Week 3 Worksheet - Solutions

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Power Series

    1. Calculate |2n+1n+1/2nn|=2nn+12 as n so the radius of convergence is 12.

    2. Calculate |(n+1)!n!|=n+1 as n so the radius of convergence is 0.

    3. Calculate |(n+1)pnp|=(n+1n)p1 as n so the radius of convergence is 1.

  1. Calculate |(1)n+1((n+1)!)22(n+1)/(1)n(n!)22n|=nn+11(n+1)20 as n so R=.

  2. If RS the radius of convergence will be min{R,S}. Indeed, if |z|<min{R,S} then both power series converge, so their sum does as well, but if min{R,S}<|z|<max{S,R} the sum cannot converge as then both series would.

    If R=S then the sum can have any radius of convergence TR. Indeed, suppose bn=an and fix a power series n=0cnzn with radius of convergence TR. Then n=0(an+cn)znn=0(bn+cn) both have radius of convergence R by the previous paragraph, but their sum has radius of convergence T.

Differentiation of Power Series

  1. We multiple the right-hand side by AB to get A(An1+An2B1++A1Bn2+Bn1)B(An1+An2B1++A1Bn2+Bn1)=(An+An1B1++A2Bn2+A1Bn1)(An1B1+An2B2++A1Bn1+Bn)=AnBn as desired.

    1. We can differentiate the power series for 1/(1z) inside B(0,1) term-by-term. This gives 1(1z)2=1+2z+3z2+4z3+

    2. Replacing z with z2 in the geometric series gives 11z2=1+z2+z4+z6+ on B(0,1) because |z|2=|z||z|<1 whenever |z|<1.

    3. Differentiating our answer to (b) on B(0,1) gives 2z(1z2)2=2z+4z3+6z5+ for all |z|<1. \qedhere

The Exponential Function and Trigonometric Functions

  1. Fix w=u+iv0. We need to produce z with exp(z)=w. From exp(x+iy)=ex(cos(y)+isin(y)) we should take x=ln(|w|) and y=Arg(w).

    1. Fix zC. We calculate exp(z+2πin)=exp(x+i(y+2πn))=ex(cos(y+2πn)+isin(y+2πn))=ex(cos(y)+isin(y))=exp(z) because sin and cos have 2πn as a period for any nZ.

    2. Suppose τ is a period of exp. Then exp(z+τ)=exp(z) for all zC. In particular exp(z)=exp(z+τ)=exp(z)exp(τ) so exp(τ)=1. Write τ=a+ib. Then 1=ea(cos(b)+isin(b)) which forces |1|=ea, cos(b)=1 and sin(b)=0. We must have a=0 and b=2πn so exp has no other periods.

  2. Write exp(x+iy)=ex(cos(y)+isin(y))=excos(y)+iexsin(y) so u(x,y)=excos(y) and v(x,y)=exsin(y). Then (1u)(x,y)=excos(y)(2u)(x,y)=exsin(y)(1v)(x,y)=exsin(y)(2v)(x,y)=excos(y) and the Cauchy-Riemann equations are seen to be true for all (x,y).

  3. If exp(x+iy) is real then exsin(y)=0 which is the same as y=πn for some nZ. If it is imaginary then excos(y)=0 which is the same as y=πn+π2.

  4. If exp(z)=1 then excos(y)=1 and exsin(y)=0 so x=0 and y=2πn+π for some nZ.

    If exp(z)=1+i then excos(y)=1 and exsin(y)=1. We have ex=|1+i|=2 so x=12ln(2). From sin(y)=12=cos(y) we get y=2πn+π4.

  5. cos(i)=exp(i2)+exp(i2)2=1e+e2=1+e22e sin(i)=exp(i2)exp(i22i=1ee2i=1e22ei

  6. No because the odd (respectively even) coefficients are zero: the quotient an+1/an is not defined for all nN.

  7. Calculate cos(z)cos(w)sin(z)sin(w)=exp(iz)+exp(iz)2exp(iw)+exp(iw)2exp(iz)exp(iz)2iexp(iw)exp(iw)2i=exp(i(z+w))+exp(i(zw))+exp(i(z+w))+exp(i(zw))4+exp(i(z+w))exp(i(zw))exp(i(z+w))+exp(i(zw))4=exp(i(z+w))+exp(i(z+w))2=cos(z+w) and sin(z)cos(w)+sin(w)cos(z)=exp(iz)exp(iz)2iexp(iw)+exp(iw)2+exp(iw)exp(iw)2iexp(iz)+exp(iz)2=exp(i(z+w))+exp(i(zw))exp(i(z+w))exp(i(zw))4i+exp(i(w+z))+exp(i(wz))exp(i(w+z))exp(i(wz))4i=exp(i(w+z))exp(i(wz))2i=sin(w+z)

  8. Calculate cosh(z)+sinh(z)=exp(z)+exp(z)2+exp(z)exp(z)2=exp(z)

  9. Calculate (cosh(z))2(sinh(z)2=(exp(z)+exp(z)2)2(exp(z)exp(z)2)2=exp(2z)+2+exp(2z)4exp(2z)2+exp(2z)4=1