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Important Work, Energy & Power Formulas for JEE and NEET

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1.
 
Work
 
done
 
by
 
variable
 
force
Suppose
 
we
 
have
 
to
 
calculate
 
work
 
done
 
in
 
moving
 
a
 
body from a
 
point
 
A( )
 
to
 
a
 
point
 
B( )
 
under
 
the
 
action
 
of
 
a
 
variable
 
force. 
So
 
the
 
work
 
done
 
by this
 
variable
 
force
 
in
 
displacing
 
a
 
body from point
  
to
  
is,
2.
 
Conservative
 
and
 
non-
conservative
 
forces
A force
 
is
 
said
 
to
 
be
 
conservative
 
if
 
work
 
done
 
by or
 
against
 
the
 
force
 
in
 
moving
 
a
 
body depends
 
only on
 
the
 
initial
 
and
 
final
 
position
 
of
 
the
 
body,
 
and
 
not
 
on
 
the
 
natural
 
path
 
followed
 
between
 
the
 
initial
 
and
 
final
 
positions.
If
 
the
 
work
 
done
 
by or
 
against
 
a
 
force
 
in
 
moving
 
a
 
body from one
 
position
 
to
 
another
 
relies
 
on
 
the
 
path
 
taken
 
between
 
these
 
two
 
places,
 
the
 
force
 
is
 
said
 
to
 
be
 
non-conservative.
3.
 
Power
 
definition and
 
relation between work
 
and
 
power
Power
 
is
 
defined
 
as
 
the
 
rate
 
at
 
which
 
work
 
is
 
completed
 
in
 
a
 
given
 
amount
 
of
 
time.
The
 
relation
 
between
 
work
 
( )
 
and
 
power
 
( )
 
is
 
expressed
 
as 
4.
 
Kinetic energy
 
and
 
linear
 
momentum
 
relation
The
 
energy of
 
a
 
body is
 
defined
 
as
 
the
 
capability or
 
ability of
 
the
 
body
 
to
 
do
 
the
 
work.
The
 
relation
 
between
 
kinetic
 
energy
 
(
)
 
and
 
linear
 
momentum( )
 
shows
 
that
 
a
 
body cannot
 
have
 
kinetic
 
energy
 
without
 
having
 
linear
 
momentum and
 
vice-versa.
 
           
Name of the Concept Key Points of the Concepts
Work,	Energy	and	Power
Page 2


1.
 
Work
 
done
 
by
 
variable
 
force
Suppose
 
we
 
have
 
to
 
calculate
 
work
 
done
 
in
 
moving
 
a
 
body from a
 
point
 
A( )
 
to
 
a
 
point
 
B( )
 
under
 
the
 
action
 
of
 
a
 
variable
 
force. 
So
 
the
 
work
 
done
 
by this
 
variable
 
force
 
in
 
displacing
 
a
 
body from point
  
to
  
is,
2.
 
Conservative
 
and
 
non-
conservative
 
forces
A force
 
is
 
said
 
to
 
be
 
conservative
 
if
 
work
 
done
 
by or
 
against
 
the
 
force
 
in
 
moving
 
a
 
body depends
 
only on
 
the
 
initial
 
and
 
final
 
position
 
of
 
the
 
body,
 
and
 
not
 
on
 
the
 
natural
 
path
 
followed
 
between
 
the
 
initial
 
and
 
final
 
positions.
If
 
the
 
work
 
done
 
by or
 
against
 
a
 
force
 
in
 
moving
 
a
 
body from one
 
position
 
to
 
another
 
relies
 
on
 
the
 
path
 
taken
 
between
 
these
 
two
 
places,
 
the
 
force
 
is
 
said
 
to
 
be
 
non-conservative.
3.
 
Power
 
definition and
 
relation between work
 
and
 
power
Power
 
is
 
defined
 
as
 
the
 
rate
 
at
 
which
 
work
 
is
 
completed
 
in
 
a
 
given
 
amount
 
of
 
time.
The
 
relation
 
between
 
work
 
( )
 
and
 
power
 
( )
 
is
 
expressed
 
as 
4.
 
