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hey guys and welcome to another as
mechanics video so this is the actual
last topic before we can move on to
doing some past papers for the year 12
content and then of course I'll St
uploading year 13 content as well but of
course we've got quite a few papers to
get through at the same time now you
might notice we're only going to go
through four questions in this topic and
the reason for that is that this comes
up in every single past paper so we're
actually going to get a lot more
questions done than you might think and
this is a fairly involved topic it while
it is called pulley it's basically
connected particles and also a little
bit of sousat and also some resolving
forces Allin one as well so we're going
to be using pretty much everything and
of course we're going to be drawing
diagrams so if we read the question two
particles A and B have a mass of 04 and8
kilos respectively they're connected by
light and extensible string so remember
what that means uh light means that uh
their detention is the same throughout
and inextensible means that the
acceleration is identical so for example
when if particle B moves then particle a
moves with the exact same acceleration
at the exact same time particle a lies
on a rough horizontal table 4 and a half
met from a smooth a small smooth pulley
so what this means is that there's no
kind of uh Force lost due to the pulley
so that means the tension on both sides
of the pulley is going to be identical
which is fixed at the edge of the table
so we can probably start drawing out
some of this stuff so if we draw our
little flat surface here well that's
terrible let's try again
there we are and then we draw that and
then we have a pulley like so we have
particles A and B so a is the one on the
table so I'm actually going to draw it
as a box um just for personal preference
technically it should be a circle but it
doesn't really matter that much and then
obviously the other one's going to be
dangling over the edge and we're going
to join them by a little string like
so cool and then we have this is 4 and
1/2 m so I'm am going to add this onto
the thing because they wouldn't give me
the information if it wasn't useful at
some point in the
question and we have the masses so
particle a is4 kilos so that's going to
be 0.4
G and particle a is8 kilos
whoops which is going to be 0.8 G so
because they're connected by string
we're going to have tension now tension
in a connect in a pulley question looks
like this now again remember when you
stretch something tension acts to to
unstretch it so this string is being
stretched over the table so mean tension
is going to act like so it's going act
upwards for particle
B particle a is going to act to the
right and hopefully this makes a bit of
sense because if you look at this
situation if it is accelerating then a
is going to accelerate to the right and
B is going to accelerate down because
there's no other way that it would make
sense right it doesn't make sense for B
to accelerate upwards and a to
accelerate to the left because there's
nothing causing that so the thing that's
causing that is going to be the tension
because of the
weight so we got that done and it says
that it hangs freely string torch torque
just means that it's there's no slack in
it 0.5 m above the ground so what we
could do is also draw this and say 0.5 M
now of course with the acceleration we
don't know it but if it is accelerating
it's going to be accelerating down and
to the
right and anything else a frictional
force oses the motion of particle a so
that's going to be going this way which
is 0.08 G that's quite nice of them to
provide they release as the systems
releasing rest find the acceleration
okay so just like with connected
particles what we can do and this is a
very Nifty trick is we can actually um
resolve them separately okay which is
extremely extremely useful so I'm
actually going to move this uh diagram
over so I can actually draw on it so
what I mean by that is we can actually
resolve particle a and particle B
separately now the key part here is I
can't just combine them do you remember
how in the connected particles thing
because they're moving in the same
direction we were able to treat them as
one big particle in this case are they
moving in the same direction no they're
moving horizontally and also vertically
but it's also like it's not in the same
Dimension either so we can though
resolve them completely separately which
is really really useful
and 99% of the time you want to resolve
particle B first the one that's hanging
over the edge first why well if we have
a look it has fewer unknowns
so in short with pulley you're going to
resolve both particles anyway because
generally speaking there's multiple
unknowns so let's start with this the
reason why I said there's multiple is
because in this case there technically a
resultant force a a normal reaction
force over there so let's resolve
particle B and again I'm going to take
downwards as positive because I always
