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Further Growth & Decay
Further Growth & Decay
In order to take into account other conditions (e.g. the temperature of
an object will never be lower than the temperature of its
surroundings), we need to change the equation.
Further Growth & Decay
In order to take into account other conditions (e.g. the temperature of
an object will never be lower than the temperature of its
surroundings), we need to change the equation.

                            dP
                                k P  N 
                            dt
Further Growth & Decay
In order to take into account other conditions (e.g. the temperature of
an object will never be lower than the temperature of its
surroundings), we need to change the equation.

                            dP
                                k P  N 
                            dt

                   the solution to the equation is;

                               PN            (trivial case)
Further Growth & Decay
In order to take into account other conditions (e.g. the temperature of
an object will never be lower than the temperature of its
surroundings), we need to change the equation.

                            dP
                                k P  N 
                            dt

                   the solution to the equation is;

                                PN           (trivial case)
                                OR
                            P  N  Ae kt
     P = population at time t        k = growth(or decay) constant

     N + A = initial population      t = time
e.g.(1993)
    Let T be the temperature inside a room at time t and let A be the
    constant outside air temperature.
    Newton’s law of cooling states that the rate of change of the
    temperature is proportional to (T – A).
e.g.(1993)
    Let T be the temperature inside a room at time t and let A be the
    constant outside air temperature.
    Newton’s law of cooling states that the rate of change of the
    temperature is proportional to (T – A).
    a) Show that T  A  Ce kt (where C and k are constants) satisfies
       Newton' s law of cooling.
e.g.(1993)
    Let T be the temperature inside a room at time t and let A be the
    constant outside air temperature.
    Newton’s law of cooling states that the rate of change of the
    temperature is proportional to (T – A).
    a) Show that T  A  Ce kt (where C and k are constants) satisfies
       Newton' s law of cooling.
                       T  A  Ce kt
e.g.(1993)
    Let T be the temperature inside a room at time t and let A be the
    constant outside air temperature.
    Newton’s law of cooling states that the rate of change of the
    temperature is proportional to (T – A).
    a) Show that T  A  Ce kt (where C and k are constants) satisfies
       Newton' s law of cooling.
                      T  A  Ce kt
                     dT
                         kCe kt
                     dt
e.g.(1993)
    Let T be the temperature inside a room at time t and let A be the
    constant outside air temperature.
    Newton’s law of cooling states that the rate of change of the
    temperature is proportional to (T – A).
    a) Show that T  A  Ce kt (where C and k are constants) satisfies
       Newton' s law of cooling.
                      T  A  Ce kt
                     dT
                         kCe kt
                     dt
                          but T  A  Ce kt
e.g.(1993)
    Let T be the temperature inside a room at time t and let A be the
    constant outside air temperature.
    Newton’s law of cooling states that the rate of change of the
    temperature is proportional to (T – A).
    a) Show that T  A  Ce kt (where C and k are constants) satisfies
       Newton' s law of cooling.
                      T  A  Ce kt
                     dT
                         kCe kt
                     dt
                          but T  A  Ce kt
                     dT
                         k T  A 
                     dt
e.g.(1993)
    Let T be the temperature inside a room at time t and let A be the
    constant outside air temperature.
    Newton’s law of cooling states that the rate of change of the
    temperature is proportional to (T – A).
    a) Show that T  A  Ce kt (where C and k are constants) satisfies
       Newton' s law of cooling.
                      T  A  Ce kt
                     dT
                         kCe kt
                     dt
                          but T  A  Ce kt
                   dT
                        k T  A 
                    dt
                                         dT
                T  A  Ce kt satisfies     k T  A
                                         dt
b) The outside air temperature is 5 C and a heating system breakdown
   causes the inside room temperature to drop from 20  C to 17  C in
   half an hour.
  After how many hours is the inside room temperature equal to 10  C ?
b) The outside air temperature is 5 C and a heating system breakdown
   causes the inside room temperature to drop from 20  C to 17  C in
   half an hour.
  After how many hours is the inside room temperature equal to 10  C ?

   T  5  Ce kt
b) The outside air temperature is 5 C and a heating system breakdown
   causes the inside room temperature to drop from 20  C to 17  C in
   half an hour.
  After how many hours is the inside room temperature equal to 10  C ?

