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Physics: Post your doubts here!

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than
Q1) Suppose the particles are separated by a particular distance x, and their charges are as you have mentioned, one with a charge "q" and another with charge "Q-q".

Then, the coulomb force acting between them would be equal to:

F(Coulomb) = kq(Q-q)/x^2

Now, we want to know what values of q (in terms of Q) will result in the greatest force on each. Therefore, we want to find the maximum value of F(Coulomb) as q varies.

Therefore, we take the derivative of F(Coulomb) with respect to q and equate that to zero as follows:

d[F(Coulomb)]/dq = kQ/x^2 - 2kq/x^2

Setting this to zero, we get kQ/x^2 = 2kq/x^2
Cancelling out k and x^2, we get:
Q = 2q
q = Q/2


Substituting this value into the equation for F(Coulomb) we get
F(Coulomb) maximum value = kQ^2/(2x^2) Newtons

Q2) I can't really understand this question; is the final situation supposed to be stable or unstable? What is the magnitude of the charge to be placed between the +q and +4q charges?

Good Luck for all your exams![/qu
 
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Q20:- As:- P=ρɡɦ
Where P= pressure
ρ= Density
ɦ= height
So:- ɦ= p/ρɡ
And 10% of p0 is multiplied with the equation

h=
C:\Users\user\AppData\Local\Temp\msohtmlclip1\01\clip_image004.png
p0 x p/ρɡ = p0/10ρɡ

Q32:- Whenever u are asked to find the Current in a circuit then always use terminal voltage instead of e.m.f of battery..as some of the voltage is used up by the internal resistor
i.e. I= V/R = 7.5/15= 0.5A
Thanks
 
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Hey
someone help me on this. We all know Power= Fv . The driving force and resistive forces are given. So isn't the F in power= Driving Force-Resistive force?
why in the markscheme is it given F= driving+resistive force.
I've attached the question for your easiness!phy.jpg

The force in (d).i. is 75N :)
 
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Please explain me: What happens when-
1.The width of each slit is increased but the separation remains constant.
2. seperation of the slits is increased
 
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Somebody?

Well, for any stationary object, i.e. an object in equilibrium, the following two conditions have to be fulfilled:

i) No net force must act on that body (so that the centre of mass does not accelerate, or if the object is stationary, start moving);

ii)No net torque must act about ANY point chosen (for the angular rotation of a body to be zero; the center of mass can remain stationary and the object rotate about it, e.g. a ceiling fan).

This is an interesting point; IF and ONLY IF the object/ system at hand is stationary, you can take moments about ANY point, even if it is outside the system boundary, and still get the right answer (example coming up soon!).

So, to simplify matters here, there are three points about which the moment equations will be simplest:

i) Contact with floor;
ii)Contact with wall;
iii)Center of mass of ladder.

i) About an axis through this point into and out of the page, the weight tries to turn the body Anticlockwise, and the normal force from the wall tries to turn the ladder Clockwise.

An interesting thing about the torque of a force about an axis: To obtain that torque, join the point through which the axis passes to the point where the force is applied. Then, slide the force along it's direction (either in the direction it's pointing, or in the opposite direction) and do so until the line you've drawn, imaginary or real, is perpendicular to the force. The length of that line is the lever arm you use in the calculation.

So, in this case, the forces F and W(by the ground) have no torque. We can slide the Weight downwards, until the line joining that force and the point of contact is perpendicular to the force. Since the force is vertical, this happens when the line is horizontal. Therefore, the distance at the horizontal level is a so the torque is Wa.

For the force F(by the wall), we can slide the force towards the right or the left; sliding it to the right gives us a moment arm of h, since the force is horizontal, and so when the line joining the point of contact and the force vector is vertical, the length of that line is h, so the torque is Fh.

So, Fh = Wa

Well, not one of the options. So we repeat for the next point.

ii) About this point, the weight W rotates it Clockwise, Friction F rotates it Clockwise and F(by the Floor) W rotates it AntiClockwise.
So, for the point of contact with the wall, we move the Weight vector opposite it's pointing direction (we move it upwards) to give us a moment arm of a and a torque of +Wa, we slide the friction vector F to give us a moment arm of h and a torque of +Fh, and we slide the F(by the floor) W vector upwards to give us a moment arm of a+a = 2a and a torque of -2Wa.

Adding these us,

Wa + Fh + (-2Wa) = 0
And therefore,

Wa + Fh = 2Wa

Still, Cambridge examiners are devious guys. :mad: We could have rearranged that option from Wa + Fh = 2Wa to give us Fh = Wa, which we would have gotten first.
Oh well. It happens;).