take the direction of acceleration as
positive and because we don't know if
it's accelerating or not it's going to
be FAL Ma and this is how we're going to
figure out if it is accelerating so the
force at the moment we have 0.8 G acting
downwards minus the tension is equal to
the mass which is 0.8 * a and again
maybe that's zero maybe that's not but
we don't know then we're going to
resolve for particle a and I take
direction of acceleration so to the
right is positive again I don't know if
it's accelerating but if it is
accelerating it's going to be going to
the right and again we use f
M8 and here we have T minus
0.08g =
0.4 a so we have two equations and two
unknowns and if we have a look something
very interesting has happened here we
have a negative T and here we have a
positive T So if I were to add these two
equations together so if I write them on
top of each other 0.8 G minus t = 0.8
a and then here we have
0.08 sorry no we don't I don't know what
I'm writing that for we have T minus
0.08
G = 0.4 a if we were to add those two
equations together we would be solving
this simultaneous equation by
elimination which is really
useful hopefully that makes sense
technically you can use a calculator to
solve simultaneous equations by the way
so there is a simultaneous equation
solver but I would recommend doing it
this way so add these two equations
together we get 0.8 G plus minus 0.08 G
so that would be 0.72 G because it's
just going to be subtracting the t's
cancel out which is exactly what we want
equals 1.2 a so a is just equal to
whatever 0.72 G ID 1.2 is so let's have
a look see shall we
0.72 * 9 8
1 ided 1.2 gives me an answer of
5886 so we normally round to three
significant figures so we have 5.89
m/s squared and that first part is
probably worth three or four marks I do
have some exam questions coming up these
are exam style questions but they are
made a tiny bit simpler just for the
purpose of demonstration but I do have
some more coming uh
soon perfect it the common mistake I see
is that people kind of assume that this
pulley this part of the pulley is going
to accelerate downwards at 9.81 but that
doesn't make sense it's being slowed
down by a okay
perfect so now we have the acceleration
that's really really useful it says find
the time taken for B to reach the ground
so this is where suac comes into place
because our acceleration is going to be
constant until it hits the ground but
that's fine because it says the time
taken for it to reach the ground so
let's write out all the variables we
know well the displacement the height
above the ground is 0.5
M what's the initial velocity well it
says it's released from rest so the
initial velocity is going to be zero do
I know the final velocity nope
acceleration is
5.89 and lastly we have time is equal to
well that's what we want to work out so
let's write down the variables we want/
have so we have s u a t so s u t plus
half a^2 would probably be the one I
use half a CU again don't forget it's
freeall right so it's normally going to
be the S UT formula and of course for
the first equation uh for the first term
is going to be zero and that means we
can rearrange T to be T is equal to the
< TK of 2 s /
a so squ < TK 2 *
0.5 over 5.89 this is going to be quite
a small number which fair enough it's
only moving half a meter so square root
and that's going to be 1 over
5.89
0.412
seconds like
so
perfect now here's where things get a
bit more
interesting we have here
a particle now it says the total
distance traveled by a before it comes
to rest so first of all since it's
attached to a light and extensible
string it is going to travel the exact
same distance as B initially so it's
going to have half a meter already
locked in okay because again that b is
pulled a half a meter before it hit the
ground now when it hits the ground the
string is now not providing a tension
force there's no tension here because
it's gone slack B is not pulling
anything
anymore hope that makes sense so what we
have to do and this is a bit tricky is
we have to work out the velocity of
a and then we need to use the fact that
it's going to be
decelerating find out the distance and
add it on this last part is normally
worth five marks so it is a bit involved
so so first thing I'm going to do is and
again because this is an inextensible
string whatever the velocity of B is is
going to be whatever the velocity of a
is correct because it's tra it's I mean
it's joined okay so we're going to work
out the final velocity now we can use
any equation we want so I'll probably
use v = u plus a for this one so the
velocity is going to
be once again that's zero so it's just
literally going to be 5.89
ultip by
0.41
2
so
5.89 multiplied by whoops our answer
gives us
2.43
m/s so again just to give you context B
has dragged a and allowed it to get to a
speed of 2.43
m/s it's then hit the ground so now is
no longer being dragged but now we're
going to
have this situation here so after the
string is slack
after and again this is where pulley
gets tricky we're going to do a lot of
