Solving Cauchy's problem with a discontinuous function
I have the Cauchy problem: $$begin{cases} f'=g(t)+2(f-5) \ f(0)=2end{cases}$$
Now $g(t)$ is a periodic function: $$g(t)=begin{cases} 0,tin(24k,24k+8)\
2,tnotin(24k,24k+8) end{cases}$$
for $k=1,2,3...$
How can I solve this Cauchy Problem? Since $g$ is not continuous I don't know what to do.
I am using sagemath to solve it.
differential-equations initial-value-problems sagemath cauchy-problem
add a comment |
I have the Cauchy problem: $$begin{cases} f'=g(t)+2(f-5) \ f(0)=2end{cases}$$
Now $g(t)$ is a periodic function: $$g(t)=begin{cases} 0,tin(24k,24k+8)\
2,tnotin(24k,24k+8) end{cases}$$
for $k=1,2,3...$
How can I solve this Cauchy Problem? Since $g$ is not continuous I don't know what to do.
I am using sagemath to solve it.
differential-equations initial-value-problems sagemath cauchy-problem
1
Use Laplace transform.
– Jacky Chong
Nov 24 at 0:47
add a comment |
I have the Cauchy problem: $$begin{cases} f'=g(t)+2(f-5) \ f(0)=2end{cases}$$
Now $g(t)$ is a periodic function: $$g(t)=begin{cases} 0,tin(24k,24k+8)\
2,tnotin(24k,24k+8) end{cases}$$
for $k=1,2,3...$
How can I solve this Cauchy Problem? Since $g$ is not continuous I don't know what to do.
I am using sagemath to solve it.
differential-equations initial-value-problems sagemath cauchy-problem
I have the Cauchy problem: $$begin{cases} f'=g(t)+2(f-5) \ f(0)=2end{cases}$$
Now $g(t)$ is a periodic function: $$g(t)=begin{cases} 0,tin(24k,24k+8)\
2,tnotin(24k,24k+8) end{cases}$$
for $k=1,2,3...$
How can I solve this Cauchy Problem? Since $g$ is not continuous I don't know what to do.
I am using sagemath to solve it.
differential-equations initial-value-problems sagemath cauchy-problem
differential-equations initial-value-problems sagemath cauchy-problem
asked Nov 24 at 0:44
John Keeper
540313
540313
1
Use Laplace transform.
– Jacky Chong
Nov 24 at 0:47
add a comment |
1
Use Laplace transform.
– Jacky Chong
Nov 24 at 0:47
1
1
Use Laplace transform.
– Jacky Chong
Nov 24 at 0:47
Use Laplace transform.
– Jacky Chong
Nov 24 at 0:47
add a comment |
1 Answer
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Rewrite as
$$ f' - 2f = g - 10 $$
A Fourier method is appropriate here. Since $g$ has a period of $24$, we can assume a series solution of similar periodicity
$$ f(t) = f_0 + sum_{n=1}^infty left[f_ncosleft(frac{npi}{12}tright) + f_n^*sinleft(frac{npi}{12}tright) right]$$
Next, decompose $g$ to its Fourier series
$$ g(t) = g_0 + sum_{n=1}^infty left[g_ncosleft(frac{npi}{12}tright) + g_n^*sinleft(frac{npi}{12}tright) right] $$
From the usual definitions:
$$ g_0 = frac{1}{24}int_0^{24} g(t) dt = int_8^{24} 2 dt = frac{4}{3} $$
$$ g_n = frac{1}{12}int_ 8^{24} 2cosleft(frac{npi}{12}tright) dt = -frac{2}{npi}sin frac{2npi}{3} $$
$$ g_n^* = frac{1}{12}int_8^{24} 2sinleft(frac{npi}{12}tright)dt = -frac{2}{npi}left[1-cos frac{2npi}{3} right] $$
Plug in the 2 series and compare coefficients, we get:
$$ -2f_0 = g_0 - 10 $$
$$ -2f_n + frac{npi}{12}f_n^* = g_n $$
$$ -2f_n^* - frac{npi}{12}f_n = g_n^* $$
Solve the above system of the equations to find $f_n$ and $f_n^*$
add a comment |
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1 Answer
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1 Answer
1
active
oldest
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active
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active
oldest
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Rewrite as
$$ f' - 2f = g - 10 $$
A Fourier method is appropriate here. Since $g$ has a period of $24$, we can assume a series solution of similar periodicity
$$ f(t) = f_0 + sum_{n=1}^infty left[f_ncosleft(frac{npi}{12}tright) + f_n^*sinleft(frac{npi}{12}tright) right]$$
Next, decompose $g$ to its Fourier series
