Understanding Electric Fields
Electric fields describe the force exerted by a charge on a test charge and are fundamental in physics. The electric field (E) is defined as the electric force (F) experienced by a small test charge (q), given by the formula:
[ E = \frac{F}{q} ]
Units of electric field are newtons per coulomb (N/C), emphasizing the force per unit charge.
Vector Nature of Electric Fields
- Positive test charge: Accelerates in the same direction as the electric field.
- Negative test charge: Accelerates opposite to the electric field direction.
Electric fields are vectors pointing:
- Away from positive charges
- Toward negative charges
For a deeper conceptual understanding, see Understanding Electric Charges and Forces: A Comprehensive Guide.
Calculating Electric Fields from Point Charges
Using Coulomb's law, the magnitude of the electric field due to a point charge ( Q ) at a distance ( r ) is:
[ E = k \frac{|Q|}{r^2} ] where ( k = 9 \times 10^9 \ \text{N·m}^2/\text{C}^2 ).
- ( Q ) is the charge magnitude in coulombs.
- ( r ) is the distance to the point of interest in meters.
When calculating, use a tiny positive test charge to avoid influencing the source charge.
For additional worked examples and calculation methods, refer to Understanding Electric Fields and Gauss's Law in Physics.
Determining Electric Field Direction
- For a positive source charge, field vectors point radially outward.
- For a negative source charge, field vectors point radially inward.
Examples involve identifying directions at various points around a charge, using arrows drawn from charge to point (positive source) or point to charge (negative source).
Practical Problem Solving
Example 1: Finding Electric Field Magnitude and Direction
Given a force of 100 N acting north on a -20 μC charge, deduce:
- Electric field direction: opposite the force direction for negative charge → south (270°).
- Electric field magnitude: ( E = F / |q| = 100 / (20 \times 10^{-6}) = 5 \times 10^{6} \ \text{N/C} ).
Example 2: Charge Suspended by Electric Field
A 50 μC positive charge is suspended in an upward-pointing 50,000 N/C field.
- Equate electric force ( (E q) ) to weight ( (m g) ) for equilibrium.
- Calculate mass: ( m = \frac{E q}{g} = \frac{50,000 \times 50 \times 10^{-6}}{9.8} \approx 0.255 \ \text{kg} ).
Example 3: Electron Acceleration in Electric Field
An electron accelerates east at ( 4 \times 10^6 \ \text{m/s}^2 ).
- Electric field points west (opposite to force on negative charge).
- Calculate magnitude: ( E = \frac{m a}{|q|} = \frac{9.11 \times 10^{-31} \times 4 \times 10^{6}}{1.602 \times 10^{-19}} = 2.27 \times 10^{-5} \ \text{N/C} ).
Example 4: Electric Field at Various Distances
Calculate the field at points near a 40 μC charge:
- At 5 m along x-axis: ( E = 14,400 \ \text{N/C} ) east.
- At point 3 m east and 4 m north (5 m distance): same magnitude, direction 53.1° north of east.
For related phenomena where electric fields interact with potentials and capacitors, consult Understanding Electric Potential, Fields, and Capacitors in Physics.
Key Takeaways
- Electric field depends directly on charge magnitude and inversely on the square of distance.
- Direction depends on the sign of the charge and relative position.
- Forces on charges and resulting accelerations can be analyzed using Newton’s laws combined with electric field equations.
- Problems often require combining vector direction with precise calculations for magnitude.
Essential Constants for Calculations
- Coulomb's constant ( k = 9 \times 10^{9} \ \text{N·m}^2/\text{C}^2 )
- Electron mass ( 9.11 \times 10^{-31} \ \text{kg} )
- Electron charge magnitude ( 1.602 \times 10^{-19} \ \text{C} )
- Proton mass ( 1.67 \times 10^{-27} \ \text{kg} )
This comprehensive guide serves as a foundation to confidently understand and solve electric field problems in physics.