practice with this so it's
fine it now behaves just like a regular
old box which has a mass of4
it has a deceleration or sorry an um
frictional force of
0.08 and there's no other forces so now
what we have to do is work out the
acceleration now how do we do that well
it's actually quite nice and easy it's
just FAL
ma the only Force we have is 0.08 now
which way do we want to take is positive
well we could take forwards as positive
still right if we wanted to because it's
going to be decelerating that would make
a bit of sense - 0.08 G equal 0.4 a so a
is equal to 0.08 G over
0.4 let's put that in and see what we
get so we get let's put in Brackets just
to make sure everything goes well with
the
calculator whoops I pressed X not times
there we are over
0.4 and we get - 1.96 I'm going to call
it okay I know this is a lot so again
the box has already traveled half a
meter and in that time has accelerated
to 2.43 m per second it's now slowing
down because the string is slack there's
no forward Force so if we set up suat
now as it is I don't know it's not this
half a meter this half a meter is before
remember and this is the a key thing
when we use suat we're using constant
acceleration when we did this half a
meter the acceleration was positive 5.89
now the acceleration has changed we have
to set up new equations the initial
velocity is
2.43 what the final velocity B it would
be zero because we're seeing how far it
travels in total a is
1.96 and T is I don't know and I don't
really care so s u v and a so the
equation that comes to my mind is V2 = U
^2 + 2 as
s so V is of course zero so now if we
push this everywhere let's say s is now
going to be u^2 netive U ^2 over 2 a so
that is going to be -
2.43 s over 2 *
-1.96 like that
cool minus
2.43 squar over
2us
1.96 gives me 1.51 m let's call
it so again it travels5 Me by itself and
then it slides for another 1.51 M so the
total is
0.5 Plus
1.51 which is of course
2.01 M to
3sf that took 15 minutes because of what
the explaining but I will point out that
all of these parts together usually
amounts to about N9 or 10 marks
sometimes up to 12 okay so we're going
to look at the other situation they can
put in Pulley there's only two which is
quite nice but you may notice the actual
structure is the same so the first
question ask you to find tension or
acceleration the second one it kind of
implies you need to work out some kind
of speed and the third one is we're
still going to do the same thing find
the greatest height so otherwise we're
going to find the total distance
traveled which is the same thing as the
first one and that's what you're going
to notice with every single pulley
question so although it does seem very
very
tricky once you kind of do it once and
you get it you can do any one of these
questions the final part is always going
to be something along the lines of find
distance traveled some kind of distance
now okay there might be a Part D where
it says State how you've used the
modeling
assumptions but that's it in terms of
calculations this is the kind of
structure they're going to always follow
every single time so I said this is a
slightly different situation because if
you notice it doesn't mention any kind
of table or uh horizontal surface
because this is actually just a normal
pulley so let me show you how it
looks that is a pulley and then it's
going to droop down either
side and this is where I actually use
normal
particles and let's call them A and
B it doesn't matter which way around you
label them because you will get the same
thing
regardless and they are four and 3 Kg as
long as you label them with the right
measurements of
course like I literally just didn't as
soon as I said that I wrote the wrong
number there there there we go and of
course the tension is still going to be
acting upwards like
so now the acceleration which way does
it make sense to accelerate well it
makes sense for a to drop because it's
the heavier one and again because we
have no tension in the pulley that means
that there is um there's no way for a to
not accelerate right in this case CU
it's smooth a is definitely accelerating
downwards no question about it in the
first question we had tension and
tension sorry we had friction which
could in theory stop it from moving but
in this case nope no way 0% chance
so they release from rest cool find the
tension so in the previous question it
said find the acceleration but if you
notice we're going to be doing the same
thing we're going to be resolving for A
and B separately and then we're going to
be solving for acceleration or tension
now if I look ahead a little bit it says
find speed which means we're going to
need acceleration anyway so I'm just
going to work out both because we will
need it at some point
so part A find tension well let's
resolve for particle a and we're going
to take downward is positive because
it's my direction of acceleration FAL ma
a so what forces do we have well we have
4 G Going downwards subtract the tension
is equal to 4 a that is my first