Either ways, going back to that earlier point, suppose we took moments about the corner in the wall.
Then we'd get:

Torque due to force F exerted by the wall = +Fh

Torque due to force W exerted by floor = -2Wa

Torque due to force W exerted by earth's gravity = +Wa

The sum would still have given us Fh = Wa.

Hope this helped!
Good Luck for all your exams!
 
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Hey
someone help me on this. We all know Power= Fv . The driving force and resistive forces are given. So isn't the F in power= Driving Force-Resistive force?
why in the markscheme is it given F= driving+resistive force.
I've attached the question for your easiness!View attachment 38508

The force in (d).i. is 75N :)

Let's think of this question in terms of net force:

We know that the boy accelerates at a constant rate until his velocity reaches 5.6 ms^-1. In part (ii), his speed is 4.5 ms^-1, so he hasn't yet finished accelerating.
From the earlier part, we know that the acceleration of the boy is 1.12 ms^-2 (5.6/5.0 = 1.12) and so we know by Newton's Second Law that:

F(net) = ma

OR

(Net Force on Boy+Bicycle) = (Mass of Boy+Bicycle) * (Acceleration of Boy+Bicycle)

Since the acceleration is 1.12 ms^-2, we can write

(Net force on Boy+Bicycle) = 67 * 1.12 = 75.04 Newtons

So, the net force on the boy+bicycle must be 75.04 Newtons for as long as they are accelerating.

However, we are also told that at this speed, a force of 23 Newtons acts against the boy's speed; there is a negative force of 23 Newtons on the system, which tries to decelerate it. Therefore:

Force applied by the boy - 23 Newtons = 75.04

Therefore, to continue accelerating himself and the bicycle at a constant rate of 1.12 ms^-2 when a resistive force of 23 Newtons acts on them, the boy has to apply 98.04 Newtons of force (more accurately, though, the ground has to apply this force).

So, If we apply P = Fv here, we get
P = 98.04 * 4.5 = 441.18 Watts = 440 W.

The key point here is that in P = Fv * cos(θ),

P = the power of a particular force (which is the work is done per unit time) in Watts;
F = the magnitude of that force in Newtons;
v = the rate at which the position vector of the object being accelerated by that force and
θ = the angle between the Force and Velocity vectors.

Here, since the angle between the two is zero, cos(θ) is equal to 1 and P = Fv.

Hope this helped!
Good Luck for all your exams!
 
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Heyy here;s a question from M/J/13 paper 42 ...

Q. state and explain the effect on the transmitted analogue waveform of increasing, for the ADC and the DAC, both the sampling frequency and the number of bits in each sample.


the answer in the marking scheme is:
increasing number of bits reduces step height
increasing sampling frequency reduces step depth / width
reproduction of signal is more exact


I get the sampling frequency part but not the part about increasing no. of bits... can anyone explain please??
 
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Well, for any stationary object, i.e. an object in equilibrium, the following two conditions have to be fulfilled:

i) No net force must act on that body (so that the centre of mass does not accelerate, or if the object is stationary, start moving);

ii)No net torque must act about ANY point chosen (for the angular rotation of a body to be zero; the center of mass can remain stationary and the object rotate about it, e.g. a ceiling fan).

This is an interesting point; IF and ONLY IF the object/ system at hand is stationary, you can take moments about ANY point, even if it is outside the system boundary, and still get the right answer (example coming up soon!).

So, to simplify matters here, there are three points about which the moment equations will be simplest:

i) Contact with floor;
ii)Contact with wall;
iii)Center of mass of ladder.

i) About an axis through this point into and out of the page, the weight tries to turn the body Anticlockwise, and the normal force from the wall tries to turn the ladder Clockwise.

An interesting thing about the torque of a force about an axis: To obtain that torque, join the point through which the axis passes to the point where the force is applied. Then, slide the force along it's direction (either in the direction it's pointing, or in the opposite direction) and do so until the line you've drawn, imaginary or real, is perpendicular to the force. The length of that line is the lever arm you use in the calculation.

So, in this case, the forces F and W(by the ground) have no torque. We can slide the Weight downwards, until the line joining that force and the point of contact is perpendicular to the force. Since the force is vertical, this happens when the line is horizontal. Therefore, the distance at the horizontal level is a so the torque is Wa.

For the force F(by the wall), we can slide the force towards the right or the left; sliding it to the right gives us a moment arm of h, since the force is horizontal, and so when the line joining the point of contact and the force vector is vertical, the length of that line is h, so the torque is Fh.