Kinetic energy
 
and
 
linear
 
momentum
 
relation
The
 
energy of
 
a
 
body is
 
defined
 
as
 
the
 
capability or
 
ability of
 
the
 
body
 
to
 
do
 
the
 
work.
The
 
relation
 
between
 
kinetic
 
energy
 
(
)
 
and
 
linear
 
momentum( )
 
shows
 
that
 
a
 
body cannot
 
have
 
kinetic
 
energy
 
without
 
having
 
linear
 
momentum and
 
vice-versa.
 
           
Name of the Concept Key Points of the Concepts
Work,	Energy	and	Power
5.
 
Work
 
energy
 
theorem
This
 
theorem states
 
that
 
if
 
some
 
work
 
( )
 
is
 
done
 
by the
 
body then
 
the
 
kinetic
 
energy( )
 
of
 
the
 
body also
 
increases
 
by the
 
same
 
amount.
Work
 
done
 
=
 
increase
 
in
 
K.E.
 
of
 
the
 
body
6.
 
Potential
 
energy
 
of
 
a
 
spring
The
 
potential
 
energy ( )
 
of
 
the
 
spring
 
is
 
the
 
energy associated
 
with
 
the
 
state
 
of
 
compression
 
or
 
expansion
 
of
 
an
 
elastic
 
spring.
 
It
 
is
 
given
 
as
Here,
  
=
 
spring
 
constant
 
and
  
=
 
stretch
 
or
 
compression
 
in
 
the
 
string
7.
 
Mechanical
 
energy
 
and
 
its
 
conservation
The
 
total
 
mechanical
 
energy of
 
the
 
system
 
is
 
conserved
 
if
 
the
 
forces
 
doing
 
work
 
on
 
the
 
system are
 
conservative
 
i.e,
 
when
 
net
 
work
 
done
 
by external
 
non-conservative
 
force
 
is
 
zero.
The
 
mechanical
 
energy ( )
 
of
 
a
 
body is
 
the
 
sum of
 
kinetic
 
energy ( )
 
and
 
potential
 
energy ( )
 
of
 
the
 
body.
 
Mathematically,
 
we
 
can
 
write
 
it
 
as
8.
 
Collision and
 
its
 
types When
 
two
 
things
 
bump
 
or
 
strike
 
against
 
each
 
other,
 
it
 
is
 
referred
 
to
 
as
 
a
 
collision.
 
There
 
are
 
two
 
types
 
of
 
collision,
Elastic collision:
 
A collision
 
in
 
which
 
there
 
is
 
no
 
kinetic
 
energy loss
 
at
 
all.
Inelastic collision:
 
A collision
 
that
 
results
 
in
 
some
 
loss
 
of
 
kinetic
 
energy.
The
 
basic characteristics
 
of
 
elastic
 
collision
 
are:
Linear
 
momentum is
 
conserved
Total
 
energy of
 
the
 
system is
 
conserved.
The
 
kinetic
 
energy is
 
conserved.
The
 
basic characteristics
 
of
 
inelastic
 
collision
 
are:
Linear
 
momentum is
 
conserved.
Total
 
energy is
 
conserved.
 
           
Name of the Concept Key Points of the Concepts
Page 3


1.
 
Work
 
done
 
by
 
variable
 
force
Suppose
 
we
 
have
 
to
 
calculate
 
work
 
done
 
in
 
moving
 
a
 
body from a
 
point
 
A( )
 
to
 
a
 
point
 
B( )
 
under
 
the
 
action
 
of
 
a
 
variable
 
force. 
So
 
the
 
work
 
done
 
by this
 
variable
 
force
 
in
 
displacing
 
a
 
body from point
  
to
  
is,
2.
 