in this video we're going to focus on electric fields let's begin our discussion
with the formula that will help us to calculate the electric field
the electric field is equal to the electric force that is acting on
a tiny test charge divided by
the magnitude of that test charge so it's f over q the force is measured in newtons
the charge q is measured in coulombs so electric field has the units newtons per coulomb
now the electric field is a vector much like force is a vector but the good thing about the electric
field is it tells you how the electric force is going to be
acting on a positive or negative charge
so let's talk about positive charges first what happens
if we put a positive test charge in an electric field and that test charge is going to fill a
force that will accelerate it in the same direction as the electric field now what about a negative test charge
what's going to happen if we put it in an electric field a negative test charge
will fill a force that will accelerate it in the opposite direction to the
electric field so make sure you understand that positive charges
they accelerate in the same direction as the electric field the force and electric field vectors will be in the
same direction but for negative charges
they will fill a force that will accelerate it in the opposite direction of the electric field
now as we said before an electric field can exert a force on
any type of charge a positive charge or a negative charge but it turns out that charges
can also create their own electric fields the electric field created by a positive
charge extends in all directions away from the positive charge
the electric field created by a negative charge extends in all directions
toward the negative charge so it's going inward towards the negative charge in all directions
now let's talk about the equation that will help us to calculate the electric field
created by a point charge so let's say we have okay let me draw a better circle
let's say we have this charge which we'll call big q and we want to calculate the electric
field at some point a
how can we do that and let's say a is some distance r well we know that
the electric field at point a will be going in this direction all you need to do is draw an arrow
from the positive charge to the point of interest and that will give you the direction
of the electric field now let's say if we place a tiny positive charge
at point a so let me just erase point a so this tiny positive charge will be considered our test charge the reason
why it has to be tiny because if it's large enough it will affect
q big q will be repelled by little q but if the magnitude of little q is very
very small it won't affect big q as much and thus it won't affect the electric
field that is created by big q as much so that this equation will work if we choose a very tiny positive test charge
now according to columbus law whenever you have two charges next to each other they will
exert a force in each other two like charges will fill a force that will repel them
and we can calculate that force using this equation it's equal to k times q1 which we'll call big q
times q2 which we'll call little q over r squared where r
is the distance between the two charges so what we're going to do now is we're
going to take this equation and substitute it for f in that equation
but first i'm going to rewrite this equation as f over 1 times 1 over q
that's the same as f divided by q so now let's replace f with what we see here
so this is going to be f i mean it's no longer f but it's going to be k big q times little q
over r squared so this whole thing is f and then we're going to multiply it by 1
over q and so we could cancel out little q the test charge
thus we get the equation that gives us the electric field or the magnitude of the electric field
for a point charge capital q so it's k q over r squared
so if we have our charge q and we wish to calculate the electric field
at point a we could use this formula k
is 9 times 10 to the 9 newtons
times square meters over square coulombs q is the magnitude of the charge in
columns now remember one micro coulomb is one times ten to the minus six
coulombs a nano clue is 10 to the negative nine clues and a
milli clue is 10 to the minus three columns and r is going to be the distance
in meters now let's say we have a positive charge here
and we have point a let's say point b
point c and point d determine the electric field
created by the charge q at points a b c and d
so at point a the electric field in order to draw it we're going to draw starting from the
positive charge towards point a and so the electric field is going north
for point b we need to draw towards point b so the electric field the direction
is west for point d it's going to be at an angle so it appears to be going in the
the northwest direction and for point c just draw towards point c
so it's going in uh oh wait i have to make a correction that is not northwest that is north east
and this is southeast now let's do something similar but with a negative charge
so for the sake of practice go ahead and determine the direction of the electric field
at the following points so point a point b
point c and point d so this time the electric field is going
to point toward the negative charge so we're going to draw it from the point to the negative charge
so this electric field vector is going west
and then here we're going to draw it from v towards the negative charge so this is going in the south direction
and then d to the negative charge here it's going east and then from c to the negative charge
this electric field vector is pointed in the northwest direction so that's how we can determine the
direction of any electric field vector that is created by some type of charge either a