$$ g(t) = g_0 + sum_{n=1}^infty left[g_ncosleft(frac{npi}{12}tright) + g_n^*sinleft(frac{npi}{12}tright) right] $$
From the usual definitions:
$$ g_0 = frac{1}{24}int_0^{24} g(t) dt = int_8^{24} 2 dt = frac{4}{3} $$
$$ g_n = frac{1}{12}int_ 8^{24} 2cosleft(frac{npi}{12}tright) dt = -frac{2}{npi}sin frac{2npi}{3} $$
$$ g_n^* = frac{1}{12}int_8^{24} 2sinleft(frac{npi}{12}tright)dt = -frac{2}{npi}left[1-cos frac{2npi}{3} right] $$
Plug in the 2 series and compare coefficients, we get:
$$ -2f_0 = g_0 - 10 $$
$$ -2f_n + frac{npi}{12}f_n^* = g_n $$
$$ -2f_n^* - frac{npi}{12}f_n = g_n^* $$
Solve the above system of the equations to find $f_n$ and $f_n^*$
add a comment |
Rewrite as
$$ f' - 2f = g - 10 $$
A Fourier method is appropriate here. Since $g$ has a period of $24$, we can assume a series solution of similar periodicity
$$ f(t) = f_0 + sum_{n=1}^infty left[f_ncosleft(frac{npi}{12}tright) + f_n^*sinleft(frac{npi}{12}tright) right]$$
Next, decompose $g$ to its Fourier series
$$ g(t) = g_0 + sum_{n=1}^infty left[g_ncosleft(frac{npi}{12}tright) + g_n^*sinleft(frac{npi}{12}tright) right] $$
From the usual definitions:
$$ g_0 = frac{1}{24}int_0^{24} g(t) dt = int_8^{24} 2 dt = frac{4}{3} $$
$$ g_n = frac{1}{12}int_ 8^{24} 2cosleft(frac{npi}{12}tright) dt = -frac{2}{npi}sin frac{2npi}{3} $$
$$ g_n^* = frac{1}{12}int_8^{24} 2sinleft(frac{npi}{12}tright)dt = -frac{2}{npi}left[1-cos frac{2npi}{3} right] $$
Plug in the 2 series and compare coefficients, we get:
$$ -2f_0 = g_0 - 10 $$
$$ -2f_n + frac{npi}{12}f_n^* = g_n $$
$$ -2f_n^* - frac{npi}{12}f_n = g_n^* $$
Solve the above system of the equations to find $f_n$ and $f_n^*$
add a comment |
Rewrite as
$$ f' - 2f = g - 10 $$
A Fourier method is appropriate here. Since $g$ has a period of $24$, we can assume a series solution of similar periodicity
$$ f(t) = f_0 + sum_{n=1}^infty left[f_ncosleft(frac{npi}{12}tright) + f_n^*sinleft(frac{npi}{12}tright) right]$$
Next, decompose $g$ to its Fourier series
$$ g(t) = g_0 + sum_{n=1}^infty left[g_ncosleft(frac{npi}{12}tright) + g_n^*sinleft(frac{npi}{12}tright) right] $$
From the usual definitions:
$$ g_0 = frac{1}{24}int_0^{24} g(t) dt = int_8^{24} 2 dt = frac{4}{3} $$
$$ g_n = frac{1}{12}int_ 8^{24} 2cosleft(frac{npi}{12}tright) dt = -frac{2}{npi}sin frac{2npi}{3} $$
$$ g_n^* = frac{1}{12}int_8^{24} 2sinleft(frac{npi}{12}tright)dt = -frac{2}{npi}left[1-cos frac{2npi}{3} right] $$
Plug in the 2 series and compare coefficients, we get:
$$ -2f_0 = g_0 - 10 $$
$$ -2f_n + frac{npi}{12}f_n^* = g_n $$
$$ -2f_n^* - frac{npi}{12}f_n = g_n^* $$
Solve the above system of the equations to find $f_n$ and $f_n^*$
Rewrite as
$$ f' - 2f = g - 10 $$
A Fourier method is appropriate here. Since $g$ has a period of $24$, we can assume a series solution of similar periodicity
$$ f(t) = f_0 + sum_{n=1}^infty left[f_ncosleft(frac{npi}{12}tright) + f_n^*sinleft(frac{npi}{12}tright) right]$$
Next, decompose $g$ to its Fourier series
$$ g(t) = g_0 + sum_{n=1}^infty left[g_ncosleft(frac{npi}{12}tright) + g_n^*sinleft(frac{npi}{12}tright) right] $$
From the usual definitions:
$$ g_0 = frac{1}{24}int_0^{24} g(t) dt = int_8^{24} 2 dt = frac{4}{3} $$
$$ g_n = frac{1}{12}int_ 8^{24} 2cosleft(frac{npi}{12}tright) dt = -frac{2}{npi}sin frac{2npi}{3} $$
$$ g_n^* = frac{1}{12}int_8^{24} 2sinleft(frac{npi}{12}tright)dt = -frac{2}{npi}left[1-cos frac{2npi}{3} right] $$
Plug in the 2 series and compare coefficients, we get:
$$ -2f_0 = g_0 - 10 $$
$$ -2f_n + frac{npi}{12}f_n^* = g_n $$
$$ -2f_n^* - frac{npi}{12}f_n = g_n^* $$
Solve the above system of the equations to find $f_n$ and $f_n^*$
edited Nov 25 at 12:12
answered Nov 25 at 10:23
Dylan
12.1k31026
12.1k31026
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Use Laplace transform.
– Jacky Chong
Nov 24 at 0:47