Conservative
 
and
 
non-
conservative
 
forces
A force
 
is
 
said
 
to
 
be
 
conservative
 
if
 
work
 
done
 
by or
 
against
 
the
 
force
 
in
 
moving
 
a
 
body depends
 
only on
 
the
 
initial
 
and
 
final
 
position
 
of
 
the
 
body,
 
and
 
not
 
on
 
the
 
natural
 
path
 
followed
 
between
 
the
 
initial
 
and
 
final
 
positions.
If
 
the
 
work
 
done
 
by or
 
against
 
a
 
force
 
in
 
moving
 
a
 
body from one
 
position
 
to
 
another
 
relies
 
on
 
the
 
path
 
taken
 
between
 
these
 
two
 
places,
 
the
 
force
 
is
 
said
 
to
 
be
 
non-conservative.
3.
 
Power
 
definition and
 
relation between work
 
and
 
power
Power
 
is
 
defined
 
as
 
the
 
rate
 
at
 
which
 
work
 
is
 
completed
 
in
 
a
 
given
 
amount
 
of
 
time.
The
 
relation
 
between
 
work
 
( )
 
and
 
power
 
( )
 
is
 
expressed
 
as 
4.
 
Kinetic energy
 
and
 
linear
 
momentum
 
relation
The
 
energy of
 
a
 
body is
 
defined
 
as
 
the
 
capability or
 
ability of
 
the
 
body
 
to
 
do
 
the
 
work.
The
 
relation
 
between
 
kinetic
 
energy
 
(
)
 
and
 
linear
 
momentum( )
 
shows
 
that
 
a
 
body cannot
 
have
 
kinetic
 
energy
 
without
 
having
 
linear
 
momentum and
 
vice-versa.
 
           
Name of the Concept Key Points of the Concepts
Work,	Energy	and	Power
5.
 
Work
 
energy
 
theorem
This
 
theorem states
 
that
 
if
 
some
 
work
 
( )
 
is
 
done
 
by the
 
body then
 
the
 
kinetic
 
energy( )
 
of
 
the
 
body also
 
increases
 
by the
 
same
 
amount.
Work
 
done
 
=
 
increase
 
in
 
K.E.
 
of
 
the
 
body
6.
 
Potential
 
energy
 
of
 
a
 
spring
The
 
potential
 
energy ( )
 
of
 
the
 
spring
 
is
 
the
 
energy associated
 
with
 
the
 
state
 
of
 
compression
 
or
 
expansion
 
of
 
an
 
elastic
 
spring.
 
It
 
is
 
given
 
as
Here,
  
=
 
spring
 
constant
 
and
  
=
 
stretch
 
or
 
compression
 
in
 
the
 
string
7.
 
Mechanical
 
energy
 
and
 
its
 
conservation
The
 
total
 
mechanical
 
energy of
 
the
 
system
 
is
 
conserved
 
if
 
the
 
forces
 
doing
 
work
 
on
 
the
 
system are
 
conservative
 
i.e,
 
when
 
net
 
work
 
done
 
by external
 
non-conservative
 
force
 
is
 
zero.
The
 
mechanical
 
energy ( )
 
of
 
a
 
body is
 
the
 
sum of
 
kinetic
 
energy ( )
 
and
 
potential
 
energy ( )
 
of
 
the
 
body.
 
Mathematically,
 
we
 
can
 
write
 
it
 
as
8.
 
Collision and
 
its
 
types When
 
two
 
things
 
bump
 
or
 
strike
 
against
 
each
 
other,
 
it
 
is
 
referred
 
to
 
as
 
a
 
collision.
 
There
 
are
 
two
 
types
 
of
 
collision,
Elastic collision:
 
A collision
 
in
 
which
 
there
 
is
 
no
 
kinetic
 
energy loss
 
at
 
all.
Inelastic collision:
 
A collision
 
that
 
results
 
in
 
some
 
loss
 
of
 
kinetic
 
energy.
The
 
basic characteristics
 
of
 
elastic
 
collision
 
are:
Linear
 
momentum is
 
conserved
Total
 
energy of
 
the
 
system is
 
conserved.
The
 
kinetic
 
energy is
 
conserved.
The
 
basic characteristics
 
of
 
inelastic
 
collision
 
are:
Linear
 
momentum is
 
conserved.
Total
 
energy is
 
conserved.
 
           
Name of the Concept Key Points of the Concepts
   
List
 
of
 
Important
 
Formulas
 
for
 
Work
 
Energy
 
and
 
Power
 
Chapter
S.No. Name
 
of
 
the
 
Concept Formula
1.
 