positive or negative charge and we could determine the direction of that vector at any point
using examples such as these but now let's focus on some word problems
number one a force of 100 newtons is directed north on a negative 20 micro coulomb point
charge what is the magnitude and direction of the electric field at this point
so feel free to pause the video and work on this example problem so let's begin by drawing a picture
so let's draw our negative point charge now there is an electric force that is
acting on this charge and that electric force is directed north what is the direction of the electric
field now if you recall if we have an electric field pointing
east and if we were to place a positive test charge in that electric field
it will fill a force in the same direction as the electric field
but a negative charge will fill a force that will accelerate in the opposite direction
so if the electric field is due east
the electric force acting on the negative charge will be west
so if the force is north what is the direction of the electric
field actin on this charge q it has to be in the other direction
it has to be south so that is the direction of the electric field
it's direct itself now if we want an angle we can draw this this is 0 90
180 270. so the electric field is directed along
the negative y-axis so we could say that it's at an angle
of 270 degrees relative to the positive x-axis
and that is in a counterclockwise direction so those are the ways in which we can
describe the direction of the electric field we could say it's
due south or it's at an angle of 270 degrees so now that we have the direction
of the electric field let's calculate the magnitude of the electric field
so we could use this formula we can take the electric force and divide it by the magnitude of the charge
the force acting on it is 100 newtons the magnitude of the charge we don't
need to worry about the negative sign since we already know the direction the charge is 20 micro coulombs
and we can replace micro with 10 to the six i mean 10 to the minus six
now let's do some algebra let's see if we can get this answer without the use of a calculator
we could divide a hundred by twenty how many twenties would make up a hundred bucks that's gonna be five
twenty so a hundred divided by twenty is five now the ten to the minus six if we move
it to the top the negative exponent will become a positive exponent so the negative six
will change to positive six and thus the answer is going to be five times ten to the sixth
and the units in newtons per coulomb so that is the electric field that's acting on this negative charge
number two a positive charge of 50 micro coulombs is placed in an electric field of 50 000
newtons per column directed upward what mass should the charge have to remain
suspended in the air well let's talk about how we can create such an electric field
we can create this electric field using a battery and two
parallel metal plates so this is the electrical symbol of a battery
we're going to connect it to these two plates this is the negative side of the battery
and this is the positive side so this plate is going to acquire a positive charge
and this plate is going to acquire a negative charge so if we choose a high enough voltage
and if the distance between the two plates is just right we can adjust it such that we get an
electric field of 50 000 newtons per coulomb now we want the electric field to be
directed upward so we want the positively charged plate to be at the bottom the negatively
charged plate to be at the top remember the electric field always extends away from a positive charge and points
towards a negative charge so this is how we can create a uniform electric field using two parallel plate
i mean using two parallel metal plates now let's place our positive charge
in the middle between these two plates if this charge has the right mass it can actually remain suspended in the
air now let's talk about it so we have an electric field that is
directed upward and it's acting on its positive charge what will be the direction of the
electric force on its charge the electric force will be the same
direction as the electric field for a positive charge so the electric force will be directed
upward now gravity gravity likes to bring things down
so gravity is going to exert a weight force on this positive charge
bringing it down in the negative y direction in order for this charge to remain
suspended in the air the electric force that wants to accelerate the charge
towards the negatively charged pay that has to be exactly equal to the gravitational force or the weight force
that wants to bring the positive charge down towards the
towards this plate so if we can get these two forces to equal each other
then the positive charge will remain suspended in the air so let's write
the forces in the y direction the sum of the forces in the y direction is equal to the electric force this is
positive and the weight force is negative because it's going in a negative y direction
and we want the the sum of the forces in the y direction to be zero so that there's no net acceleration so it
remains suspended in the air moving this term to the other side we see that the electric force has to
equal the weight force now the electric field is equal to f over q
multiplying both sides by q we can see that f the electric force is
the electric field times q so let's replace the electric force with e times q
now the wave force is simply mg so now we have everything that we need in order to calculate the mass of this
charge let's divide both sides by g so the mass of the charge is going to be
equal to the electric field times the magnitude of the charge divided by the gravitational