equation then we have particle B and
we're going to take upwards as
positive and this is actually why I like
being consistent so technically speaking
there's nothing stopping me from taking
downwards as positive again
realistically but it makes it means that
I won't be able to eliminate it as
easily I'll have to use substitution or
I'll have to subtract or do something
else this way all I need to do is add
adding with simultaneous equations is
less prone to error because when you
subtract you might need to do like minus
t minus minus t or something which I
know it doesn't sound super hard but in
an exam lots of students make mistakes
so again that's just another reason why
I always always take
um the direction of acceleration to be
positive so here again we can see all we
need to do is add and this is actually
quite easy 4 g - 3 G is just G minus t
and t cancel so we just have G is equal
to 7 a so in other words a is just equal
to a 7th G so we've got our acceleration
which is we're going to use for Part B
nice perfect but that's not what we were
here for we wanted tension so if I sub
this into equation number two and move
3G to the other side
I get T is equal 3 * a so 3 a 7 of
G plus 3 G so you could work this out in
terms of G so in some mark schemes you
might see them give answers as fractions
of G so in this case it be 3 over 7 + 3
so that would be what 24 over 7 G so you
could have it as 24 24 over 7 G and
you'll find that in quite a few mark
schemes or you can and that's just
because it keeps it nice and um a whole
number like it makes it a precise value
or if you just did 24 / by S Times by
G that is also perfectly fine either way
you want to do it so I'm going to just
leave it as a three significant figure
number because it really doesn't make
much of a difference if you take three
sigfigs but that is our value for a so
we have two different values well
they're the same value there written
differently that would probably again be
for about three marks when a is Trel a
distance of 2 m it strikes the ground
and immediately comes to rest so again
it does tell you which one's actually
going to be accelerating it's a ex um
accelerating downwards dropping find the
speed of a when it hits the ground okay
so if we do suat we have S is equal to 2
m u is equal to zero it's released from
rest V is equal to don't know and that's
what we want a is equal to a 7th of
G and it actually tells me doesn't tell
me the time
cool so v = u + 2 s is probably what I
would
use and once
again U goes to zero nice and easy so V
is just equal to the square < TK of 2 *
a 7th
G multiplied by S which is again
two excuse the really poor handwriting
at times soqu < TK 2 and we have G so
9.81 /
7ti 2 gives me a pretty hideous number
2.37 m/s so let's keep it as
that that would be a two
marker pretty solid and then it says
assuming that b does not hit the pulley
find the greatest height so they've
actually done a lot of work for us a lot
of
work but we still need to do some of it
ourselves so again for C I like to write
that there is an initial 2 meters
we have the Velocity but once again the
acceleration is not the same otherwise
it would actually keep accelerating
forever right because it's just going to
Ping off into the space it's going the
acceleration should be going downwards
now and why is that well it's actually
just a freeall question right it's
actually not too bad so if we look at
particle B now we have particle b as a
downwards force of 3G and that's
actually
it right so that means the acceleration
is also going to be down now the really
useful thing about writing in terms of
3G let me show you is because FAL ma we
have 3G equals 3 a so in other words a
is just going to be
G so that's actually one of the reasons
we use um we use G all the time because
it actually tells us what the
acceleration is straight away now
remember all objects on Earth accelerate
with G if they're under freeall so in
this case it's under free in the
previous case it wasn't under freeall it
was being dragged along a surface so in
this case it's of course going to be G
because it's falling so let's work this
out so s is don't know and again we're
actually going to take upwards as
positive for all of this I know that
that means this will be negative and and
yada yada
yada U is going to be upwards
2.37 we're going to look at when V is
equal to Z a is going to be negative
negative G why because again it should
be slowing down this object and T I
don't really care so again we can use V2
= U2 + 2 as
s oop get rid of that and if we
rearrange this for S we
get U ^2 over 2
a so - 2.37
S I just had Deja Vu I've done so many
of these questions in the past that it's
um
incredible perfect so if you want we can
actually use an exact value and whenever
you can you may as well use an exact
value because it's it's fun uh 2 *
9.81 yeah that's all good 2 over 7 wow
that's a really precise number
0 286
M so in total and again you want to make
really clear that you're doing a total 2
+
0.286 so I'm going to do that to 3 SF so