Work
 
done
 
by variable
 
force
The
 
work
 
done
 
formula
 
by variable
 
force
 
is
The
 
work
 
done
 
formula
 
for
 
non-
variable
 
force
 
is
2.
 
Kinetic
 
energy and
 
linear
 
momentum relation.
The
 
kinetic
 
energy
 
formula
 
( )
 
is
The
 
expression
 
of
 
linear
 
momentum ( )
 
is
The
 
relationship
 
between
 
kinetic
 
energy and
 
linear
 
momentum is
 
as
 
follows:
3.
  
Work
 
energy theorem
According
 
to
 
this
 
theorem,
 
=
 
increase
 
in
  
of
 
the
 
body
Here,
  
and
  
are
 
the
 
final
 
and
 
initial
 
kinetic
 
energy of
 
the
 
body.
4.
 
Potential
 
energy of
 
a
 
spring
The
 
potential
 
energy
 
formula
 
of
 
a
 
spring
 
is
The
 
maximum velocity ( )
 
of
 
a
 
block
 
of
 
mass
  
upon
 
maximum
 
displacement
 
( )
 
is
5.
 
Mechanical
 
energy and
 
its
 
conservation.
According
 
to
 
conservation
 
of
 
mechanical
 
energy,
 
           
Page 4


1.
 
Work
 
done
 
by
 
variable
 
force
Suppose
 
we
 
have
 
to
 
calculate
 
work
 
done
 
in
 
moving
 
a
 
body from a
 
point
 
A( )
 
to
 
a
 
point
 
B( )
 
under
 
the
 
action
 
of
 
a
 
variable
 
force. 
So
 
the
 
work
 
done
 
by this
 
variable
 
force
 
in
 
displacing
 
a
 
body from point
  
to
  
is,
2.
 
Conservative
 
and
 
non-
conservative
 
forces
A force
 
is
 
said
 
to
 
be
 
conservative
 
if
 
work
 
done
 
by or
 
against
 
the
 
force
 
in
 
moving
 
a
 
body depends
 
only on
 
the
 
initial
 
and
 
final
 
position
 
of
 
the
 
body,
 
and
 
not
 
on
 
the
 
natural
 
path
 
followed
 
between
 
the
 
initial
 
and
 
final
 
positions.
If
 
the
 
work
 
done
 
by or
 
against
 
a
 
force
 
in
 
moving
 
a
 
body from one
 
position
 
to
 
another
 
relies
 
on
 
the
 
path
 
taken
 
between
 
these
 
two
 
places,
 
the
 
force
 
is
 
said
 
to
 
be
 
non-conservative.
3.
 
Power
 
definition and
 
relation between work
 
and
 
power
Power
 
is
 
defined
 
as
 
the
 
rate
 
at
 
which
 
work
 
is
 
completed
 
in
 
a
 
given
 
amount
 
of
 
time.
The
 
relation
 
between
 
work
 
( )
 
and
 
power
 
( )
 
is
 
expressed
 
as 
4.
 
Kinetic energy
 
and
 
linear
 
momentum
 
relation
The
 
energy of
 
a
 
body is
 
defined
 
as
 
the
 
capability or
 
ability of
 
the
 
body
 
to
 
do
 
the
 
work.
The
 
relation
 
between
 
kinetic
 
energy
 
(
)
 
and
 
linear
 
momentum( )
 
shows
 
that
 
a
 
body cannot
 
have
 
kinetic
 
energy
 
without
 
having
 
linear
 
momentum and
 
vice-versa.
 
           
Name of the Concept Key Points of the Concepts
Work,	Energy	and	Power
5.
 
Work
 
energy
 
theorem
This
 
theorem states
 
that
 
if
 
some
 
work
 
( )
 
is
 
done
 
by the
 
body then
 
the
 
kinetic
 
energy( )
 
of
 
the
 
body also
 
increases
 
by the
 
same
 
amount.
Work
 
done
 
=
 
increase
 
in
 
K.E.
 
of
 
the
 
body
6.
 
