing something smile

Or maybe I'm just confused about the very basics of this kind of thing?

#4 Help Me ! » Geometry; similar shapes » 2025-07-14 04:50:18

paulb203
Replies: 6

9cEzamw.png

Why are there two possible values of x?

Here's what I've done so far.

AE(SF)=AD
12(SF)=15
SF=15/12
=5/4

AB(SF)=AC
8(5/4)=AC
AC=10

AC-AB=x
x=10-8
x=2

A hint please, as to my next step

#5 Re: Science HQ » Physics; conservation of energy » 2025-07-11 11:17:48

Thanks, Bob.

I’m struggling a bit with the concept of kinetic energy.
Having always thought of energy as THE CAPACITY TO DO WORK (or cause change) to discover that kinetic energy is the energy an object has BY VIRTUE OF ITS MOTION puzzles me.
If I’m sitting at home, with potential chemical energy from the food I had earlier, I have the capacity to do work, e.g., go for a walk.
When I go for the walk I think of it in terms of spending that potential energy, by doing some work.
But I’m now told that energy can’t be destroyed, that it has to go somewhere, in this case, converted into kinetic energy. It seems more intuitive to me to think of it being converted into work. I had energy, and I spent it doing some work. And the more work I do, the less energy I have.

I’m not questioning it, as such, just trying to get my head around it.

#6 Science HQ » Physics; conservation of energy » 2025-07-10 22:47:39

paulb203
Replies: 3

I’m working my way through Khan Academy’s High School Physics and I want to check that I’m getting the concept of conservation of energy. Is the following at least roughly correct?

When a ball is rolled down a U-shaped ramp from the top of one side it will, ignoring friction, travel to the bottom of the ramp, up the other side to the top, back down , and up the first side to where it began, etc, etc, ad infinitum.

The U is converted to K as the ball descends, and the K is converted to U as it ascends.

At the respective tops the U ‘tank’ is full. At the bottom it is empty.

At the tops the K ‘tank’ is empty. At the bottom it is full.

Halfway down, or up, both tanks are half full.

**
When rolling it down, and taking friction into account, it won’t get quite to the top of the other side as some of K will be converted to thermal energy and sound energy. It will get part the way up the other side, to position h, descend, and then part the way up the first side, but not as far as h, etc.
The total energy at the outset = the total energy once the ball has come to rest at the bottom of the ramp. If there was x Joules of U(GPE) at the beginning there is x Joules of energy now, but in different forms.

#8 Re: Help Me ! » Factorising harder quadratics » 2025-06-21 03:08:52

Thanks, Bob; impressive, as ever.

I did Google the Maths Genie method; seems to be common, and called, The AC Method.

Recommended as a fail safe method for exams etc

I gave it a go with a few examples and found it less convoluted than I did a first.

#9 Re: Help Me ! » Factorising harder quadratics » 2025-06-20 08:37:53

Thanks, Bob, although I'm having second thoughts;

Two examples later and my method didn't seem to work, and theirs did;

6x^2 + 11x -10

P.S. Is there a BBCode for superscript that works here?

#10 Help Me ! » Factorising harder quadratics » 2025-06-18 10:48:27

paulb203
Replies: 7

Maths Genie method

Example;

5x^2+2x-3

1. Set out brackets thus; (5x   )(5x  )
2. Thinking in terms of ax^2+bx+c, multiply a by c, i.e., multiply 5 by -3, giving us -15
(We do this because we’re going to eventually divide our answer by 5)
3. Find factors of -15, i.e.,
    1,-15
    3,-5;
    -1,15
    -3,5
4. Choose pair that adds to give b term, i.e., 2, which is -3,5
4. plug those into prepared brackets re step 1;
(5x-3)(5x+5)
5. Divide by 5;
(5x-3)(5x+5)/5
=(5x-3)(x+1) which is your answer
Q. Is this not a convoluted way of doing this?
Q. Why not find the factor pair that gives the b term (2) when you multiply one of them by 5, the other by 1?

#12 Re: Help Me ! » cube root of x^6 » 2025-05-27 02:36:30

Thanks. Really helpful smile

(xi) is interesting.