acceleration the electric field is 50 000 newtons per coulomb
the magnitude of the charge we're dealing with uh a 50 microclimate charge so it's going to be 50
times 10 to the negative 6 coulombs and then we're going to divide that by the gravitational acceleration of 9.8
meters per second squared so it's 50 000 times 50 times 10 to the minus 6 divided by 9.8
and you should get .255 kilograms
so an electric field of 50 000 newtons per coulomb can suspend
a positive charge with a mass of 0.255 kilograms or 255 grams it can suspend it in the air
if the mass is greater than this number then the charge will fall down if it's too light if the mass is less
than this number then the charge will accelerate towards the negatively charged plate
so the mass has to be at the right number in order for it to remain suspended
number three an electron is released from rust in a uniform electric field and accelerates
to the east at a rate of four times ten to the sixth meters per second squared
what is the magnitude and direction of the electric field so let's draw a picture
so first let's draw our electron and then it is
accelerating towards the east now according to newton's second law the net force is equal to the mass times the
acceleration the net force is in the same direction as the acceleration
so the electric force exerted by this electron due to the electric field is going to be due east as well
now if the electric force is east what is the direction of the electric field
it's going to have to be west let me put it here when dealing with a negative charge the
direction of the force and electric field they will be opposite to each other
so now that we have the direction of the electric field let's focus on getting the magnitude of
the electric field so from the last problem we saw that the electric force
is equal to the electric field times the charge and
using newton's second law we can replace the force with the mass times the acceleration
so now we can calculate the electric field if we divide both sides by q so for this problem
the magnitude of the electric field is going to be the mass times the acceleration which is the force
divided by the charge so the mass is what is the mass of an electron if you
look it up the mass of an electron is 9.11 times 10
to the negative 31 kilograms the acceleration given to us in this problem
is 4 times 10 to the 6 meters per second squared
and then we're going to divide that by the magnitude of the charge so what is the charge of an electron
the charge of an electron is negative 1.602 times 10 to the negative 19 coulombs
so these are some numbers that you want to be familiar with so let's put that here
so let's go ahead and plug in these numbers by the way don't worry about the
negative sign for q it's not going to be relevant here so the magnitude of the electric field
is going to be 2.27 times 10 to the negative 5 newtons per coulomb
so this is the answer for this problem and the direction is
west so make sure you write down these numbers
the mass of an electron as we've considered is 9.11 times 10 to the negative 31 kilograms
the mass of a proton is 1.67 times 10
to the negative 27 kilograms the charge of an electron
it's going to be a negative 1.602 times 10 to the negative 19 coulombs
the charge of the proton it's going to have the same magnitude but the opposite charge is going to be
positive 1.602 times 10 to the negative 19 coulombs
so those are some numbers that you want to be familiar with when working on problems associated with
electric fields if you're dealing with protons and electrons number four
a 40 micro coulomb point charge is placed at the origin calculate the magnitude and direction of
the electric field created by the point charge at the following locations
so let's draw the point charge first now point p is five meters away
from the point charge along the x-axis so this is point p and this is five meters away
what is the electric field at point p well we know the direction the direction of the electric field
is going to be east if we draw it from the positive charge
towards point p now to calculate the magnitude of the electric field it's going to be k
q divided by r squared so k is 9 times 10 to 9 and then it's
newtons times square meters over square columns
and i'm running out of space so i'm not going to put the units here i'm just going to write 9 times 10 to the nine
q is 40 micro clones so 40 times 10 to the minus 6 coulombs
r is in meters r is the distance between a charge and the point of interest
so that's five meters so it's going to be nine times 10 to the 9
times 40 times 10 to the minus 6 over 5 squared and so the electric field is going to be
14 400 newtons per coulomb
so that's the magnitude of the electric field at point p and this is the direction
for those of you who want to understand how the units work here it is so k is in newtons
times square meters over square coulombs q is in coulombs and r is in meters so we have square meters
as you can see square meters cancel now coulomb squared we can write that as coulomb times coulomb
so we can cancel one of the coulomb units thus we're left with newtons per coulomb
which is what we have here so that's it for part a so it's 14 400 newtons per coulomb directed east
now let's move on to part b so let's calculate the electric field at point s
so q is at the origin point s is three meters
east of q and then four meters north from that point
so s is at this position here the electric field
can be drawn from q to s so the electric field is going in that direction it's going in the
the northeast direction let's calculate the magnitude of the electric field
so let's use this formula again it's going to be k q
over r squared so k doesn't change it's a constant it's 9 times 10 to 9.