Potential
 
energy
 
of
 
a
 
spring
The
 
potential
 
energy ( )
 
of
 
the
 
spring
 
is
 
the
 
energy associated
 
with
 
the
 
state
 
of
 
compression
 
or
 
expansion
 
of
 
an
 
elastic
 
spring.
 
It
 
is
 
given
 
as
Here,
  
=
 
spring
 
constant
 
and
  
=
 
stretch
 
or
 
compression
 
in
 
the
 
string
7.
 
Mechanical
 
energy
 
and
 
its
 
conservation
The
 
total
 
mechanical
 
energy of
 
the
 
system
 
is
 
conserved
 
if
 
the
 
forces
 
doing
 
work
 
on
 
the
 
system are
 
conservative
 
i.e,
 
when
 
net
 
work
 
done
 
by external
 
non-conservative
 
force
 
is
 
zero.
The
 
mechanical
 
energy ( )
 
of
 
a
 
body is
 
the
 
sum of
 
kinetic
 
energy ( )
 
and
 
potential
 
energy ( )
 
of
 
the
 
body.
 
Mathematically,
 
we
 
can
 
write
 
it
 
as
8.
 
Collision and
 
its
 
types When
 
two
 
things
 
bump
 
or
 
strike
 
against
 
each
 
other,
 
it
 
is
 
referred
 
to
 
as
 
a
 
collision.
 
There
 
are
 
two
 
types
 
of
 
collision,
Elastic collision:
 
A collision
 
in
 
which
 
there
 
is
 
no
 
kinetic
 
energy loss
 
at
 
all.
Inelastic collision:
 
A collision
 
that
 
results
 
in
 
some
 
loss
 
of
 
kinetic
 
energy.
The
 
basic characteristics
 
of
 
elastic
 
collision
 
are:
Linear
 
momentum is
 
conserved
Total
 
energy of
 
the
 
system is
 
conserved.
The
 
kinetic
 
energy is
 
conserved.
The
 
basic characteristics
 
of
 
inelastic
 
collision
 
are:
Linear
 
momentum is
 
conserved.
Total
 
energy is
 
conserved.
 
           
Name of the Concept Key Points of the Concepts
   
List
 
of
 
Important
 
Formulas
 
for
 
Work
 
Energy
 
and
 
Power
 
Chapter
S.No. Name
 
of
 
the
 
Concept Formula
1.
 
Work
 
done
 
by variable
 
force
The
 
work
 
done
 
formula
 
by variable
 
force
 
is
The
 
work
 
done
 
formula
 
for
 
non-
variable
 
force
 
is
2.
 
Kinetic
 
energy and
 
linear
 
momentum relation.
The
 
kinetic
 
energy
 
formula
 
( )
 
is
The
 
expression
 
of
 
linear
 
momentum ( )
 
is
The
 
relationship
 
between
 
kinetic
 
energy and
 
linear
 
momentum is
 
as
 
follows:
3.
  
Work
 
energy theorem
According
 
to
 
this
 
theorem,
 
=
 
increase
 
in
  
of
 
the
 
body
Here,
  
and
  
are
 
the
 
final
 
and
 
initial
 
kinetic
 
energy of
 
the
 
body.
4.
 
Potential
 
energy of
 
a
 
spring
The
 
potential
 
energy
 
formula
 
of
 
a
 
spring
 
is
The
 
maximum velocity ( )
 
of
 
a
 
block
 
of
 
mass
  
upon
 
maximum
 
displacement
 
( )
 
is
5.
 
Mechanical
 
energy and
 
its
 
conservation.
According
 
to
 
conservation
 
of
 
mechanical
 
energy,
 
           
6. Collision and its types
The expression of coefficient of 
restitution ( ) is
Here,  and  are the initial and 
final velocities of the object.
The expressions of final velocities, 
after elastic collision of two object, 
are
The expression of common velocity 
( ) when two object collide 
inelastically is
       
             
     
                
                
   
                 
                 
                
                 
                
                
    
               
   
       
                 
                       
         
                 
               
               
                   
                     
                 
 
           
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