How can a=b?

#13 Re: Help Me ! » cube root of x^6 » 2025-05-24 23:16:43

Thanks.

So the nth root of x = x^1/n ?

#14 This is Cool » Acceleration » 2025-05-24 22:56:48

paulb203
Replies: 1

According to ChatGPT, acceleration, before the time of Galileo and Newton, only meant to speed up, from the Latin, accelerare (to hasten).

It was during this period the word's modern meaning developed (to, change in velocity, i.e., speeding up, slowing down, or changing direction).

So when someone like Aristotle spoke of acceleration he only meant speeding up.

He also believed;

A force is required to maintain motion (which Newton later disproved).

Objects have a “natural place”, and they move toward it unless acted on otherwise.

Heavier objects fall faster (again disproved by Galileo).

#15 Help Me ! » cube root of x^6 » 2025-05-23 10:08:15

paulb203
Replies: 6

I'm looking for a hint, not the answer

#17 Re: Help Me ! » Vectors, +/- signs » 2025-04-29 23:05:43

Suppose the lift cable breaks and the lift tumbles down with only gravity acting. The man is now in free fall, effectively weightless and he could float off the floor so the reaction of the floor on him is zero.

Thanks, Bob. When you say ‘effectively weightless’ are you referring to his apparent weight as opposed to his true weight (terms I’ve just come across)?
So if the cable breaks his apparent weight, the weight he ‘feels’(?), the weight he ‘seems’ to be(?); but his true weight his what it always is regardless of other factors, like acceleration, i.e, the gfs of 10N/kg times his mass of 90kg?

If we compare with a parachute drop, the wind rush tells us we're falling.

I’m told this isn’t actually freefall because of the force of friction involved; is that correct?

In our imaginary lift drop the air moves with the man so he'd have no way of telling that he wasn't able to float.

So the air, being matter, stuff with mass, accelerates too, at -10m/s/s?
You said he’d have no way of telling that he wasn’t able to float; so he isn’t able to float?

Now if we imagine a lift that is so powerful it can accelerate downwards at 20 m/s/s.

Do you mean 20m/s/s on top of the 10m/s/s due to gravity? Or 20m/s/s in total (10 due to gravity, 10 due to it’s motor/whatever)?

The lift would drop faster than the man because he's already floating up, until he bangs his head on the ceiling. The reaction of the ceiling on him is definitely downwards.

Ah, so he is floating, floating up. Why? Why isn’t he being pulled down at 10m/s/s due to the gfs?

But how much?  He is trying to fall at 10 m/s/s but the lift is pushing him at 20.

10 due to the gfs, 10 due to the motor/whatever?

Effectively the force on him is 90 x (20-10) downwards.  So you need to subtract the lift's acceleration from gravity to determine the effective acceleration in the frame of reference.

The force on him from the ceiling is 90(20-10)?

It's like the moving train frames of reference.  If you 'bring the lift to rest' by applying an upwards acceleration of 2 m/s/s the gravity is similarly given that upwards acceleration so -10 + 2 = -8 m/s/s.

I think I’m partly getting that, but I’ll need to try harder to grasp it better.

So I think the reaction (upwards) is ( 10 - 2 ) x 90 N

I’m not quite sure I’ve followed the above to get here but 10-2(90)=720 which I think was the correct answer to my original question.

In really fast lifts you will notice the effect as your internal organs rise up inside your body.

Rise up in the reference frame of your body? From the reference frame of a viewing platform would your organs remain stationary for a moment while you plummet, like a gory episode of The Road Runner?

#18 Help Me ! » Vectors, +/- signs » 2025-04-28 22:57:56

paulb203
Replies: 3

90kg man in a lift

Assigned signs; DOWN is MINUS; UP is POSITIVE

Acc. due to g = 10m/s/s DOWNWARDS
Acc. due to g = -10m/s/s

Fg=ma
Fg=90(-10)
Fg=-900

*

acc. due to lift’s motor =2m/s/s DOWNWARDS
a=-2m/s/s

F=ma
F=90(-2)
F=-180
Fnet=-180

*

What is the normal force?