q is still the same it's 40 times 10 to the minus
but r is different r is no longer the value that we have here
but in actuality it turns out r is the same r
is the distance between the charge and the point so we need to use the pythagorean theorem to calculate the
hypotenuse of that right triangle so this is a b and this is c so c squared is equal to a squared plus
b squared a is three b
is four three squared is nine four squared is sixteen
and then nine plus sixteen is twenty five taking the square root of both sides
we get 5 again so by coincidence the electric field is going to have the same magnitude
as it did in part a which was uh 14 400
newtons per coulomb what's going to be different though is the direction of the electric field
vector how can we determine the direction we know it's somewhat in the northeast
direction but not necessarily at a 45 degree angle what we need to do is calculate theta
so perhaps you remember from trigonometry sokotova
if we focus on the torah part that tells us tangent tangent of theta is equal to the
opposite side divided by the adjacent side so tangent of the angle theta is going
to be equal to four over three to calculate theta we need to take the arc tangent
or the inverse tangent of four over three go ahead and type in your calculator and
make sure it's in degree mode so arc tangent 4 3 is
53.1 degrees so that is the angle with respect to
the positive x-axis it's 53.1 so we could say that this is the
electric field vector at an angle of 53.1 degrees with respect to the x-axis or we could say
53.1 degrees north of east because here we're starting from east
and we're heading towards the north direction so it's 53.1 north of east
so that's it for part b so that's how we can calculate the magnitude of the electric field vector
and also its direction using arctangent number five an electron initially at rest
is placed in an electric field of two times ten to the four newtons per coulomb directed to the west
the distance between the plates is one centimeter what is the acceleration of the electron
due to the electric field so the electric field will emanate away from the positive charge and will point
towards the negative charge so as we can see the electric field is directed west
now what effect will it have on the electron a negatively charged particle will fill
a force that will accelerate it in the opposite direction to the electric field so the electron is going to shoot out of
this uh between these two parallel plates let's calculate the acceleration
we know the force acting on a charged particle is equal to the electric field times the charge of that particle
and since this is the only force acting on the electron in the x direction then that force
is going to be the electric force so we can replace the net force with m a based on newton's
second law so m a is equal to e times q and to solve for a we're going to divide
both sides by m so for part a the acceleration is going to be the force which is e
times q divided by the mass so we have an electric field of 2 times
10 to the 4 newtons per coulomb and the charge of an electron is 1.602
times 10 to the negative 19 coulombs we're not going to worry about the negative sign the mass of an electron is
9.11 times 10 to the negative 31 kilograms so let's go ahead and plug this in
so the acceleration is 3.517 times 10 to the 15
meters per second squared so that's going to be the acceleration when the electron
leaves the negatively charged plate so now let's move on to part b
what would be the speed of the electron after it leaves the hole so how can we get that
so now we need to go back to kinematics the electron is initially at rest so v initial is zero
we're looking for the final speed so we'll put a question mark and we know the distance between the
plates it's approximately it's one centimeter
so what kinematic formula has acceleration v initial v final and d it's going to be this one
v final squared is equal to v initial squared plus 2 a d
so to solve for the final speed we simply need to take the square root of both sides
so v final is equal to this the initial speed is zero this is going to be two
times the acceleration which is 3.517 times 10 to the 15.
and the distance between its plates is one centimeter so if we convert one centimeter into meters
we need to divide by 100 and it's going to be 0.01 meters and so we're going to get the square
root of 7.034 times ten to the thirteen and so the final speed
is about eight million and three hundred eighty six thousand eight ninety four point
five so we can round that to let's say 8.39
and this is times 10 to the sixth meters per second so that's how fast the electron is going
to be moving when it leaves the hole number six a 200 micro coulomb charge is placed at
the origin and a negative 300 micro coulomb charge is placed one meter to the right of it
what is the magnitude and direction of the electric field midway between the two charges and then for the second part
30 centimeters to the right of the negative charge so let's start with the first part of
the problem let's begin by drawing a picture so this is going to be the first charge
we'll call it q1 and the second charge q2 so these two charges are separated by a
distance of one meter and we want to determine
the magnitude and the direction of the electric field midway between the two charges
so that's going to be at this point how can we do that well we need to determine the direction
of each electric field at that point q1 is going to create an electric field
called e1 which will be directed east now q2 will create an electric field e2 which starts from the point but points
towards the negative charge and that's going to be directed east as well
so remember the electric field created by a positive charge extends away from the positive charge
but the electric field created by a negative charge points towards the negative charge
so at the center e1 and e2 they are in the same direction so the net electric field
is going to be e1 plus e2 along the x-axis or the horizontal axis both of these are positive because
they're going in the positive x direction e1 is k
times q1 over r1 squared e2 is k times q2 over r2 squared
now what's r1 and r2 so r1 is the distance between q1 and the point of interest