2.29 M so you can see how we're doing
like the same thing again and again and
again it's quite
nice and we're definitely building up to
that A2 knowledge which is fun and again
this kind of question will come up every
single year 12 exam period um I don't
think I've seen a paper that hasn't had
it in there um but again we're going to
do every single Paper anyway so I'll be
able to prove that to
you hello there check this out seven
10 13 14 marks you see what I mean so
they're between 10 and 14 sometimes even
15 marks these questions pretty beefy
indeed but they give us a diagram which
is very nice of them so uh which one's
going to be accelerating downwards well
if we look how here it says Q reaches
the plane so Q is heavier so again
that's fine all I'm doing this for is to
make my diagram accurate so it's not
actually like it's cheating at all you
can't really cheat in
uh in math sad L uh and that would be K
mg and this would
be 3 mg we have tension going up that's
all our forces a k is less than three oh
okay so we could have just looked there
never mind it does tell us in the
question particles connected by light in
extensible blah blah blah pass smooth
light fixed pulley yeah cool the systems
held at rest with the string Tau and
blah blah blah blah blah the same height
above a horizontal so that's a really
key Point here is that they're at the
same height which is probably why they
gave us the diagram by the way they've
been quite nice systems released from
rest and oh hello it tells us the
acceleration 1.3 1 over 3G that is very
nice of
them and part A it says calculate the
tension so once again all we're going to
do is we're going to resolve for both of
these particles so let's resolve uh q
and we're taking downwards as positive
um whoops there we are FAL ma
the we have three mg going downwards we
have a tension going upwards m is 3 m
that's also a thing that make if some
people make mistakes they write 3 a
instead of 3 ma a in this case m is 3 m
which is very confusing I do 100%
wholeheartedly agree with
you let's do the same thing for Mr
P and we
have K actually no know we have tension
minus
kmg equals km by the way there's
actually one thing that I want you to I
want you to know and I think it's really
important for teachers to tell you this
I don't know how we're going to do this
straight away so what do you do when you
don't know and bear in mind there's a
lot of mechanics questions where I don't
know kind of the full method that will
get me to the answer so what do you do
you always resolve every particle in
every direction that you can as at the
moment we're only really dealing with
one dimension right we're doal with up
and down okay but when we come on to A2
you'll find that you can resolve up down
and left right sometimes so in general
with mechanics if you're stuck if you
just look at this and you go I have no
idea what I'm going to do just resolve
everything that you can and that
sometimes leads to a um realization of
what you can
do so let's have a look at this shall we
um it says we need to calculate the tens
in the string so that probably means we
we may need to work out acceleration
actually no we know we know what
acceleration is so we have two unknowns
we have two equations don't we so what
we can do is we can actually add these
two things together which I know it's
going to get rid of the tension but
let's have a look 3 mg minus kmg so
let's write that
out I know what you're screaming but sir
isn't there three unknowns you're a very
clever
person there is three unknowns but I'm
going to show you why I don't
care and this again is why you should
just do it because there's m in every
single term I can divide everything by m
now there's only one
unknown cool
right so that's the kind of um I want to
say it's the kind of skill that you need
to develop but you just need to have
that confidence okay resolve things in
every direction and then you know start
trying to eliminate stuff and speaking
you'll come to a
solution hopefully that makes sense we
can divide everything by n so we have 3
G minus kg equal 3 * a 3 is just going
to be G Plus K over 3
G so what I want to do is I want to move
this kg over to this side and this G
over to this side so 3 G minus G gives
me 2G then we have K over 3 + G Plus kg
so that would then be um
should we do that it would be 4 over
three 4K over
3G get rid of the G's so then uh we can
work out what K is just by doing the
opposite so 2 * 3 is going to be 6 6 / 4
so half it gives me three half again
1.5 now again that's not the question
however look at Part B show that K is
equal to
1.5 good so we've actually done Part B
which is fine what we can do now is we
can actually label that as Part B and
that counts so this is another thing
that's I really really adore about the
mechanics exams is you have a lot of
freedom so you can do Part B before you
do part A and use Part B to do part A
and I have no quals about that so this
is now my part B working out so how
would you do uh part A without doing
Part B first well what you'd have to do
