Quantum information is highly constrained compared to classical information, yet has extra degrees of freedom that in a sense are "worth more" than classical bits. But this is not merely that N qubits can store M bits:
It is sometimes useful to distinguish between the different quantum information resources in terms of (classical) bits, qubits and ebits (entanglement bits). A maximally entangled two qubit state (a Bell state) has 1 ebit: tasks requiring X ebits can be done with X or more Bell states but not fewer.
This extra value can be expressed through "Bennett's laws":
1 qubit $\succeq$ 1 bit (qubits can transmit bits)
1 qubit $\succeq$ 1 ebit (qubits can generate entanglement)
1 qubit + 1 ebit $\succeq$ 2 bits (superdense coding)
1 ebit + 2 bits $\succeq$ 1 qubit (quantum teleportation)
where $\succeq$ means "can do the job of". The no-signalling theorem rules out using one ebit to do the job of one bit, and the no-teleportation theorem rules out using any number of bits to do the job of one qubit.
The Holevo bound implies that amount of classical information that can be retrieved from $n$ qubits is just $n$ classical bits, despite the much larger amount of information in the qubits.
$n$ qubits in a computation allow computing up to $2^n$ function evaluations in parallel... but only $n$ bits, randomly sampled from a probability distribution due to the quantum computation done, can be retrieved at the end.
So 60 qubits are at most worth $2^{60}$ operations but will only give you 60 bits of information at the end. They can also perform nonclassical tricks according to Bennett's laws.
As for speed, see the quantum speed limits. Basically, the fastest you can move between distinguishable quantum states is set by the energy you put into the system, not the number of bits.