Question #62809

dB/dx=B/t2
t is constant.if we solve this we get
B=B0 ex/t+B0e-x/t
if the graph is DECAYING EXPONENTIALY then can we ignore the B0 ex/t term?

Expert's answer

Answer on Question #62809 – Math – Differential Equations

Question

dB/dx=B/t2\mathrm{dB/dx = B/t2}

t is constant. if we solve this we get B=B0ex/t+B0ex/t\mathrm{B} = \mathrm{B}0\mathrm{ex/t} + \mathrm{B}0\mathrm{e - x/t} if the graph is DECAYING EXPONENTIALLY then can we ignore the B0 ex/t term?

Solution

B=B0ex/t+B0ex/tB = B_{0}e^{x / t} + B_{0}e^{-x / t} is not a solution of equation


dBdx=Bt2\frac {d B}{d x} = \frac {B}{t ^ {2}}


Because


ddx(B0ext+B0ext)=B0(1text1text)=B01t(extext)Bt2=(B0ex/t+B0ex/t)t2\frac {d}{d x} \Big (B _ {0} e ^ {\frac {x}{t}} + B _ {0} e ^ {- \frac {x}{t}} \Big) = B _ {0} \left(\frac {1}{t} e ^ {\frac {x}{t}} - \frac {1}{t} e ^ {- \frac {x}{t}}\right) = B _ {0} \frac {1}{t} \Big (e ^ {\frac {x}{t}} - e ^ {- \frac {x}{t}} \Big) \neq \frac {B}{t ^ {2}} = \frac {(B _ {0} e ^ {x / t} + B _ {0} e ^ {- x / t})}{t ^ {2}}


But, B=B0ex/t+B0ex/tB = B_0e^{x / t} + B_0e^{-x / t} is the solution of the equation


d2Bdx2=Bt2\frac {d ^ {2} B}{d x ^ {2}} = \frac {B}{t ^ {2}}


Because


d2Bdx2=ddx(B01t(extext))=B01tddx(extext)=B01t(1text+1text)=\frac {d ^ {2} B}{d x ^ {2}} = \frac {d}{d x} \left(B _ {0} \frac {1}{t} \left(e ^ {\frac {x}{t}} - e ^ {- \frac {x}{t}}\right)\right) = B _ {0} \frac {1}{t} \frac {d}{d x} \left(e ^ {\frac {x}{t}} - e ^ {- \frac {x}{t}}\right) = B _ {0} \frac {1}{t} \left(\frac {1}{t} e ^ {\frac {x}{t}} + \frac {1}{t} e ^ {- \frac {x}{t}}\right) ==B01t2(ext+ext)=Bt2= B _ {0} \frac {1}{t ^ {2}} \left(e ^ {\frac {x}{t}} + e ^ {- \frac {x}{t}}\right) = \frac {B}{t ^ {2}}


Let's solve equation


d2Bdx2=Bt2\frac {d ^ {2} B}{d x ^ {2}} = \frac {B}{t ^ {2}}


We will find the solution in the form


B=eλxB = e ^ {\lambda x}


Substituting into the equation yields


d2Bdx2=λ2eλx=1t2eλx\frac {d ^ {2} B}{d x ^ {2}} = \lambda^ {2} e ^ {\lambda x} = \frac {1}{t ^ {2}} e ^ {\lambda x}


From this we obtain the characteristic equation: λ2=1t2\lambda^2 = \frac{1}{t^2}. The solutions of this equation are


λ=±1t.\lambda = \pm \frac {1}{t}.


Thus we have two particular solutions B1=ex/tB_{1} = e^{x / t} and B2=ex/tB_{2} = e^{-x / t}.

The general solution of the original equation is the linear combination of the particular solutions:


B=Cex/t+Dex/tB = C e ^ {x / t} + D e ^ {- x / t}


where CC and DD are some constants which we chose depending on initial or boundaries conditions, if B0B \to 0 when xx \to \infty, we have to take C=0C = 0, so we have B=Dex/tB = D e^{-x / t} or B=B0ex/tB = B_0 e^{-x / t} where B=B0B = B_0 at x=0x = 0

**Answer**: B=B0ex/tB = B_{0}e^{-x / t}.

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