   T  5  Ce kt
   when t  0, T  20
       C  15
      T  5  15e kt
b) The outside air temperature is 5 C and a heating system breakdown
   causes the inside room temperature to drop from 20  C to 17  C in
   half an hour.
  After how many hours is the inside room temperature equal to 10  C ?

   T  5  Ce kt                      when t  0.5, T  17
   when t  0, T  20                 i.e. 17  5  15e 0.5 k
       C  15
      T  5  15e kt
b) The outside air temperature is 5 C and a heating system breakdown
   causes the inside room temperature to drop from 20  C to 17  C in
   half an hour.
  After how many hours is the inside room temperature equal to 10  C ?

   T  5  Ce kt                      when t  0.5, T  17
   when t  0, T  20                 i.e. 17  5  15e 0.5 k
       C  15                       15e 0.5 k  12
      T  5  15e kt
b) The outside air temperature is 5 C and a heating system breakdown
   causes the inside room temperature to drop from 20  C to 17  C in
   half an hour.
  After how many hours is the inside room temperature equal to 10  C ?

   T  5  Ce kt                      when t  0.5, T  17
   when t  0, T  20                 i.e. 17  5  15e 0.5 k
       C  15                       15e 0.5 k  12
      T  5  15e kt                                12
                                        e 0.5 k 
                                                    15
                                                   12 
                                       0.5k  log 
                                                   15 
                                                     12 
                                          k  2 log 
                                                     15 
when T  10, 10  5  15e kt
when T  10, 10  5  15e kt
            15e kt  5
                     1
              e 
                kt

                     3
                        1
               kt  log
                        3
                    1     1
                t  log
                    k     3
when T  10, 10  5  15e kt
            15e kt  5
                     1
              e 
                kt

                     3
                        1
               kt  log
                        3
                    1     1
                 t  log
                    k     3
                t  2.46167
when T  10, 10  5  15e kt
              15e kt  5
                       1
                e 
                  kt

                       3
                          1
                 kt  log
                          3
                      1     1
                   t  log
                      k     3
                  t  2.46167
         1
 After 2 hours the temperature has dropped to 10 C
         2
when T  10, 10  5  15e kt
              15e kt  5
                       1
                e 
                  kt

                       3
                          1
                 kt  log
                          3
                      1     1
                   t  log
                      k     3
                  t  2.46167
         1
 After 2 hours the temperature has dropped to 10 C
         2


                   Exercise 7H; 2, 4, 5, 8, 9, 10

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12 X1 T04 05 Further Growth and Decay (2010)

