Title | Week5exercises - from text |
---|---|
Author | Heather Terrill |
Course | Differential Equations |
Institution | Southern New Hampshire University |
Pages | 5 |
File Size | 118.7 KB |
File Type | |
Total Downloads | 73 |
Total Views | 118 |
Final exam, with the work shown. Given at the end of the course...
Charles Terrill Southern New Hampshire University Module 5 Problem Set – 3.4 (2,16); Section 3.5 (2) 3.4 2. The force due to gravity is: F1=400 lb The force due to air resistance is: F2 =−10 v
The net force acting on the object is: F =F1 + F 2=400−10 v The force does not depend on x, enabling us to regard the above equation as an FOE.
m
dv =F (t , v ) dt
Then,
F1=mg→ m=
F 1 400 = =12.5 slug g 32
Now we apply newton’s second law:
m
dv =400−100 v dt
Integrate:
12.5
dv =400−10 v dt
dv =32−0.8 v dt
1 dv=−dt 0.8 v−32
1
∫ .8 v−32 dv=−∫ dt 5 ln |.8 v− 32|=−t +C1 4 ln|.8 v −32|=−.8 t +C2 −0.8t
0.8 v −32=e
+ C2
−.8 t
0.8 v −32=C 3 e
t 0.8 v =32+ C−.8 3e
−.8t
v (t ) =40+ C e
Using substitution value condition, we find the value of C: 0
0=40+C e
−40 =C
0=40+C
Therefore: v (t ) =40 −40 e−.8 t Integrate: x (t ) =∫ v ( t ) dt=∫ ( 40−20 e
−.8t
) dt
x (t ) =40 t+50 e−.8 t + C Substitute the initial value condition x(0) = 0 and obtain the value of C: 0=40 ( 0) + 50 e 0 + C
0=50+C
−50=C
−.8 t
x (t )=40 t+50 e
−50
According to the problem the object hits the ground at 500:
500=40 t−50 ( 1−e−.8t )
500=40 t−50
500 + 50=40 t
−.8t
500=40 t+50 e
t=
−50
500+ 50 40
t ≈ 13.75 sec
16. Notation: T – Motor Torque ω – angular velocity I – inertia ω1 =initial angular velocity
When friction is the reason torque is slowing or ceasing and is proportional to the angular velocity we use: T 1 =K √ω K is proportionally constant. Use the Torque formula: Moment of inertia x angular acceleration = sum of the torques we get:
I
dw =T −K √ ω dt
We use separation of variables in order to solve the differential equation:
Id ω =dt T −K √ ω
√ ω−
⇒−
2 I √ ω − 2TIln|T −K √ ω | =t+C1 K K2
TIln |T −K √ ω| =t +C1 K 2I ⇒ ¿ K
⇒K √ ω−Tln|T −K √ ω|=
⇒√ ω−
2
K t +C 2I
TIln|T −K √ ω| Kt = +C 2 K 2I
C=K √ ω0−Tln∨T − K √ω0 ∨¿
K √ω−Tln|T −K √ ω|=K √ ω 0−Tln|T −K √ ω0|−
K2t 2I
Section 3.5 (2) 2. I used equation 3 on page 119 which is a general equation. e 100t
sin 100 t dt + K 0.000001 ∫¿ −100 t ¿ I (t )=e
100 t 100 sin 100 t−100 cos ¿ ¿ t e 100 ¿ 100 ¿ −100t ¿e ¿
¿
sin 100 t−cos 100 t +K e−100 t 2
For I(0)= 0, we obtain -1.2+K=0 so K=1/2 and the current is : sin 100 t−cos 100 t+e−100 t I ( 0 )=.5 ¿
The resistor and inductor voltages are given by E R ( t) =RI ( t ) =I ( t )
E L ( t) =L
dI =( 0.5)( cos 100t +sin 100 t−e−100t ) dt
Applying Kirchoff’s Voltage law yields: RI +q∨C=e (t) The capacitor is the rate of change of its charge: I= dq/dt I followed the steps in the second example but when I look up the answer to number one in the book, I see mine isn’t looking similar. Not sure what I am doing in the first place just trying to figure it out step by step....