is rearrange for K and sub it
in pretty ugly right so instead I've
made my life a lot
easier uh we could sub this back in um
actually can we no we can't sub it back
in all right I was trying to be a bit
lazy so what we can do is sub this into
this equation here and try and eliminate
M instead so doing that will give us the
correct answer but just so you're aware
you could have done um rearranged for k
or rearranged for M and subed it in and
you would have gotten uh the tension in
that way but for this case we need to
wipe out the tension so what I'm going
to do is I'm going to subing the K is
1.5 into this equation just so we have
it
so minus 1.5 mg
equals uh so we have 3
over2 time a thir which would be 1 / 2 G
so it' be 1 over
2
kg not K mg damn it all right here we
are G move the mg to the other side we
get T is equal to um a half plus 1.5 so
that's 3 over2 plus a half so that be 4
two which be 2
mg 2 mg like
so cool so from here we could either Sub
in that tension is equal to this work
out what m is and then work out what G
is and would that actually help
us I think it would um or we could
rearrange this for M and sub that in so
what I could do from here is I could say
that m is now equal to
t2g and sub that into one of our two
equations probably the top one because
we rearranged the second
one so
three T 2
G um minus t = 3 d 2
G time the thir G
so gather all of the t's to one side so
here we have if I factorize this out
factorize both these out we can get
T Gus one factor this T out we get
T um minus it to move it to the other
side
so I'm trying to do this all in one step
cuz I'm being a tad lazy I'm not going
to lie but we could move the T over and
then uh solve from there so let's go
through that so quick note uh we were
doing it correct this is the actual
final answer so all we need to do is
just mention that we've done part A down
here and we should be done so just erase
it back to here um back to k equals this
do this first step and then that will be
our answer we need to record a little
bit which says T = 2 mg is the answer by
the way
so if you notice uh we can't if I were
to sub this back in I can't actually
work out what the tension is as a number
and that's because in mechanics we can
leave our values as Expressions just
like this so This is actually completely
and utterly fine I can keep it as is so
that would be the answer to Part B now
for part C it says show how uh sorry
State how you've Ed the information that
the pulley is smooth well we use that
because the acceleration on both sides
of the pulley is the same so
acceleration both sides of
pulley is the same lastly we need to go
through part D which is a beefy seven
marker so let's get started with Part D
so after sending for 1.8 seconds the
particle Q reaches the plane is
immediately brought to rest by the
impact with the plane and the initial
distance blah so basically um
these last sentences that they write
here it just means that it doesn't hit
the pulley you know and in 99% of cases
it doesn't hit the pulley um they will
say like will it hit the pulley kind of
thing so if it's 2 MERS away and it
travels 2.1 M then yes it would hit the
pulley that kind of stuff so it also has
the answer in terms of G which is good
because our acceleration is in terms of
G so we're just going to leave
everything in terms of G if we can so
it's the same question but look at that
seven bloody marks that's a lot okay so
what we want to do is we want to work
out the final speed of
Q and also the distance that it travels
so if we look at just Q for a second so
uh let's look at particle
Q then it has the tension going up but
realistically I care about the
acceleration which is a third G and we
also know that so s is we don't know and
we do care we do want that U is zero
released from rest let's zoom in a
little
bit V is we also don't know a is a third
G and T was it told me I just can't
remember it was 1.8 seconds so from here
there's two things we want I want its
final velocity and the displacement
because that's going to be kind of the
um beginning distance so let's work out
let's work out V first because that'll
give me V is equal to U plus a and this
is quite nice because U is just zero so
it's just a thir
G time 1.8 and again because we want
everything in terms of G I'm actually
just going to do a third of 1.8 which is
0.6
G okay so then for S what should we use
what would be a good one um you could
use S U UT plus um UT plus a half a^
2 um yeah why not U is zero
and that means we get a
half third
G t^2 1.82 so what I'm going to do is on
my calculator is I'm going to put
in a half so 0.5 time a
thir
times uh bracket 1.8 or squar and it
gives me 27 over 50 uh is that all
correct it is okay it's a bit of an ugly
number 27 over 50 g let's leave it as
that so 27 over 50 g for S so this is
like the first part of the the distance
okay so if we look back at the question
the greatest height reached by P above
the planes 1.26 G well we have it's gone
up by 27 over 50g now there is a bit of
a stealthy nature to this so if you