  • 2. Further Growth & Decay In order to take into account other conditions (e.g. the temperature of an object will never be lower than the temperature of its surroundings), we need to change the equation.
  • 3. Further Growth & Decay In order to take into account other conditions (e.g. the temperature of an object will never be lower than the temperature of its surroundings), we need to change the equation. dP  k P  N  dt
  • 4. Further Growth & Decay In order to take into account other conditions (e.g. the temperature of an object will never be lower than the temperature of its surroundings), we need to change the equation. dP  k P  N  dt the solution to the equation is; PN (trivial case)
  • 5. Further Growth & Decay In order to take into account other conditions (e.g. the temperature of an object will never be lower than the temperature of its surroundings), we need to change the equation. dP  k P  N  dt the solution to the equation is; PN (trivial case) OR P  N  Ae kt P = population at time t k = growth(or decay) constant N + A = initial population t = time
  • 6. e.g.(1993) Let T be the temperature inside a room at time t and let A be the constant outside air temperature. Newton’s law of cooling states that the rate of change of the temperature is proportional to (T – A).
  • 7. e.g.(1993) Let T be the temperature inside a room at time t and let A be the constant outside air temperature. Newton’s law of cooling states that the rate of change of the temperature is proportional to (T – A). a) Show that T  A  Ce kt (where C and k are constants) satisfies Newton' s law of cooling.
  • 8. e.g.(1993) Let T be the temperature inside a room at time t and let A be the constant outside air temperature. Newton’s law of cooling states that the rate of change of the temperature is proportional to (T – A). a) Show that T  A  Ce kt (where C and k are constants) satisfies Newton' s law of cooling. T  A  Ce kt
  • 9. e.g.(1993) Let T be the temperature inside a room at time t and let A be the constant outside air temperature. Newton’s law of cooling states that the rate of change of the temperature is proportional to (T – A). a) Show that T  A  Ce kt (where C and k are constants) satisfies Newton' s law of cooling. T  A  Ce kt dT  kCe kt dt
  • 10. e.g.(1993) Let T be the temperature inside a room at time t and let A be the constant outside air temperature. Newton’s law of cooling states that the rate of change of the temperature is proportional to (T – A). a) Show that T  A  Ce kt (where C and k are constants) satisfies Newton' s law of cooling. T  A  Ce kt dT  kCe kt dt but T  A  Ce kt
  • 11. e.g.(1993) Let T be the temperature inside a room at time t and let A be the constant outside air temperature. Newton’s law of cooling states that the rate of change of the temperature is proportional to (T – A). a) Show that T  A  Ce kt (where C and k are constants) satisfies Newton' s law of cooling. T  A  Ce kt dT  kCe kt dt but T  A  Ce kt dT  k T  A  dt
  • 12. e.g.(1993) Let T be the temperature inside a room at time t and let A be the constant outside air temperature. Newton’s law of cooling states that the rate of change of the temperature is proportional to (T – A). a) Show that T  A  Ce kt (where C and k are constants) satisfies Newton' s law of cooling. T  A  Ce kt dT  kCe kt dt but T  A  Ce kt dT  k T  A  dt dT T  A  Ce kt satisfies  k T  A dt
  • 13. b) The outside air temperature is 5 C and a heating system breakdown causes the inside room temperature to drop from 20  C to 17  C in half an hour. After how many hours is the inside room temperature equal to 10  C ?
  • 14. b) The outside air temperature is 5 C and a heating system breakdown causes the inside room temperature to drop from 20  C to 17  C in half an hour. After how many hours is the inside room temperature equal to 10  C ? T  5  Ce kt
  • 15. b) The outside air temperature is 5 C and a heating system breakdown causes the inside room temperature to drop from 20  C to 17  C in half an hour. After how many hours is the inside room temperature equal to 10  C ? T  5  Ce kt when t  0, T  20  C  15 T  5  15e kt
  • 16. b) The outside air temperature is 5 C and a heating system breakdown causes the inside room temperature to drop from 20  C to 17  C in half an hour. After how many hours is the inside room temperature equal to 10  C ? T  5  Ce kt when t  0.5, T  17 when t  0, T  20 i.e. 17  5  15e 0.5 k  C  15 T  5  15e kt
  • 17. b) The outside air temperature is 5 C and a heating system breakdown causes the inside room temperature to drop from 20  C to 17  C in half an hour. After how many hours is the inside room temperature equal to 10  C ? T  5  Ce kt when t  0.5, T  17 when t  0, T  20 i.e. 17  5  15e 0.5 k  C  15 15e 0.5 k  12 T  5  15e kt
  • 18. b) The outside air temperature is 5 C and a heating system breakdown causes the inside room temperature to drop from 20  C to 17  C in half an hour. After how many hours is the inside room temperature equal to 10  C ? T  5  Ce kt when t  0.5, T  17 when t  0, T  20 i.e. 17  5  15e 0.5 k  C  15 15e 0.5 k  12 T  5  15e kt 12 e 0.5 k  15  12  0.5k  log   15   12  k  2 log   15 
  • 19. when T  10, 10  5  15e kt
  • 20. when T  10, 10  5  15e kt 15e kt  5 1 e  kt 3 1 kt  log 3 1 1 t  log k 3
  • 21. when T  10, 10  5  15e kt 15e kt  5 1 e  kt 3 1 kt  log 3 1 1 t  log k 3 t  2.46167
  • 22. when T  10, 10  5  15e kt 15e kt  5 1 e  kt 3 1 kt  log 3 1 1 t  log k 3 t  2.46167 1  After 2 hours the temperature has dropped to 10 C 2
  • 23. when T  10, 10  5  15e kt 15e kt  5 1 e  kt 3 1 kt  log 3 1 1 t  log k 3 t  2.46167 1  After 2 hours the temperature has dropped to 10 C 2 Exercise 7H; 2, 4, 5, 8, 9, 10