Fn-Fg=Fnet
Fn-(-900)=Fnet
Fn+900=-180
Fn=-180-900
Fn=-1080?

But the normal force is always is in the UPWARDS direction, which given the assigned +/- in this example, is +; The Fn should be POSITIVE.
Where have I gone wrong?

#19 Re: Science HQ » Inertia » 2025-04-27 23:04:51

Thanks, Bob.

I asked chatgpt about it.

I said,

"If inertia is 'an object's tendency to resist acceleration', and increasing velocity alters that tendency, then inertia must depend, at least partially, on velocity."

It replied with,

"And you're not wrong — if we use that broad, intuitive definition of inertia.


And then it got complicated, with how Newton actually defined things like mass, and acceleration, in terms of F=ma, etc.

I think I'll leave it for now, let it brew, and come back to it later. Thanks for your help with this one.

#20 Re: Science HQ » Inertia » 2025-04-25 23:26:09

Thanks, Bob.

Returning to,

"“If you set up a frame of reference that travels at 6 m/s in the second case, then the trolley is only travelling at 6 m/s relative to that frame and so can be 'brought to rest' in the frame with the same effort as the first case.”

What if we then look at a trolley travelling at 9m/s in the ground reference frame, and therefore travelling at 3m/s in the train reference frame?

Now, to stop the respective trolleys in 2s, we have;

Trolley A (6m/s in the train reference frame)

F=ma
F=100kg(-3m/s/s)
F=-300N

Trolley B (3m/s in the train reference frame)

F=ma
F=100kg(-1.5m/s/s)
F=-150N

So, in the train reference frame, we have two trolleys OF THE SAME MASS, (100kg), but more force is required to stop one than is required to stop the other, due to their different velocities.

#21 Re: Science HQ » Inertia » 2025-04-23 22:02:52

Fascinating. And mind-bending. For me at least.

So you, Bob, are driving a train, east at 6m/s.

And I’m driving a trolley east at 6m/s, parallel to you.

From the reference frame of your train I’m at rest.

And in your reference frame no force is required to stop me, because I’m already at rest? Even though we both know a force would be required to stop me in the reference frame of the ground beneath me?

#22 Re: Coder's Corner » BBcode Practice » 2025-04-22 23:12:20

I just found out what BB stands for in BBcode smile

Bulletin Board smile

#23 Re: Science HQ » Inertia » 2025-04-21 23:08:42

Thanks, Bob

So now we view the trolley in the second example in the reference frame of the train moving at 6m/s in the same direction as the trolley.
To stop the trolley in 2s;

F=ma
F=100kg(-3m/s/s)
F=-300N

But if we view the trolley in the second example in the reference frame of the train why not view the trolly in the first example from that reference frame?
It was moving at 6m/s with reference to the ground. Now it’s moving at 0m/s with reference to the train.
But we still want to stop it in 2s.
So,

F=ma
F=100kg(a)

What do we put for ‘a’?

A=(v-u)/t
A=(0-0)/2
A=0/2
A=0

So,

F=100kg(0)
F=0N
But we know that a force of >0N would be required to stop the trolley, don’t we?

#24 Re: Coder's Corner » BBcode Practice » 2025-04-21 09:50:29

Bob wrote:

Have I told you where to look for a long list of these?

Go to help and you'll find it in the third thread.

Thanks, Bob

Bob wrote:

Do I know them all? Certainly not!  I don't fill my head with stuff like that

So do you just get to know by heart the ones that you use frequently, without trying to memorise them; and consult the list when there's one you've either forgotten or didn't know by heart in the first place?

#25 Re: Science HQ » Inertia » 2025-04-20 23:16:52

“I just used those as examples.  There's no limit to the number of possible frames.”

Thanks, Bob. I thought that might be the case, but wanted to be sure.

“If you set up a frame of reference that travels at 6 m/s in the second case, then the trolley is only travelling at 6 m/s relative to that frame”

Do you mean something like;

Train heading west at 6m/s relative to ground.
Trolley on platform heading west at 12/ms relative to ground.
Trolley in reference frame of train = 6m/s west
(12m/s – 6m/s)?

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