r2 is the distance between q2 and the point of interest
so r1 and r2 they're both half of point of one meter which means that r1 and r2 they're both equal to 0.5
so because r1 and r2 are the same we can simply call it r so let's replace r1 with r
and let's replace r2 with r as well so now we could simplify this equation
by factoring out the gcf the greatest common factor which is going to be k
over r squared and then we're left with q1 plus q2 so this is the formula that we could use
to calculate the net electric field for this particular part in the problem now let's go ahead and plug in the
numbers so it's going to be k which is 9 times 10 to the 9
over r squared r is 0.5 and then times q1 q1 is 200
times 10 to the negative six now for q2 we're going to use a positive value not
negative 300 times 10 to the negative six because we already know the direction of
e2 it's going to the right and it's going to have a positive value because it's heading
in the eastward direction so whenever you're calculating the magnitude for electric field or electric
force you don't need to include the negative charge
you could just find the direction based on where the arrow is going so let's replace q2 with 300
times 10 to the negative six coulombs so 200 plus 300 this becomes 500 so it's
9 times 10 to the 9 times 500 times 10 to negative 6
divided by 0.5 squared thus the net electric field is 18 million which is 1.8
times 10 to the 7 newtons per coulomb so that's the answer for part a
now let's move on to part b so let's redraw the picture for that so here we have our positive charge
and the negative charge so we got q1 q2 and they're separated by distance of
one meter but 30 centimetres to the right or 0.3 meters
we're going to have our new point of interest and let's call this
point b so we want to determine the net electric field at point b
so e1 the electric field created by q1 if we draw it from q1 to point b we could see that it's going east
now if we draw an electric field from point b to q two because it's a negative charge it needs
to go towards a negative charge it's going to the left now which of these two electric fields
is greater e1 or e2 what would you say notice that point b is closer to the negative charge
than it is to the positive charge so e2 is going to have a greater effect than uh i mean q2 is going to have a
greater effect on point b than q1 because it's closer so if you go back to the equation for
electric field there's two things that the electric field depends on
the magnitude of the charge and the inverse square of the distance but the distance is square
so the distance has a greater impact than the charge but also
q2 has a bigger charge in q1 so those are two factors that favor q2 over q1 point b is closer to q2
and q2 has a greater uh charge magnitude than q1 so therefore we can conclude that e2 is
going to be bigger than e1 now the net electric field is going to be positive e1 because it's
going along the positive x-axis and then plus negative e2 because that's moving towards the west or the
negative x-axis now if e1 is bigger than e2 the net electric field will be positive
if e2 is greater than e1 it's going to be negative and we've confirmed that e2 is going to be bigger so we should get a
negative value if we get a positive value for the net electric field we did something wrong
so let's go ahead and do the math so then that electric field is going to be k
q 1 over r 1 squared plus k
q q2 over r2 squared so this time r1 and r2 will be different
so we can't simplify this process by factoring so let's plug in the numbers this is k
q1 is 200 oh this should be a negative sign by the way
based on what we have here so q1 is 200 times 10 to negative 6. now r1
r1 is the distance between q1 and point b so r1 is going to be the sum of one and
point three thus r1 is 1.3 meters squared and then minus
now because we've considered the direction of e2 we've assigned a negative value
we don't need to plug in this negative value for q2 we've already taken that into an account
so it's to be minus k and then q2 we're going to use the positive value of q2
300 times 10 to the minus 6 and r2 that's the distance between q2 and point b
that's 0.3 meters so let's calculate e1 first let's focus on this fraction
nine times ten to the nine times two hundred times ten to the negative six divided by one point three squared
that's one point zero six five times ten to the seven
newton newtons per coulomb now focusing on e2
that's gonna be nine times ten to nine times three hundred times ten to negative six
divided by point three squared so this is 3
times 10 to the 7 newtons per coulomb so we can see that this number is bigger than that number
so the net electric field is going to be negative 1.065
minus 3. wait something is wrong let me double check my work
this should be times ten to the six not ten to the seven that's one million sixty five thousand
and eighty eight so that's one point zero six five times ten to six e2 is 30 million which is three times
ten to seven so now if we subtract those two numbers we get this answer
negative two point eight nine
times so it's 28 million nine hundred thirty five thousand
so it's negative two point eight nine times ten to the seven newtons per coulomb
so we can see why it's negative e2 is significantly larger than e1
and so that's it for this problem number seven the electric field at point x
two meters to the right of a certain positive charge is 100 newtons per coulomb
what will be the magnitude of the new electric field if the magnitude of the positive charge doubles in value
so let's draw a picture first so here is our positive charge and let's say this is
point x and the distance between these two is two meters
now at that point the electric field is a hundred newtons per coulomb when the magnitude of the charge is
we'll call it q but what happens if we double the magnitude of the charge
so the electric field is k q over r squared if you double q
the electric field is going to double a quick and simple way to get the answer is to
plug in 1 for everything that that doesn't change q doubles so we're going to plug in 2
r remains the same so the electric field is going to double it's going to go from 100 to 200.
