One more qubit = ×2 states
Adding 10 qubits multiplies the state space by 1024. Growth is multiplicative, not additive.
See exponential growth in action: n qubits span 2n basis states. Compare that with classical bits and estimate how much RAM a full state vector needs—or how many qubits your RAM can hold.
This is a back-of-the-envelope, state-vector view. Tensor networks, sparsity, or algorithm-specific tricks can simulate some circuits with fewer bytes, but the exponential ceiling still appears for generic states.
Adding 10 qubits multiplies the state space by 1024. Growth is multiplicative, not additive.
50 qubits at 16 bytes per amplitude need ~16 PB. 60 qubits blow past exabyte scale.
You only read one basis string per run. The power comes from interference before measurement.
On a 1–2 TB workstation, full state-vector simulators top out near 45–50 qubits at double precision.
Algorithms with low entanglement (e.g., certain shallow circuits) can be simulated with tensor networks beyond 50 qubits.
Classical bits carry a single 0 or 1. n bits let you pick exactly one of 2n strings at a time. Qubits extend that space: an n-qubit register is a vector in a 2n-dimensional complex space, with an amplitude attached to every basis string. That is why the state-vector memory scales as 2n—you track a complex number for every possible classical configuration.
The RAM estimator translates the abstract 2n into hardware cost. At 30 qubits, storing the full vector is already about 16 GB in double precision. Each new qubit doubles that. By 45 qubits you are near half a petabyte; by 60 qubits the number is so large that traditional clusters struggle unless the circuit has exploitable structure. This is why quantum speedups can appear: the space being explored is too large to enumerate classically.
Keep in mind that practical quantum algorithms rarely need the full state vector printed out. The point is to manipulate amplitudes so that when you finally measure, the desired basis state is likely. These calculations simply show the gap between “I can list all classical states” and “I can hold a coherent superposition of them.”