remember p and Q were at the same height
okay so let me just draw out the
situation that's
happening that's P that's q and there's
a floor down here now Q has
dropped 27 over
50g yeah that means P must have started
off at 27 over
50g correct but now it's moved up so Q
has ended up down here and P has ended
up somewhere up here so it's gone up by
another 27 over
50g so it's an additional part I can
imagine that potentially being a bit
confusing so realistically this distance
is actually doubled because remember
what it's saying above the plane it
starts off already 27 over 50g and then
because Q has gone down 27 over 50g this
side must go up 27 so in total it's two
lots of 27 over
50 I hope that makes sense I hope that
makes
sense so if we double that um we get
1.08
G you can probably see why it's like
seven marks now so now what happened is
p is no longer uh being dragged up so we
need to now work out the new
acceleration so we don't have a value
for tension
uh but that's fine because tension has
disappeared but we have kmg and if you
look our acceleration was in terms of G
beforehand anyway so if we write so
let's draw out the situation for p
now it's going down by kmg but if you
remember we worked out K as 1.5 so it's
1.5 mg
and that's it so if we do fals
ma again we want to take upwards as
positive can so we have - 1.5 mg equals
um I mean
1.5
M times
a those two things cancel out and we
left
with a isal to
G now you do see that once more so s is
equal to don't know U is equal to
0.6
G our final velocity is equal to uh z a
is going to equal G yeah this should be
fine and T is equal to don't know and we
want s so uh v = u + 2 a s just like
we've used
before so V is zero so our value for S
is going to be negative U 2 over 2 a
that's - 0.6 g^ 2
over uh 2 * negative G so -2 G uh what I
can do here is I can cancel a g and one
of those G's out so let's do that it's
going to be canceling that and
technically the squared so it's going to
be
0.6 s g over -2 cancel out the negatives
so that would be 0.36 0.18
G
and okay that works perfectly because if
you notice now the total height or the
max
height is 1.08 G Plus 0.18
G which gives us the 1.26 G that they
were talking about
earlier 1.26 G
now here's where the mistakes would
obviously be made is the timesing this
by two um I've taught stats and
Mechanics for six years and I have seen
this question
before but uh I did actually kind of
forget about it but then when I went
through it again before the lesson of
course I did realize very quickly so
with mechanics the wording is very
careful it's very particular now this
for seven marks isn't actually that bad
if you think about it but again the
timesing this by two is definitely where
people mess up and another thing that
people mess up on is when the answer is
in terms of G they don't do all their
working out in terms of G so what they
do is they'll let's say for example
instead of 27 over 50g they'll put it as
a decimal so I actually don't even know
what that would be as a decimal uh times
9.81 and the problem is now they're
dealing with numbers that are quite long
and so they might round it so then when
they then try and put it in terms of G
by dividing by G they've got the wrong
answer like then instead of getting 1.26
they might get 1.24 1.25 or 1.27 and
then they go where where have I gone
wrong it's like you haven't gone wrong
it's just that you've
rounded so keep that in mind if they
give you the answer in terms of G do all
your working out in terms of G it's not
that bad if anything makes it slight
easier maybe but I hope that makes sense
that was a very long question 4 marker
not bad we've got one more and then
we'll be done once again we have a
pretty annoying uh in terms of length
question if you look at the whole
paragraph yeah you need to get used used
to this unfortunately uh they do give
you quite a bit of information but what
I'll do is I'll start adding some of the
forces that you know are going to be
here so 1.5g it's obviously going to be
accelerating downwards because again it
it can't really
accelerate left so two two and a half
kilos so let's put that for Force there
it's a rough table so let's put the
friction there uh the tensions of course
going this way and this
way is K Newton so that frictional force
here is
K system released from rest okay let's
make sure we haven't done anything else
and then after release Q descends a
distance of8 m in
0.75 seconds by modeling p andq as
particles calculate the acceleration of
Q now there are a few things you can
consider uh one of which is of course
using suat to work out the answer to
this so we have S we have t and we have
U because it's from rest so we could
work out what a is from
there bit cheeky but you can absolutely
do it um by doing v u plus oh by doing a
is the the change of velocity or
something or v = u + 2 a s any one of
these things um but I think it again it
makes sense that even if you're not sure
you may as well just resolve for p and Q
and see what happens so for this
question because it's specifically