So, Fh = Wa

Well, not one of the options. So we repeat for the next point.

ii) About this point, the weight W rotates it Clockwise, Friction F rotates it Clockwise and F(by the Floor) W rotates it AntiClockwise.
So, for the point of contact with the wall, we move the Weight vector opposite it's pointing direction (we move it upwards) to give us a moment arm of a and a torque of +Wa, we slide the friction vector F to give us a moment arm of h and a torque of +Fh, and we slide the F(by the floor) W vector upwards to give us a moment arm of a+a = 2a and a torque of -2Wa.

Adding these us,

Wa + Fh + (-2Wa) = 0
And therefore,

Wa + Fh = 2Wa

Still, Cambridge examiners are devious guys. :mad: We could have rearranged that option from Wa + Fh = 2Wa to give us Fh = Wa, which we would have gotten first.
Oh well. It happens;).

Either ways, going back to that earlier point, suppose we took moments about the corner in the wall.
Then we'd get:

Torque due to force F exerted by the wall = +Fh

Torque due to force W exerted by floor = -2Wa

Torque due to force W exerted by earth's gravity = +Wa

The sum would still have given us Fh = Wa.

Hope this helped!
Good Luck for all your exams!
Thanks! Your detailed method of explanation was very helpful.
Could you help me with my other query too? It's posted above.
 
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Thanks to ZaqZainab

when S2 is closed the "path of least resistance" will take up most of the current
so the current would flow through S2 rather than through B cause here B has resistance
for (i) we use power= VI
we don't have I so we replace I with V/R which we take from the equation R=V/I
power=v^2/r
R=38.4
ii) they are talking about total poser
so if S1 open there is no power you get this one right because the circuit is not complete
S1 and S2 closed as i said current always takes easier path so it will not go through B so in P=IV I=O the P is also 0 for B but then the current flows through A so its 1.5k+0=1.5k
if all of them are closed here again we will take power of B as 0 and if you see we have A and C in parallel Total power=P1+P2......... SO 1.5+1.5
S1 is closed so so we have A and B in series 1/total power = 1/p1 + 1/p2 +............
so 1/total power= 1/1.5 +1/1.5
total power =0.75
here s1 and S3 are closed so we have A and B parallel to C ie (AB) parallel to C for parallel Total power=P1+P2.........
and we already found AB which is 0.75 so now we just need to add 1.5
 
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Thanks to ZaqZainab

when S2 is closed the "path of least resistance" will take up most of the current
so the current would flow through S2 rather than through B cause here B has resistance
for (i) we use power= VI
we don't have I so we replace I with V/R which we take from the equation R=V/I
power=v^2/r
R=38.4
ii) they are talking about total poser
so if S1 open there is no power you get this one right because the circuit is not complete
S1 and S2 closed as i said current always takes easier path so it will not go through B so in P=IV I=O the P is also 0 for B but then the current flows through A so its 1.5k+0=1.5k
if all of them are closed here again we will take power of B as 0 and if you see we have A and C in parallel Total power=P1+P2......... SO 1.5+1.5
S1 is closed so so we have A and B in series 1/total power = 1/p1 + 1/p2 +............
so 1/total power= 1/1.5 +1/1.5
total power =0.75
here s1 and S3 are closed so we have A and B parallel to C ie (AB) parallel to C for parallel Total power=P1+P2.........
and we already found AB which is 0.75 so now we just need to add 1.5

thank you so much! :)
 
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unique111
Potentiometers are variable resistors. Potentiometers are resistors where the resistance can be changed using a knob or a slider. Potentiometers are used to control many things, including how bright or dim the lights in your house are and the volume controls on your television.

There are many different types of potentiometers. These different types include carbon potentiometers, plastic potentiometers, and wire potentiometers. Carbon potentiometers are the most common potentiometers that we use today because they are inexpensive to make and are easy to put together. Wire potentiometers are the most powerful type out of the three listed above. The wire inside the potentiometer is wound so that it has more power. Plastic potentiometers have the same amount of power that carbon potentiometers do, but are of a higher quality. They are made of a special kind of plastic that conducts electricity just as effectively as carbon potentiometers. It as a better life than carbon potentiometers do. Trimmer potentiometers are small.


If more help : http://www.wikihow.com/Wire-a-Potentiometer

Detailed notes : http://web.cecs.pdx.edu/~eas199/A/topics/circuits/pot_voltage_divider.pdf
 
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