now what about part b let's say the distance between the charge and point x doubles
so let's say point x is now over here and the magnitude is q what will be the new electric field
so this time q doesn't change k is the same so we're going to replace it with a 1. everything that doesn't
change replace it with 1. now the distance doubles two squared is four so the electric
field is going to be one-fourth of its original value one-fourth of a hundred or hundred
divided by four that's 25 so what you need to take from this is
that the electric field is weaker at a greater distance away from the charge
the closer you move towards the point charge the greater the electric field will be
so as the distance increases the electric field decreases but as the distance from the point
charge decreases the electric field increases there's two ways in which you can
increase the electric field you can increase the magnitude of the charge
which will cause the electric field to go up or
you could reduce the distance between the point of interest and the charge and that will also increase the electric
field now let's move on to part c the distance between the charge
and point x reduces by a factor of three so what's going to be the the magnitude of the new electric field in that case
so we're bringing it a lot closer to q so here's the new uh position of x
so here the distance doubled to 4 meters but now it's going to be reduced by factor three so it's two thirds
of a meter so let's use this formula again for part c k and q doesn't change
r is now one third of its original value one times one is one one squared is one three squared is nine
now we need to multiply the top and the bottom by nine one times nine is nine
one-ninth times nine the nines cancel we get one so the electric field is going to
increase by a factor of nine a hundred times nine is nine hundred so as you can see as we get closer
to the point charge the magnitude of the electric field greatly increases
now what happens if we triple the magnitude of the charge but at the same time reduce the distance
to one-fourth of its original value so i won't draw a new picture for this let's just get the answer
so k doesn't change q triples
and the distance is reduced to one fourth of its value so we have one times three which is
three one squared is one four squared is sixteen
so now i'm going to multiply the top and the bottom by sixteen so it's going to be three times sixteen
which is forty eight so the electric field will increase by a magnitude of forty eight
so the original electric field was a hundred if we multiply that by 48 the new electric field will be 4 800
newtons per coulomb so this right here is the answer to part d so the reason why it's so high is
because we've increased the charge which causes e to go up and at the same
time we reduce the distance which greatly increase the value of e
so that's it for this problem number eight two identical point charges with a
magnitude of a hundred microclimbs are separated by distance of one meter as shown below
part a at what point will the net electric field be equal to zero will it be to the left will it be
between q1 and q2 or to the right so let's identify three points of interest
the first point will be somewhere to the left which we'll call point a
the second point will be somewhere in the middle between q1 and q2 likely the midpoint
and then c will be to the right now to draw the electric field vector created by q1
we need to draw a line from q1 to point a this is going to be e1
and for e2 we're going to draw it from q2 to point a
so at point a both electric fields are moving to the left
so there's going to be a net electric field at point eight it's not going to be zero but here's a question for you
which electric field will be greater e1 or e2 now remember
these charges are identical so the magnitude of the charge is the same the only thing that's different is the
distance q1 is closer to point a than q2 so e1 is going to be bigger
than e2 so this is e1 e2 is going to be a smaller vector nevertheless the net electric field at
point a will be directed west now what about at point c to draw e1 we're going to draw
a line from q1 to point c and e2 will be from q2 to point c now which one is bigger
q2 is closer to point c than q1 so e2 is gonna be bigger at point two i mean e2 is going to be bigger at point
so for e1 we're going to draw a small vector and for e2 we're going to draw a bigger
vector nevertheless the net electric field at point c will be directed east
now what about at point b e1 is going to be directed away from q1 but towards point b
e2 will be directed away from q2 but towards point b and q1 and q2 have the same charge and
at the midpoint at point b they will be equally distant from point b so if the charges are the same and the
distances are the same the magnitude of e1 and e2 will be the same but they're opposite in direction which means that
e1 and e2 cancels so at point b the net electric field is zero
so let's assume that q1 is the origin it's at position zero point b will be at 0.5 meters
so at 0.5 meters relative to the first charge then that electric field
will be zero e1 and e2 will cancel completely so that's the answer for part a
at point b or at the midpoint between q1 and q2 the net electric field will be
zero now what about part b if the charge on q2
doubles to 200 micro coulombs where along the x-axis relative to the
first charge will the net electric field be equal to zero
and the distance between these two is still the same you think the net electric field will be
equal to zero between q1 and b or between b and q2 now q2 is bigger
than q1 so at point b where they're equidistant e1
is going to be a smaller vector than e2 e2 is going to be twice as large in order