asking me for acceleration and they gave
me information in terms of suat let's do
suat so a part I we have S is equal to
0.8 U is equal to Z it's released from
rest V is equal to don't know and I
don't care a is equal to don't know but
I do care and T is equal to 3 3/4 of a
second so s u a and t the equation that
comes to my mind is s = u + a
t^2 which again because it's in free
four this is a equation we use all the
time that goes to zero we want a so
let's quickly rearrange times both sides
by two gives me 2
s uh so be 2 s over
t^2 so 2 *
0.8 over 0.75 2
let's have a look see and see what
happens two 0.8 close bracket uh
0.75 all
squared that gives me an answer of God
um 2.84 m/s squared three
marks three bloody
marks it's not bad is it not bad at
all part
two show that the tension is okay so
again this is where we're going to
actually start resolving now again I
would always recommend resolving p and Q
if you're unsure but if we have a look
at this P has two unknowns T and K we
know what a is now whereas Q only has
one unknown tension so let's resolve for
Q and we I like to take the direction of
acceleration which is downwards as
positive so again we're using classic
fals ma as usual so the downwards force
is its mass which is or sorry it weight
which is 1.5 G minus t equal Mass which
is 1.5 *
2.84 so if you were to rearrange this
you move the T to the other side move
this thing over to this side you get
that t is equal to 1.5
Gus 1.5 * 2.84 and we may as well put
that in Brackets because we obviously
mean to work that out first not too bad
I hope so 1.5 m by
9.81 subtract 1.5 MTI by oops
2.84 of
10455 let's say it's
10.
five I should actually put that these
are 3sf because they are answers so they
should realistically be given um
estimates for accuracy so that's four
marks
oh hang on it says 10.4 to three
significant yeah sorry 10.4 then that's
totally
fine if you're wondering why I got um
10.5 instead of 10.4 it's because they
used um 9.8 as their value for
G so we did get the right answer just in
case you're wondering uh the reason why
I always use 9.81 is because in some
exams and some exam boards they use 9.8
some they use 9.81 so it looks like um
they haven't mentioned it but they
mentioned it at the beginning of the
paper the annoying thing is is in some
papers some years they say 9.81 or in
some questions they say use 9.8 or use
9.81 so in this question obviously they
meant for us to use 9.8 so that's why I
got a slightly different answer but I
promise you in the question or the paper
they will tell you to use G is equal to
something 9.8 9.81 whatever it is plus
four marks four marks
come on it's like three lines of mats
and it's easy mats too not bad not too
shabby at all and that's again why I
love mechanics it's my favorite Topic in
math find the value of K well again
we're going to be resolving P again we
always resolve p and Q eventually anyway
and we only have one unknown which is K
nice and
easy and you might also notice that in
these mechanics questions they give you
a lot of information for free so for
example our questions show that here so
that means if you didn't get this right
part correct you can do part C still so
we have T minus K so T is 10 well it
says 10.4 to 3sf let's just use the
value they give us minus k equals mass I
can't remember the mass it was
2.5 times the acceleration which was
2.84 yeah got the memory of a Civ all
right so then K if we just rearrange
this is going to be 10.4 actually
K =
10.4 minus 2.5 *
2.84 not bad and this was an actual exam
question by the way so I know I normally
say I I won't put like all of the exam
questions in there I haven't put all of
them by the way but I just wanted to let
you know and in the textbook by the way
there are previous exam questions if
you're interested but after this this is
3.3 we are doing every every single P
paper in
existence Part B how have used the
information that the string is
inextensible simple the acceleration oh
sorry both particles accelerate at the
same time that's it and that's it for
pulley my goodness and that's it for as
mechanics and stats we're done so there
it's not that long which is really good
uh the bright side is A2 stats is three
chapters it's really small which is
really really nice mechanics is a bit
longer what we're going to do for now is
we're going to do a bunch of past papers
and what I will also do and you might
notice we're going to finish really
really early so what I'll do is I'll do
year 12 stuff as in the the past papers
every single one that should take us
until about January because there's
quite a few papers then we're going to
start A2 but before your actual exams in
May June July time I'm going to go back
and do some predicted paper some um
specimen papers Solomon papers basically
papers are extremely difficult I'll even
do some of the really difficult
questions in the textbook The Challenge
questions just to prepare you for your
exam okay so we will go back to year 12
stuff other than that hope you have a
wonderful day I'll see you in the next
one