to make these vectors equal we need to increase e1 and decrease e2 if we can't change q1 and q2 the only
thing we could change is location we need to move closer to q1 as we move closer to q1 e1 is going to get bigger
e2 will get smaller and at some point they're going to equal each other so we're going to place point p
between q1 and b somewhere between q1 and b the net electric field will be equal to
zero and we need to find that point so that point is going to be r1 r2
is the distance between q2 and point p now let's call r1x if r1 is equal to x what's r2
notice that the total distance is 1 so r2 is going to be 1 minus x
if you add x and 1 minus x you're gonna get one so at this point
all we need to do to get the answer for part b is
get the value of x because x represents the distance relative to the first charge where the
net electric field will be equal to zero so how can we calculate x the net electric field at point b
remember at point b we have e1 which is going towards the right and e2 i mean at point not b but point p
at point p we have e1 going to the right and e2 is going to be going to the left so because e1 is going to the right it's
positive e2 is going to the left it's negative now we want
point p is defined as the point where the net electric field is zero so e1 minus e2 will be zero if we add e2 to
both sides we'll get that e1 is equal to e2 they have to be the same in magnitude
but opposite direction e1 is k q1
over r1 squared e2 is k q2
over r2 squared now let's divide both sides by k so we can cancel
that term let's replace r1 with x so we have q1 over x squared and let's
replace r2 with one minus x don't forget to square it
now let's cross multiply so here we're going to have q 2 times x squared
and then this is going to be q 1 times 1 minus x squared now let's replace q2 with
its value and let's keep the unit micro coulombs so we have 200 micro coulombs times x
squared q1 is a hundred micro coulombs
and what we're going to do at this point is we're going to divide both sides by 100
micro coulombs so the unit micro coulombs will cancel on the left side
on the left we have two hundred over one hundred which is two so we get two x squared is equal to one
minus x squared now we don't need to foil 1 minus x squared
what we could do is take the square root of both sides so we're going to have the square root
of 2 and the square root of x squared is just x the square root of 1 minus x squared is
just 1 minus x now the square root of 2 is 1.414 so now we need to do some algebra
let's add 1x to both sides let me write that better so there's a coefficient of one here
as we add one x to both sides my handwriting is just not working today i don't know why one point four one x
plus one x is two point four one x and we can bring down the one on the right side
so we have two point four one x i mean two point four one four x is equal to one so to get x by itself we
need to divide both sides by two point four one four
so x is going to be one divided by two 2.414 and so we get 0.414
so at 0.414 meters to the right of q1 which is point p at that point
the net electric field will be equal to zero so that's how we can calculate the exact
location along the x axis where the net electric field will be
equal to zero if q1 and q2 have different magnitudes of charge you
An electric field represents the force exerted by an electric charge on a small test charge placed nearby. It is mathematically defined as the force (F) experienced per unit positive test charge (q), given by the formula E = F/q, where the electric field E has units of newtons per coulomb (N/C).
The direction of the electric field depends on the sign of the source charge: for a positive charge, electric field vectors point radially outward away from the charge; for a negative charge, they point radially inward toward the charge. A positive test charge moves along the field direction, while a negative test charge moves opposite to it.
Use Coulomb's law with the formula E = k |Q| / r², where E is the electric field magnitude, k is Coulomb's constant (9 × 10⁹ N·m²/C²), Q is the source charge magnitude in coulombs, and r is the distance in meters from the charge to the point of interest. This gives the field strength at that point due to the charge.
First, note the charge's sign and the force direction. Since E = F/q, calculate magnitude by dividing force magnitude by the absolute value of the charge. Determine direction: for positive charges, electric field aligns with force; for negative charges, it points opposite. This approach combines force analysis and knowledge of charge sign to find the electric field vector.
Set the electric force equal to the gravitational force for equilibrium: E × q = m × g, where E is the electric field strength, q is the charge, m is mass, and g is gravitational acceleration (9.8 m/s²). Rearrange to find mass or electric field as needed, such as m = (E × q) / g for a given electric field and charge.
Because an electron is negatively charged, it experiences a force opposite to the electric field vector direction. To find field strength when given acceleration (a), use E = (m × a) / |q|, where m is electron mass and q is electron charge magnitude. This calculates the electric field magnitude causing the given electron acceleration.
The electric field magnitude decreases with the square of the distance from the charge, following E = k |Q| / r². Direction depends on position relative to the charge—field vectors radiate outward or inward depending on charge sign. For points not along a principal axis, calculate vector components considering distances along each axis to find overall magnitude and direction.
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